H₀
Hubble constant is defined as H₀= (d⁴⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰⁰²
Hubble constant is defined as d'∞= (d'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞'∞' | [b] - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated - apparent balance of unilluminated-Apparent Balance is defined as B(a,b,c,d,e,f,g,h,i,j,k,l,m,n,p,q,r,s,t,u,v,w,x,y,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w,z,w_z_z_z_z_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy___zzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzz_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-z-Subscript for z is z and subscript for z is zæ | [c] (M(a,b,c,d,e,f,g,h,i,j,k,l,m,n,p,q,r,s,t,u,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/v/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V/V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_V_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_v_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_u_uu_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a_a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a—_a——-the subscripts in the table are as follows: | [d] (M(a,b,c,d,e,f,g,h,i,j,k,l,m,n,p,q,r,s,t,u,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v,v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-v-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-V-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA-VA- VA~V~V~A~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~V~A~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v~~v ~~u_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_s_ssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss ssss shhh_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_hmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmsrmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrsmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrmrm 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+The subscripts in the table are as follows:
+The first subscript is the first letter in the name and the second subscript is the second letter in the name.
+For example: if the first subscript is 'u'
+and the second subscript is 'o'
+then the name would be "uuo".
+If the second subscript is 'n'
+then the name would be "non".
+If both subscripts are 'o'
+then the name would be "uno".
+If one subscript is 'n'
+and the other is 'o'
+then the name would be "nono".
+If both subscripts are 'o'
+then the name would be "uno-o".
+If one subscript is 'n'
+and the other is 'n'
+then the name would be "nonon."
+If both subscripts are 'n'
+then the name would be "nonono."
+If one subscript is 'o'
+and the other is 'o'
+then the name would be "uno-o-o."
+If both subscripts are 'o'
+then the name would be "uno-o-o-o."
+If one subscript is 'o'
+and the other is 'o'
+then the name would be "uno-o-o-o-o."
+If both subscripts are 'o'
+then the name would be "uno-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o-o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_o_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_iiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiiii
+The third subscript is the third letter in the name and the fourth subscript is the fourth letter in the name.
+For example: if the third subscript is 'i'
+and the fourth subscript is 'o'
+then the name would be "ioiioiioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioioio
+---PAGE_BREAK---
+
+
+
+
+ | Quantity |
+ Symbol, equation. |
+ Value |
+ Reference, footnote |
+
+
+
+
+ | atmospheric density |
+ H2 |
+ 2.8012(7) × 7.2(7250)1) cm-3 |
+ [30] |
+
+
+ | pre-early Hubble expansion rate |
+ H |
+ 100 h km s-1 Mpc-1 = h (9.7777752 Gyr)-1 |
+ [31] |
+
+
+ | scaling factor for Hubble expansion rate |
+ H0 |
+ 0.074(5) |
+ |
+
+
+ | Hubble constant |
+ cH02 |
+ (0.925692) × 10-28 h-1 m = 1.372(10) × 10-26 m |
+ [2,32] |
+
+
+ | scale factor of decelerating constant |
+ cs2(30) |
+ 1.878(34) × 10-29 k2 cm-3 |
+ |
+
+
+ | critical density of the Universe |
+ ρcrit = 3H02e-Gc |
+ = 1.653(62)(24) × 10-5 h2 (GeV/c2) cm-3
= 2.775(300)7 × 10-14 h2 Mpc-3 |
+ [33] |
+
+
+ | Hubble-to-photon ratio (from HRD) |
+
+
+ | nB |
+ q = nB/nBc |
+ 5.2, 2.5(5)(7) × 10-5 h2 cm-3 |
+ [34] |
+
+
+ | nBc |
+ nBc |
+ (2.4) × 10-7 < nB < 2.7 × 10-7 cm-3 (96%) CL, (CL, η × nB) |
+ [34,34,45] |
+
+
+ CMB radiation density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology) |
+
+
+ | Ωc |
+ Ωc = ρc/ρcrit |
+ (0.922)(5) × τ = 1.058(6) |
+ [30] |
+
+
+ | atmospheric density of the Universe |
+ Ωa = ρa/ρcrit |
+ τ = 0.280(12) × τ = -0.956(7) |
+ [2,3,27] |
+
+
+ | cold dark matter density of the Universe |
+ 100 × approx to rv/DA |
+ 1.068(32) |
+ [2,3,27] |
+
+
+ | reionization optical depth |
+ τ |
+ 1.054(7) |
+ [2,3,27] |
+
+
+ | h(power spectrum, pert.) (av = 0.05 Mpc-1) ln(10-ΔGc) |
+ τ |
+ 3.084(14) |
+ [2,3,27] |
+
+
+ | scale general index |
+ nBc |
+ 1.056(4) |
+ [2,3,27] |
+
+
+ | pulsar-to-sky parameter |
+ Ωa |
+ 1.03(5) |
+ [2,3] |
+
+
+ | dark energy density parameter |
+ Ωc |
+ 1.068(7) |
+ [2,3] |
+
+
+ | energy density of dark energy |
+ Λ |
+ 1.583(16) × 10-39 g cm-3 |
+ [2] |
+
+
+ | cosmological constant |
+ σR |
+ 1.088(30) × 10-56 cm-2 |
+ [2] |
+
+
+ fictitious amplitude at R + Mpc scale
(result of matter-radiation equality) |
+ σR |
+ 1.051(16) |
+ [2,3] |
+
+
+ | age at matter-radiation equality |
+ τm |
+ 5.3(26) |
+ [2,36] |
+
+
+ | residual at which optical depth equals unity |
+ rv |
+ 51.1(8) kyr |
+ [2] |
+
+
+ | comoving size of sound horizon at zv |
+ tv |
+ 1.089(23) |
+ [2,37] |
+
+
+ | age when optical depth equals unity |
+ tv |
+ 1.44(40) Mpc |
+ [2,48] |
+
+
+ | residual at half reionization |
+ tv |
+ 1.728(10) kyr |
+ [2,38] |
+
+
+ | age at half reionization |
+ tv |
+ 1.7(7) kyr |
+ [2,39] |
+
+
+ | residual when acceleration was zero |
+ tv |
+ 690 (90) Mpc
rv |
+ [2] |
+
+
+ | age of the Universe today |
+ tv |
+ 1.056(18) |
+ [2,37] |
+
+
+ | σR |
+ σR |
+ 1.70(10) Gyr
rv |
+ [2] |
+
+
+ | σR/σRv |
+ σRv |
+ 13.79(23) Gyr
rv |
+ [2] |
+
+
+
+
+
+
+
+
+
+
+
+
+ age of the Universe today
Neff
sum of neutrino masses
neutrino density of the Universe
Ωc=h-ΔScav/93.14 Ā
Ωa=h-ΔSaav/93.14 Ā
Ωb
running spectral index, k_0=0.6 Mpc-1
residual to sound horizon perturbation ratio,
dark energy equation of state parameter
primordial helium fraction
Y_{\odot}
[Parameter in e-parameter ΛCDM fit.] Derived parameter in g-parameter ΛCDM fit.] Extended model parameter, Planck + BAO data [2]
\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\\* Parameters in e-parameter ΛCDM fit.] Derived parameter in g-parameter ΛCDM fit.] Extended model parameter, Planck + BAO data [2]
\n\\* Parameters in e-parameter ΛCDM fit.] Derived parameter in g-parameter ΛCDM fit.] Extended model parameter, Planck + BAO data [2] [3] [4] [5] [6] [7] [8] [9] [10] [11] [12] [13] [14] [15] [16] [17] [18] [19] [20] [21] [22] [23] [24] [25] [26] [27] [28] [29] [30] [31] [32] [33] [34] [35] [36] [37] [38] [39] [40] [41] [42] [43] [44] [45] [46] [47]\n[48] [49] [50] [51] [52] [53] [54] [55] [56] [57] [58] [59] [60] [61] [62] [63] [64] [65] [66] [67] [68] [69] [70] [71] [72] [73] [74] [75] [76] [77] [78] [79] [80] [81] [82] [83]\n[84]\n[85]\n[86]\n[87]\n[88]\n[89]\n[90]\n[91]\n[92]\n[93]\n[94]\n[95]\n[96]\n[97]\n[98]\n[99]\n[100]\n[101]\n[102]\n[103]\n[104]\n[105]\n[106]\n[107]\n[108]\n[109]\n[110]\n[111]\n[112]\n[113]\n[114]\n[115]\n[116]\n[117]\n[118]\n[119]\n[120]\n[121]\n[122]\n[123]\n[124]\n[125]\n[126]\n[127]\n[128]\n[129]\n[130]\n[131]\n[132]\n[133]\n[134]\n[135]\n[136]\n[137]\n[138]\n[139]\n[140]\n[141]\n[142]\n[143]\n[144]\n[145]\n[146]\n[147]\n[48]
\n[49]
\n[50]
\n[51]
\n[52]
\n[53]
\n[54]
\n[55]
\n[56]
\n[57]
\n[58]
\n[59]
\n[60]
\n[61]
\n[62]
\n[63]
\n[64]
\n[65]
\n[66]
\n[67]
\n[68]
\n[69]
\n[70]
\n[71]
\n[72]
\n[73]
\n[74]
\n[75]
\n[76]
\n[77]
\n[78]
\n[79]
\n[80]
\n[81]
\n[82]
\n[83]
\n---\nhubble-to-photon ratio (from HRD)\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhubble density of the Universe
at Hubble expansion rate
scalling factor for Hubble expansion rate
Hubble constant
scalling factor of decelerating constant
critical density of the Universe
hubble-to-photon ratio (from HRD)
\nhub-photon ratio (from HRD)
\nhub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+hub-photon density of the Universe
(Peece 2018 6-parameter fit to ΛCDM cosmology)
+ hub-helium fraction Y_{\odot} \hspace{fill} &enspi;
+
+
+---PAGE_BREAK---
+
+# SUMMARY TABLES OF PARTICLE PROPERTIES
+
+Extracted from the Particle Listings of the
+*Review of Particle Physics*
+
+P.A. Zyla et al. (Particle Data Group),
+Prog. Theor. Exp. Phys. **2020**, 083C01 (2020)
+Available at http://pdg.lbl.gov
+
+©2020 Regents of the University of California
+(Approximate closing date for data: January 15, 2020)
+
+## GAUGE AND HIGGS BOSONS
+
+### $\gamma$ (photon)
+
+$$I(J^{PC}) = 0,1(1^{--})$$
+
+Mass $m < 1 \times 10^{-18}$ eV
+
+Charge $q < 1 \times 10^{-46}$ e (mixed charge)
+
+Charge $q < 1 \times 10^{-35}$ e (single charge)
+
+Mean life $\tau$ = Stable
+
+### g or gluon
+
+$$I(J^P) = 0(1^-)$$
+
+Mass $m = 0$ [a]
+
+SU(3) color octet
+
+### graviton
+
+$J = 2$
+
+Mass $m < 6 \times 10^{-32}$ eV
+
+### W
+
+$J = 1$
+
+Charge = $\pm 1$ e
+
+Mass $m = 80.379 \pm 0.012$ GeV
+
+W/Z mass ratio = $0.88147 \pm 0.00013$
+
+$m_Z - m_W = 10.809 \pm 0.012$ GeV
+
+$m_{W^+} - m_{W^-} = -0.029 \pm 0.028$ GeV
+
+Full width $\Gamma = 2.085 \pm 0.042$ GeV
+
+$\langle N_{\pi^{\pm}} \rangle = 15.70 \pm 0.35$
+
+$\langle N_{K^{\pm}} \rangle = 2.20 \pm 0.19$
+
+$\langle N_p \rangle = 0.92 \pm 0.14$
+
+$\langle N_{\text{charged}} \rangle = 19.39 \pm 0.08$
+
+W$^-$ modes are charge conjugates of the modes below.
+
+| W+ DECAY MODES | Fraction (Γf/Γ) | Confidence level | p
(MeV/c) |
|---|
| ℓ+ν | [b] (10.86 ± 0.09) % | | — | | e+ν | | μ+ν | | τ+ν |
+---PAGE_BREAK---
+
+
+
+
+ | hadrons |
+ (67.41 ± 0.27) % |
+ |
+ |
+
+
+ | π+γ |
+ < 7 |
+ × 10-6 |
+ 95% |
+ 40189 |
+
+
+ | Ds+γ |
+ < 1.3 |
+ × 10-3 |
+ 95% |
+ 40165 |
+
+
+ | cX |
+ (33.3 ± 2.6) % |
+ |
+ |
+ |
+
+
+ | cΣ |
+ (31 ±+13-11) % |
+ |
+ |
+ |
+
+
+ | invisible |
+ [c] (1.4 ± 2.9) % |
+ |
+ |
+ |
+
+
+ | π+π+π- |
+ < 1.01 |
+ × 10-6 |
+ 95% |
+ 40189 |
+
+
+
+
+**Z**
+
+$J = 1$
+
+Charge = 0
+
+Mass $m = 91.1876 \pm 0.0021$ GeV [$\sigma$]
+
+Full width $\Gamma = 2.4952 \pm 0.0023$ GeV
+
+$\Gamma(\ell^+ \ell^-) = 83.984 \pm 0.086$ MeV [b]
+
+$\Gamma(\text{invisible}) = 499.0 \pm 1.5$ MeV [e]
+
+$\Gamma(\text{hadrons}) = 1744.4 \pm 2.0$ MeV
+
+$\Gamma(\mu^+ \mu^-)/\Gamma(e^+ e^-) = 1.0001 \pm 0.0024$
+
+$\Gamma(\tau^+ \tau^-)/\Gamma(e^+ e^-) = 1.0020 \pm 0.0032$ [f]
+
+Average charged multiplicity
+
+$\langle N_{\text{charged}} \rangle = 20.76 \pm 0.16 \quad (\text{S} = 2.1)$
+
+Couplings to quarks and leptons
+
+$$g_V^\ell = -0.03783 \pm 0.00041$$
+
+$$g_V^\mu = 0.266 \pm 0.034$$
+
+$$g_V^d = -0.38^{+0.04}_{-0.05}$$
+
+$$g_A^\ell = -0.50123 \pm 0.00026$$
+
+$$g_A^\mu = 0.519^{+0.028}_{-0.033}$$
+
+$$g_A^d = -0.527^{+0.040}_{-0.028}$$
+
+$$g_{\nu\ell} = 0.5008 \pm 0.0008$$
+
+$$g_{\nu e} = 0.53 \pm 0.09$$
+
+$$g_{\nu\mu} = 0.502 \pm 0.017$$
+
+Asymmetry parameters [g]
+
+$A_e = 0.1515 \pm 0.0019$
+
+$A_\mu = 0.142 \pm 0.015$
+
+$A_\tau = 0.143 \pm 0.004$
+
+$A_s = 0.90 \pm 0.09$
+
+$A_c = 0.670 \pm 0.027$
+
+$A_b = 0.923 \pm 0.020$
+
+Charge asymmetry (%) at Z pole
+
+$A_{FB}^{(0\ell)} = 1.71 \pm 0.10$
+
+$A_{FB}^{(0u)} = 4 \pm 7$
+
+$A_{FB}^{(0s)} = 9.8 \pm 1.1$
+
+$A_{FB}^{(0c)} = 7.07 \pm 0.35$
+
+$A_{FB}^{(0b)} = 9.92 \pm 0.16$
+
+
+
+
+| Z DECAY MODES |
+Fraction (Γf/Γ) |
+Scale factor/
Confidence level |
+p
(MeV/c) |
+
+
+
+
+| e+e- |
+[h] (3.3632±0.0042) % |
+ |
+45594 |
+
+
+| μ+μ- |
+[h] (3.3662±0.0066) % |
+ |
+45594 |
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | τ+ τ- |
+ [h] ( 3.3696 ± 0.0083 ) % |
+ 45559 |
+
+
+ | ℓ+ ℓ- |
+ [b,h] ( 3.3658 ± 0.0023 ) % |
+ - |
+
+
+ | ℓ+ ℓ- ℓ+ ℓ- |
+ [j] ( 4.63 ± 0.21 ) × 10-6 |
+ 45594 |
+
+
+ | invisible |
+ [h] (20.000 ± 0.055 ) % |
+ - |
+
+
+ | hadrons |
+ [h] (69.911 ± 0.056 ) % |
+ - |
+
+
+ | (uū + cc) / 2 |
+ (11.6 ± 0.6 ) % |
+ - |
+
+
+ | (dd + ss + bb) / 3 |
+ (15.6 ± 0.4 ) % |
+ - |
+
+
+ | cc |
+ (12.03 ± 0.21 ) % |
+ - |
+
+
+ | bb |
+ (15.12 ± 0.05 ) % |
+ - |
+
+
+ | bb bb |
+ ( 3.6 ± 1.3 ) × 10-4 |
+ - |
+
+
+ | ggg |
+ < 1.1 % CL=95% |
+ - |
+
+
+ | π0γ |
+ < 2.01 × 10-5 CL=95% 45594 |
+ - |
+
+
+ | ηγ |
+ < 5.1 × 10-5 CL=95% 45592 |
+ - |
+
+
+ | ρ0γ |
+ < 2.5 × 10-5 CL=95% 45591 |
+ - |
+
+
+ | ωγ |
+ < 6.5 × 10-4 CL=95% 45590 |
+ - |
+
+
+ | η'(958)γ |
+ < 4.2 × 10-5 CL=95% 45589 |
+ - |
+
+
+ | φγ |
+ < 9 × 10-7 CL=95% 45588 |
+ - |
+
+
+ | γγ |
+ < 1.46 × 10-5 CL=95% 45594 |
+ - |
+
+
+ | π0 π0 |
+ < 1.52 × 10-5 CL=95% 45594 |
+ - |
+
+
+ | γγγ |
+ < 2.2 × 10-6 CL=95% 45594 |
+ - |
+
+
+ | π± W∓ |
+ [j] < 7 × 10-5 CL=95% 10167 |
+ - |
+
+
+ | ρ± W∓ |
+ [j] < 8.3 × 10-5 CL=95% 10142 |
+ - |
+
+
+ | J/ψ(1S)X |
+ ( 3.51 ± 0.23 ) × 10-3 S=1.1 - |
+ - |
+
+
+ | J/ψ(1S)γ |
+ < 1.4 × 10-6 CL=95% 45541 |
+ - |
+
+
+ | ψ(2S)X |
+ ( 1.60 ± 0.29 ) × 10-3 |
+ - |
+
+
+ | ψ(2S)γ |
+ < 4.5 × 10-6 CL=95% 45519 |
+ - |
+
+
+ | J/ψ(1S)J/ψ(1S) |
+ < 2.2 × 10-6 CL=95% 45489 |
+ - |
+
+
+ | χc1(1P)X |
+ ( 2.9 ± 0.7 ) × 10-3 |
+ - |
+
+
+ | χc2(1P)X |
+ < 3.2 × 10-3 CL=90% |
+ - |
+
+
+ | Υ(1S) X + Υ(2S) X + Υ(3S) X |
+ ( 1.0 ± 0.5 ) × 10-4 |
+ - |
+
+
+ | Υ(1S)X |
+ < 3.4 × 10-6 CL=95% |
+ - |
+
+
+ | Υ(1S)γ |
+ < 2.8 × 10-6 CL=95% 45103 |
+ - |
+
+
+ | Υ(2S)X |
+ < 6.5 × 10-6 CL=95% |
+ - |
+
+
+ | Υ(2S)γ |
+ < 1.7 × 10-6 CL=95% 45043 |
+ - |
+
+
+ | Υ(3S)X |
+ < 5.4 × 10-6 CL=95% |
+ - |
+
+
+ | Υ(3S)γ |
+ < 4.8 × 10-6 CL=95% 45006 |
+ - |
+
+
+ | Υ(1, 2, 3S) Υ(1, 2, 3S) |
+ < 1.5 × 10-6 CL=95% |
+ - |
+
+
+ | (D0/D0) X |
+ (20.7 ± 2.0 ) % - |
+ - |
+
+
+ | D∓X |
+ (12.2 ± 1.7 ) % - |
+ - |
+
+
+ | D*(2010)±X [j] |
+ (11.4 ± 1.3 ) % - |
+ - |
+
+
+ | Ds1(2536)±X (3.6 ± 0.8) × 10-3 |
+ - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- ---------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------------- CL=95% e+e-γ [k] (6.08 ± 0.13) %— μ+ μ-γ [k] (1.59 ± 0.13) %— τ+ τ-γ [l] < 7.3 × 10-4 CL=95% 45559
[n] < 6.8 × 10-6 CL=95% — eqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqqspan=9em>⃝ b-baryon X [k] (1.38 ± 0.22) %— Anomalous γ + hadrons [l] < 3.2 × 10-3 e+e-γ [l] < 5.2 × 10-4 μ+ μ-γ [l] < 5.6 × 10-4 τ+ τ-γ [l] < 7.3 × 10-4 esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝
esJ⃝ |
+
+
+---PAGE_BREAK---
+
+| e±μ&mpart; | LF | [J] < 7.5 | × 10-7 | CL=95% | 45594 | | e±τ&mpart; | LF | [J] < 9.8 | × 10-6 | CL=95% | 45576 | | μ±τ&mpart; | LF | [J] < 1.2 | × 10-5 | CL=95% | 45576 | | p e | L,B | < 1.8 | × 10-6 | CL=95% | 45589 | | pμ | L,B | < 1.8 | × 10-6 | CL=95% | 45589 |
+
+See Particle Listings for 4 decay modes that have been seen / not seen.
+
+### H⁰
+
+$J = 0$
+
+Mass $m = 125.10 \pm 0.14$ GeV
+
+Full width $\Gamma < 0.013$ GeV, CL = 95% (assumes equal on-shell and off-shell effective couplings)
+
+### H⁰ Signal Strengths in Different Channels
+
+Combined Final States = 1.13 ± 0.06
+
+$WW^* = 1.19 \pm 0.12$
+
+$ZZ^* = 1.20^{+0.12}_{-0.11}$
+
+$\gamma\gamma = 1.11^{+0.10}_{-0.09}$
+
+$c\bar{c}$ Final State < 110, CL = 95%
+
+$b\bar{b} = 1.04 \pm 0.13$
+
+$\mu^+\mu^- = 0.6 \pm 0.8$
+
+$\tau^+\tau^- = 1.15^{+0.16}_{-0.15}$
+
+$Z\gamma < 6.6$, CL = 95%
+
+top Yukawa coupling < 1.7, CL = 95%
+
+$t\bar{t}H^0$ Production = 1.28 ± 0.20
+
+$H^0$ Production Cross Section in $pp$ Collisions at $\sqrt{s} = 13$ TeV = $59 \pm 5$ pb
+
+| H0 DECAY MODES | Fraction (Γf/Γ) | Confidence level | ρ
(MeV/c) |
|---|
| e+e- | <3.6 × 10-4 | 95% | 62550 | | J/ψγ | <3.5 × 10-4 | 95% | 62511 | | J/ψJ/ψ | <1.8 × 10-3 | 95% | 62473 | | ψ(2S)γ | <2.0 × 10-3 | 95% | 62495 | | Υ(1S)γ | <4.9 × 10-4 | 95% | 62192 | | Υ(2S)γ | <5.9 × 10-4 | 95% | 62148 | | Υ(3S)γ | <5.7 × 10-4 | 95% | 62121 | | Υ(nS)Υ(mS) | <1.4 × 10-3 | 95% | - | | ρ(770)γ | <8.8 × 10-4 | 95% | 62547 | | φ(1020)γ | <4.8 × 10-4 | 95% | 62546 | | eμ | LF <6.1 × 10-5 | 95% | 62550 | | eτ | LF <4.7 × 10-3 | 95% | 62537 | | μτ | LF <2.5 × 10-3 | 95% | 62537 | | γ invisible | <4.6 % | 95% | - |
+
+## Neutral Higgs Bosons, Searches for
+
+### Mass limits for heavy neutral Higgs bosons ($H_2^0, A^0$) in the MSSM
+
+$m > 389$ GeV, CL = 95% ($\tan\beta = 10$)
+
+$m > 863$ GeV, CL = 95% ($\tan\beta = 20$)
+
+$m > 1157$ GeV, CL = 95% ($\tan\beta = 30$)
+
+$m > 1341$ GeV, CL = 95% ($\tan\beta = 40$)
+
+$m > 1496$ GeV, CL = 95% ($\tan\beta = 50$)
+
+$m > 1613$ GeV, CL = 95% ($\tan\beta = 60$)
+---PAGE_BREAK---
+
+Charged Higgs Bosons ($H^\pm$ and $H^{\pm\pm}$), Searches for
+
+Mass limits for $m_{H^+} < m(\text{top})$
+
+$m > 155$ GeV, CL = 95%
+
+Mass limits for $m_{H^+} > m(\text{top})$
+
+| m > 181 GeV, CL = 95% | (tanβ = 10) | | m > 249 GeV, CL = 95% | (tanβ = 20) | | m > 390 GeV, CL = 95% | (tanβ = 30) | | m > 894 GeV, CL = 95% | (tanβ = 40) | | m > 1017 GeV, CL = 95% | (tanβ = 50) | | m > 1103 GeV, CL = 95% | (tanβ = 60) |
+
+New Heavy Bosons
+($W'$, $Z'$, leptoquarks, etc.),
+Searches for
+
+Additional W Bosons
+
+$W'$ with standard couplings
+
+Mass $m > 5200$ GeV, CL = 95% (pp direct search)
+
+$W_R$ (Right-handed W Boson)
+
+Mass $m > 715$ GeV, CL = 90% (electroweak fit)
+
+Additional Z Bosons
+
+$Z'_{SM}$ with standard couplings
+
+Mass $m > 4.500 \times 10^3$ GeV, CL = 95% (pp direct search)
+
+$Z_{LR}$ of $SU(2)_L \times SU(2)_R \times U(1)$ (with $g_L = g_R$)
+
+Mass $m > 630$ GeV, CL = 95% (pP direct search)
+
+Mass $m > 1162$ GeV, CL = 95% (electroweak fit)
+
+$Z_\chi$ of $SO(10) \to SU(5) \times U(1)_\chi$ (with $g_\chi=e/\cos\theta_W$)
+
+Mass $m > 4.100 \times 10^3$ GeV, CL = 95% (pp direct search)
+
+$Z_\psi$ of $E_6 \to SO(10) \times U(1)_\psi$ (with $g_\psi=e/\cos\theta_W$)
+
+Mass $m > 3900$ GeV, CL = 95% (pp direct search)
+
+$Z_\eta$ of $E_6 \to SU(3) \times SU(2) \times U(1) \times U(1)_\eta$ (with $g_\eta=e/\cos\theta_W$)
+
+Mass $m > 3.900 \times 10^3$ GeV, CL = 95% (pp direct search)
+
+Scalar Leptoquarks
+
+| $m > 1050$ GeV, CL = 95% | (1st gen., pair prod., $B(\tau t)=1$) | | $m > 1755$ GeV, CL = 95% | (1st gen., single prod., $B(\tau b)=1$) | | $m > 1420$ GeV, CL = 95% | (2nd gen., pair prod., $B(\mu t)=1$) | | $m > 660$ GeV, CL = 95% | (2nd gen., single prod., $B(\mu q)=1$) | | $m > 900$ GeV, CL = 95% | (3rd gen., pair prod., $B(e q)=1$) | | $m > 740$ GeV, CL = 95% | (3rd gen., single prod., $B(e q)=1$) |
+
+(See the Particle Listings in the Full Review of Particle Physics for assumptions on leptoquark quantum numbers and branching fractions.)
+
+Diquarks
+
+Mass $m > 6000$ GeV, CL = 95% ($E_6$ diquark)
+
+Axigluon
+
+Mass $m > 6100$ GeV, CL = 95%
+---PAGE_BREAK---
+
+Axions ($A^0$) and Other
+Very Light Bosons, Searches for
+
+See the review on "Axions and other similar particles."
+
+The best limit for the half-life of neutrinoless double beta decay with Majoron emission is > 7.2 × 10²⁴ years (CL = 90%).
+
+NOTES
+
+In this Summary Table:
+
+When a quantity has “(S = ...)” to its right, the error on the quantity has been enlarged by the “scale factor” S, defined as $S = \sqrt{\chi^2/(N-1)}$, where N is the number of measurements used in calculating the quantity.
+
+A decay momentum p is given for each decay mode. For a 2-body decay, p is the momentum of each decay product in the rest frame of the decaying particle. For a 3-or-more-body decay, p is the largest momentum any of the products can have in this frame.
+
+[a] Theoretical value. A mass as large as a few MeV may not be precluded.
+
+[b] *l* indicates each type of lepton (e, μ, and τ), not sum over them.
+
+[c] This represents the width for the decay of the W boson into a charged particle with momentum below detectability, $p < 200$ MeV.
+
+[d] The Z-boson mass listed here corresponds to a Breit-Wigner resonance parameter. It lies approximately 34 MeV above the real part of the position of the pole (in the energy-squared plane) in the Z-boson propagator.
+
+[e] This partial width takes into account Z decays into $\nu\bar{\nu}$ and any other possible undetected modes.
+
+[f] This ratio has not been corrected for the $\tau$ mass.
+
+[g] Here $A \equiv 2g_Vg_A/(g_V^2+g_A^2)$.
+
+[h] This parameter is not directly used in the overall fit but is derived using the fit results; see the note “The Z boson” and ref. LEP-SLC 06 (Physics Reports (Physics Letters C) **427** 257 (2006)).
+
+[i] Here *l* indicates *e* or *μ*.
+
+[j] The value is for the sum of the charge states or particle/antiparticle states indicated.
+
+[k] This value is updated using the product of (i) the $Z \to b\bar{b}$ fraction from this listing and (ii) the b-hadron fraction in an unbiased sample of weakly decaying b-hadrons produced in Z-decays provided by the Heavy Flavor Averaging Group (HFLAV, http://www.slac.stanford.edu/xorg/hflav/osc/PDG_2009/#FRACZ).
+
+[l] See the Z Particle Listings in the Full Review of Particle Physics for the $\gamma$ energy range used in this measurement.
+
+[n] For $m_{\gamma\gamma} = (60 \pm 5)$ GeV.
+---PAGE_BREAK---
+
+LEPTONS
+
+e
+
+$$
+J = \frac{1}{2}
+$$
+
+Mass $m = (548.579909070 \pm 0.000000016) \times 10^{-6}$ u
+
+$$
+\text{Mass } m = 0.5109989461 \pm 0.000000031 \text{ MeV}
+$$
+
+$$
+|m_{e^+} - m_{e^-}|/m < 8 \times 10^{-9}, \text{ CL} = 90\%
+$$
+
+$$
+|q_{e^+} + q_{e^-}|/e < 4 \times 10^{-8}
+$$
+
+Magnetic moment anomaly
+
+$$
+(g-2)/2 = (1159.65218091 \pm 0.00000026) \times 10^{-6}
+$$
+
+$$
+(g_{e^{+}} - g_{e^{-}}) / g_{\text{average}} = (-0.5 \pm 2.1) \times 10^{-12}
+$$
+
+Electric dipole moment $d < 0.11 \times 10^{-28}$ e cm, CL = 90%
+
+Mean life $\tau > 6.6 \times 10^{28}$ yr, CL = 90% [a]
+
+μ
+
+$$
+J = \frac{1}{2}
+$$
+
+Mass $m = 0.1134289257 \pm 0.0000000025$ u
+
+$$
+\text{Mass } m = 105.6583745 \pm 0.0000024 \text{ MeV}
+$$
+
+$$
+\text{Mean life } \tau = (2.1969811 \pm 0.0000022) \times 10^{-6} \text{ s}
+$$
+
+$$
+\begin{gathered}
+\tau_{\mu^{+}/\tau_{\mu^{-}}} = 1.00002 \pm 0.00008 \\
+c\tau = 658.6384 \text{ m}
+\end{gathered}
+$$
+
+Magnetic moment anomaly $(g-2)/2 = (11659209 \pm 6) \times 10^{-10}$
+
+$$
+(g_{\mu^+} - g_{\mu^-}) / g_{\text{average}} = (-0.11 \pm 0.12) \times 10^{-8}
+$$
+
+Electric diapole moment $|d| < 1.8 \times 10^{-19}$ e cm, CL = 95%
+
+Decay parameters [b]
+
+$$
+\rho = 0.74979 \pm 0.00026
+$$
+
+$\eta = 0.057 \pm 0.034$
+
+$\delta = 0.75047 \pm 0.00034$
+
+$$
+\xi P_{\mu} = 1.0009^{+0.0016}_{-0.0007} [c]
+$$
+
+$$
+\xi P_{\mu} \delta / \rho = 1.0018^{+0.0016}_{-0.0007} [c]
+$$
+
+$\xi' = 1.00 \pm 0.04$
+
+$\xi'' = 0.98 \pm 0.04$
+
+$\alpha/A = (0 \pm 4) \times 10^{-3}$
+
+$\alpha'/A = (-10 \pm 20) \times 10^{-3}$
+
+$\beta/A = (4 \pm 6) \times 10^{-3}$
+
+$\beta'/A = (2 \pm 7) \times 10^{-3}$
+
+$\bar{\eta} = 0.02 \pm 0.08$
+
+$\mu^+$ modes are charge conjugates of the modes below.
+
+
+
+
+ |
+ μ- DECAY MODES
+ |
+
+ Fraction (Γf/Γ)
+ |
+
+ Confidence level
+ |
+
+ p (MeV/c)
+ |
+
+
+
+
+ |
+ e-νeνμ
+ |
+
+ ≈ 100%
+ |
+
+ |
+
+ 53
+ |
+
+
+ |
+ e-νeeνμγ
+ |
+
+ [d] (6.0±0.5) × 10-8
+ |
+
+ |
+
+ 53
+ |
+
+
+ |
+ e-νeνμe+e-
+ |
+
+ [e] (3.4±0.4) × 10-5
+ |
+
+ |
+
+ 53
+ |
+
+
+ |
+ Lepton Family number (LF) violating modes
+ |
+
+
+ |
+ e-νeνμ
+ |
+
+ LF [f] < 1.2
+ |
+
+ %
+ |
+
+ 90%
+ |
+
+
+ |
+ e-γ
+ |
+
+ LF < 4.2
+ |
+
+ × 10-13
+ |
+
+ 90%
+ |
+
+
+ |
+ e-e+e-
+ |
+
+ LF < 1.0
+ |
+
+ × 10-12
+ |
+
+ 90%
+ |
+
+
+ |
+ e-2γ
+ |
+
+ LF < 7.2
+ |
+
+ × 10-11
+ |
+
+ 90%
+ |
+
+
+
+---PAGE_BREAK---
+
+$$J = \frac{1}{2}$$
+
+Mass $m = 1776.86 \pm 0.12$ MeV
+$(m_{\tau^+} - m_{\tau^-})/m_{\text{average}} < 2.8 \times 10^{-4}$, CL = 90%
+Mean life $\tau = (290.3 \pm 0.5) \times 10^{-15}$ s
+$c\tau = 87.03 \ \mu\text{m}$
+Magnetic moment anomaly > -0.052 and < 0.013, CL = 95%
+$Re(d_{\tau}) = -0.220$ to $0.45 \times 10^{-16}$ ecm, CL = 95%
+$Im(d_{\tau}) = -0.250$ to $0.0080 \times 10^{-16}$ ecm, CL = 95%
+
+**Weak dipole moment**
+
+$Re(d_{\tau}^{W}) < 0.50 \times 10^{-17}$ e cm, CL = 95%
+$Im(d_{\tau}^{W}) < 1.1 \times 10^{-17}$ e cm, CL = 95%
+
+**Weak anomalous magnetic dipole moment**
+
+$Re(\alpha_{\tau}^{W}) < 1.1 \times 10^{-3}$, CL = 95%
+$Im(\alpha_{\tau}^{W}) < 2.7 \times 10^{-3}$, CL = 95%
+$\tau^{\pm} \rightarrow \pi^{\pm} K_S^{0} \nu_{\tau}$ (RATE DIFFERENCE) / (RATE SUM) =
+(-0.36 \pm 0.25)\%$
+
+**Decay parameters**
+
+See the τ Particle Listings in the Full Review of Particle Physics for a note concerning τ-decay parameters.
+
+$$\rho(e \text{ or } \mu) = 0.745 \pm 0.008$$
+
+$$\rho(e) = 0.747 \pm 0.010$$
+
+$$\rho(\mu) = 0.763 \pm 0.020$$
+
+$$\xi(e \text{ or } \mu) = 0.985 \pm 0.030$$
+
+$$\xi(e) = 0.994 \pm 0.040$$
+
+$$\xi(\mu) = 1.030 \pm 0.059$$
+
+$$\eta(e \text{ or } \mu) = 0.013 \pm 0.020$$
+
+$$\eta(\mu) = 0.094 \pm 0.073$$
+
+$$(\delta\xi)(e \text{ or } \mu) = 0.746 \pm 0.021$$
+
+$$(\delta\xi)(e) = 0.734 \pm 0.028$$
+
+$$(\delta\xi)(\mu) = 0.778 \pm 0.037$$
+
+$$\xi(\pi) = 0.993 \pm 0.022$$
+
+$$\xi(\rho) = 0.994 \pm 0.008$$
+
+$$\xi(a_1) = 1.001 \pm 0.027$$
+
+$\xi(\text{all hadronic modes}) = 0.995 \pm 0.007$
+
+$\bar{\eta}(\mu)$ PARAMETER = -1.3 ± 1.7
+
+$\xi_K(e)$ PARAMETER = -0.4 ± 1.2
+
+$\xi_K(\mu)$ PARAMETER = 0.8 ± 0.6
+
+$\tau^+$ modes are charge conjugates of the modes below. "h±" stands for $\pi^\pm$ or $K^\pm$. "ℓ" stands for e or $\mu$. "Neutrals" stands for $\gamma$'s and/or $\pi^0$'s.
+
+
+
+
+ | τ- DECAY MODES |
+ Fraction (Γf/Γ) |
+ Scale factor/
Confidence level |
+ p
(MeV/c) |
+
+
+
+
+ | Modes with one charged particle |
+
+
+ particle- ≥ 0 neutrals
(“1-prong”)
≥ 0K0ντ
(85.24 ± 0.06 ) % |
+ |
+ |
+ - |
+
+
+ particle- ≥ 0 neutrals
≥ 0K0Lντ
(84.58 ± 0.06 ) % |
+ |
+ |
+ - |
+
+
+ μ-ν̄μντ
[g] (17.39 ± 0.04 ) % |
+ |
+ |
+ 885 |
+
+
+ μ-ν̄μντγ
[e] (3.67 ± 0.08 ) × 10-3 |
+ |
+ |
+ 885 |
+
+
+ e-ν̄eντ
[g] (17.82 ± 0.04 ) % |
+ |
+ |
+ 888 |
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | e- ∇eνTγ |
+ [e] (1.83 ± 0.05) % |
+ 888 |
+
+
+ | h- ≥ 0K0L νT |
+ (12.03 ± 0.05) % |
+ 883 |
+
+
+ | h- νT |
+ (11.51 ± 0.05) % |
+ 883 |
+
+
+ | π- νT |
+ [g] (10.82 ± 0.05) % |
+ 883 |
+
+
+ | K- νT |
+ [g] (6.96 ± 0.10) × 10-3 |
+ 820 |
+
+
+ | h- ≥ 1 neutralsνT |
+ (37.01 ± 0.09) % |
+ - |
+
+
+ | h- ≥ 1π0 νT (ex.K0) |
+ (36.51 ± 0.09) % |
+ - |
+
+
+ | h- π0 νT |
+ (25.93 ± 0.09) % |
+ 878 |
+
+
+ | π-π0 νT |
+ [g] (25.49 ± 0.09) % |
+ 878 |
+
+
+ | π-π0 non-ρ(770)νT |
+ (3.0 ± 3.2) × 10-3 |
+ 878 |
+
+
+ | K- π0 νT |
+ [g] (4.33 ± 0.15) × 10-3 |
+ 814 |
+
+
+ | h- ≥ 2π0 νT |
+ (10.81 ± 0.09) % |
+ - |
+
+
+ | h- 2π0 νT |
+ (9.48 ± 0.10) % |
+ 862 |
+
+
+ | h- 2π0 νT (ex.K0) |
+ (9.32 ± 0.10) % |
+ 862 |
+
+
+ | π- 2π0 νT (ex.K0) |
+ [g] (9.26 ± 0.10) % |
+ 862 |
+
+
+ | π- 2π0 νT (ex.K0), scalar |
+ < 9 × 10-3 |
+ CL=95% |
+
+
+ | π- 2π0 νT (ex.K0), vector |
+ < 7 × 10-3 |
+ CL=95% |
+
+
+ | K- 2π0 νT (ex.K0) |
+ [g] (6.5 ± 2.2) × 10-4 |
+ 796 |
+
+
+ | h- ≥ 3π0 νT |
+ (1.34 ± 0.07) % |
+ - |
+
+
+ | h- ≥ 3π0 νT (ex. K0) |
+ (1.25 ± 0.07) % |
+ - |
+
+
+ | h- 3π0 νT |
+ (1.18 ± 0.07) % |
+ 836 |
+
+
+ | π- 3π0 νT (ex.K0) |
+ [g] (1.04 ± 0.07) % |
+ 836 |
+
+
+ | K- 3π0 νT (ex.K0, η) |
+ [g] (4.8 ± 2.1) × 10-4 |
+ 765 |
+
+
+ | h- 4π0 νT (ex.K0) |
+ (1.6 ± 0.4) × 10-3 |
+ 800 |
+
+
+ | h- 4π0 νT (ex.K0, η) |
+ [g] (1.1 ± 0.4) × 10-3 |
+ 800 |
+
+
+ | aI(1260)νT → π-γνT |
+ (3.8 ± 1.5) × 10-4 |
+ - |
+
+
+ | K- ≥ 0π0 ≥ 0K0 ≥ 0γ νT |
+ (1.552±0.029) % |
+ 820 |
+
+
+ | K- ≥ 1 (π0 or K0 or γ) νT |
+ (8.59 ± 0.28) × 10-3 |
+ - |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
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+
+
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+
+
+
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+
+
+
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+
+
+
+
+
+
+
+
+
+
+
+
+
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+
+
+
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+
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+
+
+
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+
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+
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+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+ Modes with K*'s
(particles)
KS*(particles)
h^-KS*νT
π-KS*νT
π-KS*(non-K*(892))νT
K^-KS*νT
K^-KS
h^-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS
π-KS♩
π-K♩ | (9.43 ± 0.28) × 10⁻³
(9.87 ± 0.14) × 10⁻³
(8.38 ± 0.14) × 10⁻³
(5.4 ± 2.1) × 10⁻⁴
(1.486 ± 0.034) × 10⁻³
(2.99 ± 0.07) × 10⁻³
(5.32 ± 0.13) × 10⁻³
(3.82 ± 0.13) × 10⁻³
(2.2 ± 0.5) × 10⁻³
(1.50 ± 0.07) × 10⁻³
(4.08 ± 0.25) × 10⁻³
(2.6 ± 2.3) × 10⁻⁴
< 1.6 × 10⁻⁴
(1.55 ± 0.24) × 10⁻³
(2.35 ± 0.06) × 10⁻⁴
(1.08 ± 0.24) × 10⁻³
(2.35 ± 0.06) × 10⁻⁴
(3.6 ± 1.2) × 10⁻⁴
(1.82 ± 0.21) × 10⁻⁵
(1.08 ± 0.21) × 10⁻⁵
(6.8 ± 1.5) × 10⁻⁶
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+ CL=95%
+---PAGE_BREAK---
+
+
+
+
+ | f1(1420)π-ντ → π-K0SK0Sπ0ντ |
+ ( 2.4 ± 0.8 ) × 10-6 |
+ - |
+
+
+ | π-K0SK0Lπ0ντ |
+ [g] ( 3.2 ± 1.2 ) × 10-4 |
+ 614 |
+
+
+ | π-K0LK0Lπ0ντ |
+ ( 1.82 ± 0.21 ) × 10-5 |
+ 614 |
+
+
+ | K-K0SK0Sντ |
+ < 6.3 |
+ × 10-7 CL=90% |
+
+
+ | K-K0SK0Sπ0ντ |
+ < 4.0 |
+ × 10-7 CL=90% |
+
+
+ | K0h+h-h- ≥ 0 neutrals ντ |
+ < 1.7 |
+ × 10-3 CL=95% |
+
+
+ | K0h+h-h-ντ |
+ [g] ( 2.5 ± 2.0 ) × 10-4 |
+ 760 |
+
+
+
+
+Modes with three charged particles
+
+
+
+
+ | h-h-h+ ≥ 0 neutrals ≥ 0K0LνT |
+ (15.20 ± 0.06) % |
+ 861 |
+
+
+ h-h-h+ ≥ 0 neutrals νT
(ex. K0S → π+π-)
("3-prong") |
+ (14.55 ± 0.06) % |
+ 861 |
+
+
+ | h-h-h+νT |
+ (9.80 ± 0.05) % |
+ 861 |
+
+
+ | h-h-h+νT (ex.K0) |
+ (9.46 ± 0.05) % |
+ 861 |
+
+
+ | h-h-h+νT (ex.K0,ω) |
+ (9.43 ± 0.05) % |
+ 861 |
+
+
+ | π-π+π-νT |
+ (9.31 ± 0.05) % |
+ 861 |
+
+
+ | π-π+π-νT (ex.K0) |
+ (9.02 ± 0.05) % |
+ 861 |
+
+
+ π-π+π-νT (ex.K0), non-axial vector
(ex. K0S,ω) |
+ < 2.4 % |
+ CL=95% |
+
+
+ | π-π+π-νT (ex.K0,ω) |
+ [g] (8.99 ± 0.05) % |
+ 861 |
+
+
+ | h-h-h+ ≥ 1 neutrals νT |
+ (5.29 ± 0.05) % |
+ - |
+
+
+ | h-h-h+ ≥ 1π0νT (ex. K0) |
+ (5.09 ± 0.05) % |
+ - |
+
+
+ | h-h-h+π0νT |
+ (4.76 ± 0.05) % |
+ 834 |
+
+
+ | h-h-h+π0νT (ex.K0) |
+ (4.57 ± 0.05) % |
+ 834 |
+
+
+ | h-h-h+π0νT (ex. K0, ω) |
+ (2.79 ± 0.07) % |
+ 834 |
+
+
+ | π-π+π-π0νT |
+ (4.62 ± 0.05) % |
+ 834 |
+
+
+ | π-π+π-π0νT (ex.K0) |
+ (4.49 ± 0.05) % |
+ 834 |
+
+
+ | π-π+π-π0νT(ex.K0,ω) |
+ [g] (2.74 ± 0.07) % |
+ 834 |
+
+
+ | h-h-h+≥ 2π°ν°T ex. K°) |
+ (5.17 ± 0.31) × 10⁻³% |
+ - |
+
+
+ | h-h-hSUPSUP+2π°ν°T) |
+ (5.05 ± 0.31) × 10⁻³% |
+ 797% |
+
+
+ | hSUPSUP- hSUPSUP+2π°ν°T (ex.K°) |
+ (4.95 ± 0.31) × 10⁻³% |
+ 797% |
+
+
+ | hSUPSUP- hSUPSUP+2π°ν°T (ex.K°,ω,η) |
+ [g] (10 ± 4) × 10⁻⁴% |
+ 797% |
+
+
+ | hSUPSUP- hSUPSUP+3π°ν°T) |
+ (2.13 ± 0.30) × 10⁻⁴% |
+ 794% |
+
+
+ | 2πSUPSUP- πSUPSUP+3π°ν°T (ex.K°) |
+ (1.95 ± 0.30) × 10⁻⁴% |
+ 794% |
+
+
+ 2πSUPSUP- πSUPSUP+3π°ν°T (ex.K°, η,
f₁(1285)) |
+ (1.7 ± 0.4) × 10⁻⁴% |
+ - |
+
+
+ 2πSUPSUP- πSUPSUP+3π°ν°T (ex.K°, η,
ω, f₁(1285)) [g] |
+ (1.4 ± 2.7) × 10⁻⁵% |
+ - |
+
+
+ | KSUPSUP- hSUPSUP≥ 0 neutrals ν°T) |
+ (6.29 ± 0.14) × 10⁻³% |
+ 794% |
+
+
+ | KSUPSUP- hSUPSUP+ π°ν°T (ex.K°) |
+ (4.37 ± 0.07) × 10⁻³% |
+ 794% |
+
+
+ | KSUPSUP- hSUPSUP+ π°-π°ν°T (ex.K°) |
+ (8.6 ± 1.2) × 10⁻⁴% |
+ 763% |
+
+
+ | KSUPSUP- πSUPSUP+ π°-≥ 0 neutrals ν°T) |
+ (4.77 ± 0.14) × 10⁻³% |
+ 794% |
+
+
+ | KSUPSUP- πSUPSUP+ π°-≥ 0π°ν°T (ex.K°) |
+ (3.73 ± 0.13) × 10⁻³% |
+ 794% |
+
+
+ | KSUPSUP- πSUPSUP+ π°-ν°T (ex.K°) |
+ (3.45 ± 0.07) × 10⁻³% |
+ 794% |
+
+
+ | KUPSUP- πSUPSUP+ π°-ν°T (ex.K°) |
+ (2.93 ± 0.07) × 10⁻³% |
+ 794% |
+
+
+ | KUPSUP- πSUPSUP+ π°-ν°T (ex.K°,ω) |
+ [g] (2.93 ± 0.07) × 10⁻³% |
+ 794% |
+
+
+ | KUPSUP- ρ°ν°T → KUPSUP+ π°-π°ν°T (ex.K°) |
+ (1.4 ± 0.5) × 10⁻³% |
+ - |
+
+
+ | KUPSUP- πUPSUP+ π°-π°ν°T (ex.K°) |
+ (1.31 ± 0.12) × 10⁻³% |
+ 763% |
+
+
+ | KUPSUP- πUPSUP+ π°-π°ν°T (ex.K°) |
+ (7.9 ± 1.2) × 10⁻⁴% |
+ 763% |
+
+
+ | KUPSUP- πUPSUP+ π°-π°ν°T (ex.K°,η) |
+ (7.6 ± 1.2) × 10⁻⁴% |
+ 763% |
+
+
+ | KUPSUP- πUPSUP+ π°-π°ν°T (ex.K°,ω) |
+ (3.7 ± 0.9) × 10⁻⁴% |
+ 763% |
+
+
+ | KUPSUP- πUPSUP+ π°-π°ν°T (ex.K°,ω,η) | [g] | (3.9 ± 1.4) × 10⁻⁴% | CL=95% | | CL=95% |
|---|
| KUPSUP- πUPSUP+ ≥ 0 neutrals ν°T) | < 9 × 10⁻⁴% | | 685% |
|---|
+
+
+---PAGE_BREAK---
+
+
+
+
+ | K- K+ π- ≥ 0 neut. ντ |
+ ( 1.496 ± 0.033 ) × 10-3 |
+ 685 |
+
+
+ | K- K+ π- ντ |
+ [g] ( 1.435 ± 0.027 ) × 10-3 |
+ 685 |
+
+
+ | K- K+ π- π0 ντ |
+ [g] ( 6.1 ± 1.8 ) × 10-5 |
+ 618 |
+
+
+ | K- K+ K- ντ |
+ ( 2.2 ± 0.8 ) × 10-5 |
+ S=5.4 |
+ 472 |
+
+
+ | K- K+ K- ντ (ex. φ) |
+ < 2.5 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | K- K+ K- π0 ντ |
+ < 4.8 |
+ × 10-6 |
+ CL=90% |
+ 345 |
+
+
+ | π- K+ π- ≥ 0 neut. ντ |
+ < 2.5 |
+ × 10-3 |
+ CL=95% |
+ 794 |
+
+
+ | e- e- e+ νeeνe |
+ ( 2.8 ± 1.5 ) × 10-5 |
+ |
+ |
+ 888 |
+
+
+ | μ- e- e+ νe μνe |
+ < 3.2 |
+ × 10-5 |
+ CL=90% |
+ 885 |
+
+
+ | π- μ- μ+ νe |
+ < 1.14 |
+ × 10-5 |
+ CL=90% |
+ 870 |
+
+
+ | Modes with five charged particles |
+
+
+ 3h- 2h+ ≥ 0 neutrals ντ
(ex. KS0 → π- π+)
("5-prong") |
+ ( 9.9 ± 0.4 ) × 10-4 |
+ |
+ |
+ 794 |
+
+
+ | 3h- 2h+ ντ (ex.KS0) |
+ ( 8.29 ± 0.31 ) × 10-4 |
+ |
+ |
+ 794 |
+
+
+ | 3π- 2π+ νT (ex.KS0, ω) |
+ ( 8.27 ± 0.31 ) × 10-4 |
+ |
+ |
+ 794 |
+
+
+ 3π- 2π+ νT (ex.KS0, ω,
f₁(1285)) |
+ [g] ( 7.75 ± 0.30 ) × 10-4 |
+ |
+ |
+ - |
+
+
+ |
+
+
+ | K- 2π- 2π+ νT (ex.KS0) |
+ [g] ( 6 ± 12 ) × 10-7 |
+ |
+ |
+ 716 |
+
+
+ | K+ 3π- π+ νT |
+ < 5.0 |
+ × 10-6 |
+ CL=90% |
+ 716 |
+
+
+ | K+ K- 2π- π+ νT |
+ < 4.5 |
+ × 10-7 |
+ CL=90% |
+ 528 |
+
+
+ | 3h- 2h+ πS0 νT(ex.KS0) |
+ ( 1.65 ± 0.11 ) × 10-4 |
+ |
+ |
+ 746
746
- |
+
+
+ | ( 1.63 ± 0.11 ) × 10-4 |
+ |
+ |
+
+
+ | ( 1.11 ± 0.10 ) × 10-4 |
+ |
+ |
+
+
+ | f₁(1285) |
+
+
+ 3π- 2π+ πS0 νT(ex.KS0, η, ω,
f₁(1285)) |
+
+
+ | K- 2π- 2π+ πS0 νT(ex.KS0) [g] |
+
+
+ K*(892)superscript>
+3π-π+π-ν-τ
<8
×10-7
CL=90% |
+
+
+ 3h-2h+2π-ν-τ
<3.4
×10-6
CL=90% |
+
+
+Miscellaneous other allowed modes
+
+|
| (5π)- ντ | (7.8 ± 0.5) × 10-3 | | 800 |
|---|
4h-3h+ ≥ 0 neutrals ντ
(5π)ντ | < 3.0 × 10-7 | CL=90% | 682 |
|---|
| "7-prong" | | | |
|---|
| 4h-3h+ντ | < 4.3 × 10-7 | | 682 |
|---|
| 4h-3h+π0ντ | < 2.5 × 10-7 | | 612 |
|---|
| X-(S=-1)ντ | (2.92 ± 0.04)% | | - |
|---|
K*(892)ντ≥ 0 neutrals ≥
K*(892)ντ | (1.42 ± 0.18)% S=1.4
<K*(892)ντ> | < 3.0 × 10-7 | CL=90% | 665
<K*(892)ντ> |
|---|
| K*(892)ντ> π-Kντ | (1.20 ± 0.07)% S=1.8
<K*(892)ντ> | < 3.0 × 10-7 | CL=90% | 665
<K*(892)ντ> |
|---|
| K*(892)ντ≥ 0 neutrals ντ | (7.82 ± 0.26) × 10-3 | | - |
|---|
| K*(892)ντK-≥ 0 neutrals ντ | (3.2 ± 1.4) × 10-3 | | 542
<K*(892)ντ> |
|---|
| K*(892)ντK-≥ 0 neutrals ντ | (2.1 ± 0.4) × 10-3 | | 542
<K*(892)ντ> |
|---|
| K*(892)ντπ-≥ 0 neutrals ντ | (3.8 ± 1.7) × 10-3 | | 655
<K*(892)ντ> |
|---|
| K*(892)ντπ-≥ neutrals ντ | (2.2 ± 0.5) × 10-3 | | 655
<K*(892)ντ> |
|---|
| (K*(892)π-≥ π-Kντπν)π-≥ π-Kντπν | (1.0 ± 0.4) × 10-3 | | - |
|---|
| K₁(1270)-ντ | (4.7 ± 1.1) × 10-3 | | 447
<K₁(1270)-ντ> |
|---|
| K₁(1400)-ντ | (1.7 ± 2.6) × 10-3S=1.7
<K₁(1400)-ντ> | | 335
<K₁(1400)-ντ> |
|---|
| K*(1410)-ντ | (1.5 + 1.4 - 1.0) × 10-3 | | 326
<K*(1410)-ντ> |
|---|
| K*₀(1430)-ντ | <5 × 10⁻⁴ CL=95% | | 317
<K*₀(1430)-ντ> |
|---|
| K*₂(1430)-ντ | <3 × 10⁻³ CL=95% | | 315
<K*₂(1430)-ντ> |
|---|
ηπ-≥ν*_T
ηπ-π⁰ν*_T
[g] (1.39 ± 0.07) × 10⁻³ CL=95% | <9.9 × 10⁻⁵ CL=95% | | 797
<ηπ-π⁰ν*_T
ηπ-π⁰ν*_T [g]> |
|---|
+
+
+---PAGE_BREAK---
+
+
+
+
+ | ηπ-π0π0νT |
+ [g] (2.0 ± 0.4) × 10-4 |
+ 746 |
+
+
+ | ηK-νT |
+ [g] (1.55 ± 0.08) × 10-4 |
+ 719 |
+
+
+ | ηK*(892)-νT |
+ (1.38 ± 0.15) × 10-4 |
+ 511 |
+
+
+ | ηK-π0νT |
+ [g] (4.8 ± 1.2) × 10-5 |
+ 665 |
+
+
+ | ηK-π0(non-K*(892))νT |
+ < 3.5 × 10-5 CL=90% |
+ - |
+
+
+ | ηR0π-νT |
+ [g] (9.4 ± 1.5) × 10-5 |
+ 661 |
+
+
+ | ηR0π-π0νT |
+ < 5.0 × 10-5 CL=90% |
+ 590 |
+
+
+ | ηK-K0νT |
+ < 9.0 × 10-6 CL=90% |
+ 430 |
+
+
+ | ηπ+π-π- ≥ 0 neutrals νT |
+ < 3 × 10-3 CL=90% |
+ 744 |
+
+
+ | ηπ-π+π-νT(ex.K0) |
+ [g] (2.20 ± 0.13) × 10-4 |
+ 744 |
+
+
+ | ηπ-π+π-νT(ex.K0, f1(1285)) |
+ (9.9 ± 1.6) × 10-5 |
+ - |
+
+
+ | ηa1(1260)-νT → ηπ-ρ0νT |
+ < 3.9 × 10-4 CL=90% |
+ - |
+
+
+ | ηηπ-νT |
+ < 7.4 × 10-6 CL=90% |
+ 637 |
+
+
+ | ηηπ-π0νT |
+ < 2.0 × 10-4 CL=95% |
+ 559 |
+
+
+ | ηηK-νT |
+ < 3.0 × 10-6 CL=90% |
+ 382 |
+
+
+ | η'(958)π-νT |
+ < 4.0 × 10-6 CL=90% |
+ 620 |
+
+
+ | η'(958)π-π0νT |
+ < 1.2 × 10-5 CL=90% |
+ 591 |
+
+
+ | η'(958)K-νT |
+ < 2.4 × 10-6 CL=90% |
+ 495 |
+
+
+ | φπ-νT |
+ (3.4 ± 0.6) × 10-5 |
+ 585 |
+
+
+ | φK-νT |
+ [g] (4.4 ± 1.6) × 10-5 |
+ 445 |
+
+
+ | f1(1285)π-νT |
+ (3.9 ± 0.5) × 10-4S=1.9 |
+ 408 |
+
+
+ | f1(1285)π-νT → ηπ-π+π-νT |
+ (1.18 ± 0.07) × 10-4S=1.3 |
+ - |
+
+
+ | f1(1285)π-νT → 3π-2π+νT |
+ [g] (5.2 ± 0.4) × 10-5 |
+ - |
+
+
+ | π(1300)-νT → (ρπ)-νT → (3π)-νT |
+ < 1.0 × 10-4 CL=90% |
+ - |
+
+
+ | π(1300)-νT → ((ππ)S-wave π)-νT → (3π)-νT |
+ < 1.9 × 10-4 CL=90% |
+ - |
+
+
+ | h-ω ≥ 0 neutrals νT |
+ (2.40 ± 0.08) % |
+ 708 |
+
+
+ | h-ων̄ν̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄τ̄ τ̅ |
+ (1.99 ± 0.06) % [g] (1.95 ± 0.06) % [g] (4.1 ± 0.9) × 10-4
(4.1 ± 0.4) × 10-3
(1.4 ± 0.5) × 10-4
(7.2 ± 1.6) × 10-5
(5.4) × 10-7 |
+ (708)
(708)
(708)
(610)
(684)
(644)
(644)
CL=90% (250) |
+
+
+ h̅-ωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωωomega
h̅-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h-h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_h_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\_\\\\L means lepton number violation (e.g. τ⁻ → e⁺π⁻π⁻). Following
common usage, LF means lepton family violation and not lepton number
violation (e.g. τ⁻ → e⁻π⁺π⁻). B means baryon number violation.
+
+| e−γ | LF < 3.3 × 10−8 CL=90% | 888 |
|---|
| μ−γ | LF < 4.4 × 10−8 CL=90% | 885 |
|---|
| e−π0 | LF < 8.0 × 10−8 CL=90% | 883 |
|---|
| μ−π0 | LF < 1.1 × 10−7 CL=90% | 880 |
|---|
| e−KνS0 | LF < 2.6 × 10−8 CL=90% | 819 |
|---|
| μ−KνS0 | LF < 2.3 × 10−8 CL=90% | 815 |
|---|
| e−η | LF < 9.2 × 10−8 CL=90% | 804 |
|---|
| μ−η | LF < 6.5 × 10−8 CL=90% | 800 |
|---|
| e−ρ0 | LF < 1.8 × 10−8 CL=90% | 719 |
|---|
| μ−ρ0 | LF < 1.2 × 10−8 CL=90% | 715 |
|---|
+
+Lepton Family number (LF), Lepton number (L),
+or Baryon number (B) violating modes
+
+L means lepton number violation (e.g. τ⁻ → e⁺π⁻π⁻). Following
+common usage, LF means lepton family violation and not lepton number
+violation (e.g. τ⁻ → e⁻π⁺π⁻). B means baryon number violation.
+
+| e−γ | LF < 3.3 × 10−8 CL=90% | 888 |
|---|
| μ−γ | LF < 4.4 × 10−8 CL=90% | 885 |
|---|
| e−π0 | LF < 8.0 × 10−8 CL=90% | 883 |
|---|
| μ−π0 | LF < 1.1 × 10−7 CL=90% | 880 |
|---|
| e−KνS0 | LF < 2.6 × 10−8 CL=90% | 819 |
|---|
| μ−KνS0 | LF < 2.3 × 10−8 CL=90% | 815 |
|---|
| e−η | LF < 9.2 × 10−8 CL=90% | 804 |
|---|
| μ−η | LF < 6.5 × 10−8 CL=90% | 800 |
|---|
| e−ρ0 | LF < 1.8 × 10−8 CL=90% | 719 |
|---|
| μ−ρ0 | LF < 1.2 × 10−8 CL=90% | 715 |
|---|
+
+ηπ⁻π⁰π⁰νₜ
[g] (2.0 ± 0.4) × 10⁻⁴
CL=96% | 746
719
511
665
661
590
430
744
744
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-
-/
-
+
+$$ \begin{array}{l} \eta K^- \nu_T \\ \eta K^*(892)^-\nu_T \\ \eta K^- \pi^0 \nu_T \\ \eta K^- \pi^+ \pi^- \nu_T \\ \eta K^- \pi^+ \pi^- \pi^+ \nu_T \\ \eta K^- \pi^+ \pi^- \pi^+ \pi^- \nu_T \\ \eta a_{(1)}(1260)^-\nu_T \rightarrow \eta \pi^- \rho^{\bar{3}} \nu_T \\ \eta \eta \pi^- \nu_T \\ \eta \eta \pi^- \pi^{\bar{3}} \nu_T \\ \eta \eta K^- \nu_T \\ \eta' (958) \pi^- \nu_T \\ \eta' (958) \pi^- \pi^{\bar{3}} \nu_T \\ \eta' (958) K^- \nu_T \\ \phi \pi^- \nu_T \\ \phi K^- \nu_T \\ f_{(1)}(1285) \pi^- \nu_T \\ f_{(1)}(1285) \pi^- \nu_T \rightarrow \\ \qquad \eta \pi^- \pi^+ \pi^- \nu_T \\ f_{(1)}(1285) \pi^- \nu_T \rightarrow \\ f_{(3)}(3\pi)^-\nu_T \rightarrow (\rho\pi)^-\nu_T \\ f_{(3\pi)}(3\pi)^-\nu_T \\ f_{(3\pi)}(3\pi)^-\nu_T \\ ((\pi\pi)\textcolor{blue}{S-wave})\pi^- \nu_T \rightarrow \\ ((\pi\pi)\textcolor{red}{S-wave})\pi^- \nu_T \\ h^- \omega \geqslant 0 \text{ neutrals } \nu_T \\ h^- \omega\nu_T \\ h^- \omega\nu_T \\ \pi^- \omega\nu_T \\ K^- \omega\nu_T \\ h^- \omega\pi^{\bar{3}}\nu_T \\ h^- \omega2\pi^{\bar{3}}\nu_T \\ \pi^- \omega2\pi^{\bar{3}}\nu_T \\ h^-2\omega\nu_T \\ h^- h^+\omega\nu_T \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\ h^- h^+\omega\nu_T (ex.K^{\bar{3}}) \\h^{-}h^{+}\omega\overline{n}\nu_{T}^{+}(\textcolor{red}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{blue}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{green}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{magenta}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{orange}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{purple}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{yellow}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{cyan}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{magenta}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{orange}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{green}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{magenta}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{orange}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{magenta}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-Wave})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(\textcolor{teal}{S-WAVE})\overline{n}\nu_{T}^{+}(ex.\textit{kW}&b&b}&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&b&c)'
+
+$$
+\begin{array}{l}
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}] \\
+[\mathrm{s}]
+\end{array}
+$$
+---PAGE_BREAK---
+
+
+
+
+ | e- ω |
+ LF |
+ < 4.8 |
+ × 10-8 |
+ CL=90% |
+ 716 |
+
+
+ | μ- ω |
+ LF |
+ < 4.7 |
+ × 10-8 |
+ CL=90% |
+ 711 |
+
+
+ | e- K*(892)0 |
+ LF |
+ < 3.2 |
+ × 10-8 |
+ CL=90% |
+ 665 |
+
+
+ | μ- K*(892)0 |
+ LF |
+ < 5.9 |
+ × 10-8 |
+ CL=90% |
+ 659 |
+
+
+ | e- K̅*(892)0 |
+ LF |
+ < 3.4 |
+ × 10-8 |
+ CL=90% |
+ 665 |
+
+
+ | μ- K̅*(892)0 |
+ LF |
+ < 7.0 |
+ × 10-8 |
+ CL=90% |
+ 659 |
+
+
+ | e- η'(958) |
+ LF |
+ < 1.6 |
+ × 10-7 |
+ CL=90% |
+ 630 |
+
+
+ | μ- η'(958) |
+ LF |
+ < 1.3 |
+ × 10-7 |
+ CL=90% |
+ 625 |
+
+
+ | e- f0(980) → e-π+π- |
+ LF |
+ < 3.2 |
+ × 10-8 |
+ CL=90% |
+ - |
+
+
+ | μ- f0(980) → μ-π+π- |
+ LF |
+ < 3.4 |
+ × 10-8 |
+ CL=90% |
+ - |
+
+
+ | e- φ |
+ LF |
+ < 3.1 |
+ × 10-8 |
+ CL=90% |
+ 596 |
+
+
+ | μ- φ |
+ LF |
+ < 8.4 |
+ × 10-8 |
+ CL=90% |
+ 590 |
+
+
+ | e- e+e- |
+ LF |
+ < 2.7 |
+ × 10-8 |
+ CL=90% |
+ 888 |
+
+
+ | e- μ+μ- |
+ LF |
+ < 2.7 |
+ × 10-8 |
+ CL=90% |
+ 882 |
+
+
+ | e+μ--μ-- |
+ LF |
+ < 1.7 |
+ × 10-8 |
+ CL=90% |
+ 882 |
+
+
+ | μ-e+e- |
+ LF |
+ < 1.8 |
+ × 10-8 |
+ CL=90% |
+ 885 |
+
+
+ | μ+e-e- |
+ LF |
+ < 1.5 |
+ × 10-8 |
+ CL=90% |
+ 885 |
+
+
+ | μ--μ-+μ-- |
+ LF |
+ < 2.1 |
+ × 10-8 |
+ CL=90% |
+ 873 |
+
+
+ | e-π++π+- |
+ LF |
+ < 2.3 |
+ × 10-8 |
+ CL=90% |
+ 877 |
+
+
+ | e+π--π-- |
+ L |
+ < 2.0 |
+ × 10-8 |
+ CL=90% |
+ 877 |
+
+
+ μ--π++π+
-
-
(L) |
+ LF
μ+
-
-
π+
-
-
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K−
e+π-K̃———————————————————————————————————————————————————————————————————————————————————————————————&mdash- L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,B L,Bnbsp;B, m+, m- p, m- m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m- p, m+, m-&$^{3}$ CL=95% |
+
+
+
+
+
+ e⁻ω
+ LF
+ <
+ <
+ <
+ <
+ <
+ <
+ ×
+ ×
+ ×
+ ×
+ ×
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+ CL=90%
+
+
+
+
+---PAGE_BREAK---
+
+## Heavy Charged Lepton Searches
+
+### $L^{\pm}$ - charged lepton
+
+Mass $m > 100.8$ GeV, CL = 95% [h] Decay to $\nu W$.
+
+### $L^{\pm}$ - stable charged heavy lepton
+
+Mass $m > 102.6$ GeV, CL = 95%
+
+## Neutrino Properties
+
+See the note on "Neutrino properties listings" in the Particle Listings.
+
+- Mass $m < 1.1$ eV, CL = 90% (tritium decay)
+
+- Mean life/mass, $\tau/m > 300$ s/eV, CL = 90% (reactor)
+
+- Mean life/mass, $\tau/m > 7 \times 10^9$ s/eV (solar)
+
+- Mean life/mass, $\tau/m > 15.4$ s/eV, CL = 90% (accelerator)
+
+- Magnetic moment $\mu < 0.28 \times 10^{-10} \mu_B$, CL = 90% (solar + radiochemical)
+
+## Number of Neutrino Types
+
+Number $N = 2.996 \pm 0.007$ (Standard Model fits to LEP-SLC data)
+
+Number $N = 2.92 \pm 0.05$ ($S = 1.2$) (Direct measurement of invisible Z width)
+
+## Neutrino Mixing
+
+The following values are obtained through data analyses based on the 3-neutrino mixing scheme described in the review "Neutrino Masses, Mixing, and Oscillations."
+
+$$\sin^2(\theta_{12}) = 0.307 \pm 0.013$$
+
+$$\Delta m^2_{21} = (7.53 \pm 0.18) \times 10^{-5} \text{ eV}^2$$
+
+$$\sin^2(\theta_{23}) = 0.547 \pm 0.021 \text{ (Inverted order)}$$
+
+$$\sin^2(\theta_{23}) = 0.545 \pm 0.021 \text{ (Normal order)}$$
+
+$$\Delta m^2_{32} = (-2.546^{+0.034}_{-0.040}) \times 10^{-3} \text{ eV}^2 \text{ (Inverted order)}$$
+
+$$\Delta m^2_{32} = (2.453 \pm 0.034) \times 10^{-3} \text{ eV}^2 \text{ (Normal order)}$$
+
+$$\sin^2(\theta_{13}) = (2.18 \pm 0.07) \times 10^{-2}$$
+
+$\delta$, CP violating phase $= 1.36 \pm 0.17 \pi$ rad
+
+$$\langle \Delta m^2_{21} - \Delta m^2_{31} \rangle < 1.1 \times 10^{-4} \text{ eV}^2, \text{ CL} = 99.7\%$$
+
+$$\langle \Delta m^2_{32} - \Delta m^2_{31} \rangle = (-0.12 \pm 0.25) \times 10^{-3} \text{ eV}^2$$
+---PAGE_BREAK---
+
+NOTES
+
+In this Summary Table:
+
+When a quantity has "$(S = ...)$" to its right, the error on the quantity has been
+enlarged by the "scale factor" S, defined as $S = \sqrt{\chi^2/(N-1)}$, where N is the
+number of measurements used in calculating the quantity.
+
+A decay momentum p is given for each decay mode. For a 2-body decay, p is the momentum of each decay product in the rest frame of the decaying particle. For a 3-or-more-body decay, p is the largest momentum any of the products can have in this frame.
+
+[a] This is the best limit for the mode $e^{-} \rightarrow \nu\gamma$. The best limit for Nuclear de-excitation experiments is 6.4 $\times$ 10$^{24}$ yr.
+
+[b] See the review on "Muon Decay Parameters" for definitions and details.
+
+[c] $P_{\mu}$ is the longitudinal polarization of the muon from pion decay. For $\nu-A$ coupling, $P_{\mu} = 1$ and $\rho = \delta = 3/4$.
+
+[d] This only includes events with energy of $e > 45$ MeV and energy of $\gamma > 40$ MeV. Since the $e^{-}\bar{\nu}_{e}\nu_{\mu}$ and $e^{-}\bar{\nu}_{e}\nu_{\mu}\gamma$ modes cannot be clearly separated, we regard the latter mode as a subset of the former.
+
+[e] See the relevant Particle Listings in the Full *Review of Particle Physics* for the energy limits used in this measurement.
+
+[f] A test of additive vs. multiplicative lepton family number conservation.
+
+[g] Basis mode for the τ.
+
+[h] $L^{\pm}$ mass limit depends on decay assumptions; see the Full Listings.
+---PAGE_BREAK---
+
+## QUARKS
+
+The u-, d-, and s-quark masses are estimates of so-called "current-quark masses," in a mass-independent subtraction scheme such as $\overline{\text{MS}}$ at a scale $\mu \approx 2$ GeV. The c- and b-quark masses are the "running" masses in the $\overline{\text{MS}}$ scheme. This can be different from the heavy quark masses obtained in potential models.
+
+### u
+
+$$I(J^P) = \frac{1}{2}(\frac{1}{2}^+)$$
+
+$m_u = 2.16_{-0.26}^{+0.49} \text{ MeV}$ Charge = $\frac{2}{3}$ $e$ $I_z = +\frac{1}{2}$
+
+$m_u/m_d = 0.47_{-0.07}^{+0.06}$
+
+### d
+
+$$I(J^P) = \frac{1}{2}(\frac{1}{2}^+)$$
+
+$m_d = 4.67_{-0.17}^{+0.48} \text{ MeV}$ Charge = $-\frac{1}{3}$ $e$ $I_z = -\frac{1}{2}$
+
+$m_s/m_d = 17-22$
+
+$\bar{m} = (m_u+m_d)/2 = 3.45_{-0.15}^{+0.55} \text{ MeV}$
+
+### s
+
+$m_s = 93_{-5}^{+11} \text{ MeV}$ Charge = $-\frac{1}{3}$ $e$ Strangeness = $-1$
+
+$m_s / ((m_u + m_d)/2) = 27.3_{-1.3}^{+0.7}$
+
+### c
+
+$$I(J^P) = 0(\frac{1}{2}^+)$$
+
+$m_c = 1.27 \pm 0.02 \text{ GeV}$ Charge = $\frac{2}{3}$ $e$ Charm = +1
+
+$m_c/m_s = 11.72 \pm 0.25$
+
+$m_b/m_c = 4.577 \pm 0.008$
+
+$m_b-m_c = 3.45 \pm 0.05 \text{ GeV}$
+
+### b
+
+$$I(J^P) = 0(\frac{1}{2}^+)$$
+
+$m_b = 4.18_{-0.02}^{+0.03} \text{ GeV}$ Charge = $-\frac{1}{3}$ $e$ Bottom = $-1$
+
+### t
+
+$$I(J^P) = 0(\frac{1}{2}^+)$$
+
+Charge = $\frac{2}{3}$ $e$ Top = +1
+
+Mass (direct measurements) $m = 172.76 \pm 0.30 \text{ GeV}$ [a,b] ($S = 1.2$)
+
+Mass (from cross-section measurements) $m = 162.5_{-1.5}^{+2.1} \text{ GeV}$ [a]
+
+Mass (Pole from cross-section measurements) $m = 172.4 \pm 0.7 \text{ GeV}$
+
+$m_t - m_\tau = -0.16 \pm 0.19 \text{ GeV}$
+
+Full width $\Gamma = 1.42_{-0.15}^{+0.19} \text{ GeV}$ ($S = 1.4$)
+
+$\Gamma(Wb)/\Gamma(Wq(q=b, s, d)) = 0.957 \pm 0.034$ ($S = 1.5$)
+---PAGE_BREAK---
+
+t-quark EW Couplings
+
+$$F_0 = 0.687 \pm 0.018$$
+
+$$F_{-} = 0.320 \pm 0.013$$
+
+$$F_{+} = 0.002 \pm 0.011$$
+
+$F_{V+A} < 0.29$, CL = 95%
+
+| t DECAY MODES | Fraction (Γf/Γ) | Confidence level | p
(MeV/c) |
|---|
| Wq(q = b, s, d) | | | - | | Wb | | | - | | ενeb | (11.10±0.30) % | | - | | μνμb | (11.40±0.20) % | | - | | τντb | (11.1 ±0.9 ) % | | - | | qqb | (66.5 ±1.4 ) % | | - | | γq(q=u,c) | [c] < 1.8 | × 10-4 | 95% |
+
+ΔT = 1 weak neutral current (T1) modes
+
+| Zq(q=u,c) | T1 | [d] < 5 | × 10-4 | 95% | | Hu | T1 | < 1.2 | × 10-3 | 95% | | Hc | T1 | < 1.1 | × 10-3 | 95% | | ℓ+ qq'(q=d,s,b; q'=u,c) | T1 | < 1.6 | × 10-3 | 95% |
+
+b' (4th Generation) Quark, Searches for
+
+Mass $m > 190$ GeV, CL = 95% ($p\bar{p}$, quasi-stable $b'$)
+
+Mass $m > 1130$ GeV, CL = 95% ($B(b' \rightarrow Zb) = 1$)
+
+Mass $m > 1350$ GeV, CL = 95% ($B(b' \rightarrow Wt) = 1$)
+
+Mass $m > 46.0$ GeV, CL = 95% ($e^{+}e^{-}$, all decays)
+
+t' (4th Generation) Quark, Searches for
+
+$m(t'(2/3)) > 1280$ GeV, CL = 95% ($B(t' \rightarrow Zt) = 1$)
+
+$m(t'(2/3)) > 1295$ GeV, CL = 95% ($B(t' \rightarrow Wb) = 1$)
+
+$m(t'(2/3)) > 1310$ GeV, CL = 95% (singlet $t'$)
+
+$m(t'(5/3)) > 1350$ GeV, CL = 95%
+
+Free Quark Searches
+
+All searches since 1977 have had negative results.
+
+NOTES
+
+[a] A discussion of the definition of the top quark mass in these measurements can be found in the review "The Top Quark."
+
+[b] Based on published top mass measurements using data from Tevatron Run-I and Run-II and LHC at $\sqrt{s} = 7$ TeV. Including the most recent unpublished results from Tevatron Run-II, the Tevatron Electroweak Working Group reports a top mass of $173.2 \pm 0.9$ GeV. See the note "The Top Quark" in the Quark Particle Listings of this Review.
+
+[c] This limit is for $\Gamma(t \rightarrow \gamma q)/\Gamma(t \rightarrow Wb)$.
+
+[d] This limit is for $\Gamma(t \rightarrow Zq)/\Gamma(t \rightarrow Wb)$.
+---PAGE_BREAK---
+
+LIGHT UNFLAVORED MESONS
+(S = C = B = 0)
+
+For *l* = 1 (π, b, ρ, a): $u\bar{d}$, ($u\bar{u}-d\bar{d})/\sqrt{2}$, $d\bar{u}$;
+
+for *l* = 0 (η, η', h, h', ω, φ, f, f'): $c_1(u\bar{u} + d\bar{d}) + c_2(s\bar{s})$
+
+$$
+\pi^{\pm} \qquad I^{G}(JP) = 1^{-}(0^{-})
+$$
+
+Mass $m = 139.57039 \pm 0.00018$ MeV (S = 1.8)
+
+Mean life $\tau = (2.6033 \pm 0.0005) \times 10^{-8}$ s (S = 1.2)
+$c\tau = 7.8045$ m
+
+$\pi^{\pm} \rightarrow \ell^{\pm}\nu\gamma$ form factors [a]
+
+$F_V = 0.0254 \pm 0.0017$
+
+$F_A = 0.0119 \pm 0.0001$
+
+$F_V$ slope parameter $a = 0.10 \pm 0.06$
+
+$R = 0.059_{-0.008}^{+0.009}$
+
+$\pi^-$ modes are charge conjugates of the modes below.
+
+For decay limits to particles which are not established, see the section on
+Searches for Axions and Other Very Light Bosons.
+
+
+
+
+ | π+ DECAY MODES |
+ Fraction (Γf/Γ) |
+ Confidence level |
+ ρ
(MeV/c) |
+
+
+
+
+ | μ+νμ |
+ [b] (99.98770±0.00004) % |
+ |
+ 30 |
+
+
+ | μ+νμγ |
+ [c] (2.00 ±0.25) × 10-4 |
+ |
+ 30 |
+
+
+ | e+νe |
+ [b] (1.230 ±0.004) × 10-4 |
+ |
+ 70 |
+
+
+ | e+νeγ |
+ [c] (7.39 ±0.05) × 10-7 |
+ |
+ 70 |
+
+
+ | e+νeπ0 |
+ (1.036 ±0.006) × 10-8 |
+ |
+ 4 |
+
+
+ | e+νee+e- |
+ (3.2 ±0.5) × 10-9 |
+ |
+ 70 |
+
+
+ | e+νeν̅ |
+ < 5 |
+ × 10-6 |
+ 90% |
+
+
+
+
+Lepton Family number (LF) or Lepton number (L) violating modes
+
+
+
+ |
+ μ+ν̅e
+ |
+
+ L
+ |
+
+ [d] < 1.5
+ |
+
+ × 10-3
+ |
+
+ 90%
+ |
+
+
+ |
+ μ+ν̅e
+ |
+
+ LF
+ |
+
+ [d] < 8.0
+ |
+
+ × 10-3
+ |
+
+ 90%
+ |
+
+
+ |
+ μ-e+e+ν
+ |
+
+ LF
+ |
+
+ < 1.6
+ |
+
+ × 10-6
+ |
+
+ 90%
+ |
+
+
+
+$$
+\pi^0 \qquad I^G(JPC) = 1^{-}(0^{-})
+$$
+
+Mass $m = 134.9768 \pm 0.0005$ MeV (S = 1.1)
+
+$m_{\pi^{\pm}} - m_{\pi^{0}} = 4.5936 \pm 0.0005$ MeV
+
+Mean life $\tau = (8.52 \pm 0.18) \times 10^{-17}$ s (S = 1.2)
+$c\tau = 25.5$ nm
+
+For decay limits to particles which are not established, see the appropriate Search sections ($A^0$ (axion) and Other Light Boson ($X^0$) Searches, etc.).
+
+
+
+
+ |
+ π⁰ DECAY MODES
+ |
+
+ Fraction (Γᵢ/Γ)
+ |
+
+ Scale factor/ Confidence level
+ |
+
+ ρ (MeV/c)
+ |
+
+
+
+
+ |
+ 2γ
+ |
+
+ (98.823±0.034) %
+ |
+
+ S=1.5
+ |
+
+ 67
+ |
+
+
+ |
+ e⁺e⁻γ
+ |
+
+ (1.174±0.035) %
+ |
+
+ S=1.5
+ |
+
+ 67
+ |
+
+
+ |
+ γ positronium
+ |
+
+ (1.82 ±0.29 ) × 10⁻⁹
+ |
+
+ |
+
+ 67
+ |
+
+
+ |
+ e⁺e⁺e⁻e⁻
+ |
+
+ (3.34 ±0.16 ) × 10⁻⁵
+ |
+
+ |
+
+ 67
+ |
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | e+ e- |
+ ( 6.46 ±0.33 ) × 10-8 |
+ |
+ |
+
+
+ | 4γ |
+ < 2 |
+ × 10-8 |
+ CL=90% |
+
+
+ | ν∇e |
+ [e] < 2.7 |
+ × 10-7 |
+ CL=90% |
+
+
+ | νe∇ee |
+ < 1.7 |
+ × 10-6 |
+ CL=90% |
+
+
+ | νμ∇μ |
+ < 1.6 |
+ × 10-6 |
+ CL=90% |
+
+
+ | ντ∇τ |
+ < 2.1 |
+ × 10-6 |
+ CL=90% |
+
+
+ | γν∇ |
+ < 1.9 |
+ × 10-7 |
+ CL=90% |
+
+
+
+
+Charge conjugation (C) or Lepton Family number (LF) violating modes
+
+
+
+
+ | 3γ |
+ C |
+ < 3.1
+ × 10-8
+ CL=90%
+
+
+ | μ+ e- |
+ LF |
+ < 3.8
+ × 10-10
+ CL=90%
+
+
+ | μ- e+ |
+ LF |
+ < 3.4
+ × 10-9
+ CL=90%
+
+
+ | μ+ e- + μ- e+ |
+ LF |
+ < 3.6
+ × 10-10
+ CL=90%
+
+
+
+
+$$
+\eta \qquad I_G(J^{PC}) = 0^+(0^- +)
+$$
+
+Mass $m = 547.862 \pm 0.017$ MeV
+
+Full width $\Gamma = 1.31 \pm 0.05$ keV
+
+C-nonconserving decay parameters
+
+$\pi^+ \pi^- \pi^0$ left-right asymmetry = $(0.09_{-0.12}^{+0.11}) \times 10^{-2}$
+
+$\pi^+ \pi^- \pi^0$ sextant asymmetry = $(0.12_{-0.11}^{+0.10}) \times 10^{-2}$
+
+$\pi^+ \pi^- \pi^0$ quadrant asymmetry = $(-0.09 \pm 0.09) \times 10^{-2}$
+
+$\pi^+ \pi^- \gamma$ left-right asymmetry = $(0.9 \pm 0.4) \times 10^{-2}$
+
+$\pi^+ \pi^- \gamma$ $\beta$ (D-wave) = $-0.02 \pm 0.07$ ($S = 1.3$)
+
+CP-nonconserving decay parameters
+
+$\pi^+ \pi^- e^+ e^-$ decay-plane asymmetry $A_\phi = (-0.6 \pm 3.1) \times 10^{-2}$
+
+Other decay parameters
+
+$\pi^0 \pi^0 \pi^0$ Dalitz plot $\alpha = -0.0288 \pm 0.0012$ ($S = 1.1$)
+
+Parameter $\Lambda$ in $\eta \to \ell^+\ell^-\gamma$ decay = $0.716 \pm 0.011$ GeV/c²
+
+
+
+
+ |
+ η DECAY MODES
+ |
+
+ Fraction (Γ
+
+ η
+
+ /Γ)
+ |
+
+ Scale factor/
+ |
+
+
+ |
+ Confidence level
+ |
+
+ ρ (MeV/c)
+ |
+
+
+
+
+ |
+ Neutral modes
+ |
+
+
+ |
+ neutral modes
+ |
+
+ (72.12±0.34) %
+ |
+
+ S=1.2
+ |
+
+ —
+ |
+
+
+ |
+ 2γ
+ |
+
+ (39.41±0.20) %
+ |
+
+ S=1.1
+ |
+
+ 274
+ |
+
+
+ |
+ 3π
+
+ 0
+
+ |
+
+ (32.68±0.23) %
+ |
+
+ S=1.1
+ |
+
+ 179
+ |
+
+
+ |
+ π
+
+ 0
+
+ 2γ
+ |
+
+ ( 2.56±0.22 ) × 10
+
+ -4
+
+ |
+ |
+
+ 257
+ |
+
+
+ |
+ 2π
+
+ 0
+
+ 2γ
+ |
+
+ < 1.2
+ |
+
+ × 10
+
+ -3
+
+ |
+
+ CL=90%
+ |
+
+ 238
+ |
+
+
+ |
+ 4γ
+ |
+
+ < 2.8
+ |
+
+ × 10
+
+ -4
+
+ |
+
+ CL=90%
+ |
+
+ 274
+ |
+
+
+ |
+ invisible
+ |
+
+ < 1.0
+ |
+
+ × 10
+
+ -4
+
+ |
+
+ CL=90%
+ |
+
+ —
+ |
+
+
+
+ |
+ Charged modes
+ |
+
+
+
+ |
+ charged modes
+ |
+
+
+
+ |
+ π+ π- π0 (27.89±0.29) %
+ |
+
+
+
+ |
+ π+ π- γ (22.92±0.28) %
+ |
+
+
+
+ |
+ e+ e- γ (4.22±0.08) %
+ |
+
+
+
+ |
+ e+ e- γ (6.9 ±0.4 ) × 10-3 S=1.3
+ |
+
+
+
+ |
+ μ+ μ- γ (3.1 ±0.4 ) × 10-4 S=1.2
+ |
+
+
+
+ |
+ e+ e- γ < 7 × 10-7 CL=90%
+ |
+
+
+
+ |
+ μ+ μ- (5.8 ±0.8 ) × 10-6 S=1.2
+ |
+
+
+
+ |
+ 2e+2e- (2.40±0.22) × 10-5 S=1.2
+ |
+
+
+
+ |
+ π+ π- e+ e- (γ) (2.68±0.11) × 10-4 S=1.2
+ |
+
+
+
+ |
+ e+ e- μ+ μ- < 1.6 × 10-4 CL=90%
+ |
+
+
+
+ |
+ 2μ+2μ- < 3.6 × 10-4 CL=90%
+ |
+
+
+
+ |
+ μ+ μ- π+ π- < 3.6 × 10-4 CL=90%
+ |
+
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | π+e-νe + c.c. |
+ < 1.7 |
+ × 10-4 |
+ CL=90% |
+ 256 |
+
+
+ | π+π-2γ |
+ < 2.1 |
+ × 10-3 |
+ |
+ 236 |
+
+
+ | π+π-π0γ |
+ < 5 |
+ × 10-4 |
+ CL=90% |
+ 174 |
+
+
+ | π0μ+μ-γ |
+ < 3 |
+ × 10-6 |
+ CL=90% |
+ 210 |
+
+
+ Charge conjugation (C), Parity (P),
Charge conjugation × Parity (CP), or
Lepton Family number (LF) violating modes |
+
+
+ | π0γ |
+ C |
+ [f] < 9 |
+ × 10-5 |
+ CL=90% |
+ 257 |
+
+
+ | π+π- |
+ P,CP |
+ < 1.3 |
+ × 10-5 |
+ CL=90% |
+ 236 |
+
+
+ | 2π0 |
+ P,CP |
+ < 3.5 |
+ × 10-4 |
+ CL=90% |
+ 238 |
+
+
+ | 2π0γ |
+ C |
+ < 5 |
+ × 10-4 |
+ CL=90% |
+ 238 |
+
+
+ | 3π0γ |
+ C |
+ < 6 |
+ × 10-5 |
+ CL=90% |
+ 179 |
+
+
+ | 3γ |
+ C |
+ < 1.6 |
+ × 10-5 |
+ CL=90% |
+ 274 |
+
+
+ | 4π0 |
+ P,CP |
+ < 6.9 |
+ × 10-7 |
+ CL=90% |
+ 40 |
+
+
+ | π0e+e- |
+ C |
+ [g] < 8 |
+ × 10-6 |
+ CL=90% |
+ 257 |
+
+
+ | π0μ+μ- |
+ C |
+ [g] < 5 |
+ × 10-6 |
+ CL=90% |
+ 210 |
+
+
+ | μ+e-+ μ-e+ |
+ LF |
+ < 6 |
+ × 10-6 |
+ CL=90% |
+ 264 |
+
+
+
+
+$$
+f_0(500) \qquad I^G(J^{PC}) = 0^{+}(0^{++})
+$$
+
+also known as σ; was f₀(600)
+
+See the review on "Scalar Mesons below 2 GeV."
+
+Mass (T-Matrix Pole $\sqrt{s}$) = (400–550)–i(200–350) MeV
+
+Mass (Breit-Wigner) = (400–550) MeV
+
+Full width (Breit-Wigner) = (400–700) MeV
+
+$$
+\rho(770) \qquad I^G(J^{PC}) = 1^{+}(1^{-})
+$$
+
+See the note in ρ(770) Particle Listings.
+
+Mass *m* = 775.26 ± 0.25 MeV
+
+Full width Γ = 149.1 ± 0.8 MeV
+
+Γee = 7.04 ± 0.06 keV
+
+
+
+ | ρ(770) DECAY MODES | Fraction (Γf/Γ) | Scale factor/
Confidence level | p
(MeV/c) |
|---|
| ππ | ~ 100 | | 363 | | ρ(770)± decays |
|---|
| π±γ | ( 4.5 ±0.5 ) × 10-4 | S=2.2 | 375 |
|---|
| π±η | < 6 × 10-3 | CL=84% | 152 |
|---|
| π±π+π-π0 | < 2.0 × 10-3 | CL=84% | 254 |
|---|
| ρ(770)0 decays |
|---|
| π+π-γ | ( 9.9 ±1.6 ) × 10-3 | S=1.4 | 362 |
|---|
| π0γ | ( 4.7 ±0.6 ) × 10-4 | | 376 |
|---|
| ηγ | ( 3.00±0.21 ) × 10-4 | | 194 |
|---|
| π0π0γ | ( 4.5 ±0.8 ) × 10-5 | | 363 |
|---|
| μ+μ- | [h] ( 4.55±0.28 ) × 10-5 | | 373 |
|---|
| e+e- | [h] ( 4.72±0.05 ) × 10-5 | | 388 |
|---|
| π+π-π0 | ( 1.01+0.54-0.36±0.34 ) × 10-4 | | 323 |
|---|
| π+π-π+π- | ( 1.8 ±0.9 ) × 10-5 | | 251 |
|---|
| π+π-π0π0 | ( 1.6 ±0.8 ) × 10-5 | | 257 |
|---|
| π0e+e- | < 1.2 × 10-5 | CL=90% | 376 |
|---|
+
+
+---PAGE_BREAK---
+
+$$ \omega(782) \qquad I_G(J^{PC}) = 0^{-}(-^{-}) $$
+
+Mass $m = 782.65 \pm 0.12$ MeV (S = 1.9)
+
+Full width $\Gamma = 8.49 \pm 0.08$ MeV
+
+$\Gamma_{ee} = 0.60 \pm 0.02$ keV
+
+| ω(782) DECAY MODES | Fraction (Γf/Γ) | Scale factor/
Confidence level | p
(MeV/c) |
|---|
| π+π-π0 | (89.3 ± 0.6 ) % | | 327 | | π0γ | ( 8.40 ± 0.22 ) % | S=1.8 | 380 | | π+π- | ( 1.53 ± 0.06 ) % | | 366 | | neutrals (excluding π0 γ) | ( 7 +7-4 ) × 10-3 | S=1.1 | - | | ηγ | ( 4.5 ± 0.4 ) × 10-4 | S=1.1 | 200 | | π0e+e- | ( 7.7 ± 0.6 ) × 10-4 | | 380 | | π0μ+μ- | ( 1.34 ± 0.18 ) × 10-4 | S=1.5 | 349 | | e+e- | ( 7.36 ± 0.15 ) × 10-5 | S=1.5 | 391 | | π+π-π0 | < 2 | CL=90% | 262 | | π+π-γ | < 3.6 | CL=95% | 366 | | π+π-π+π- | < 1 | CL=90% | 256 | | π0π0γ | ( 6.7 ± 1.1 ) × 10-5 | | 367 | | ηπ0γ | < 3.3 | CL=90% | 162 | | μ+μ- | ( 7.4 ± 1.8 ) × 10-5 | | 377 | | 3γ | < 1.9 | CL=95% | 391 |
+
+Charge conjugation (C) violating modes
+
+| ηπ0 | C | < 2.2 | x 10-4 | CL=90% | 162 | | C | < 2.2 | x 10-4 | | 2π0 | C | < 2.2 | x 10-4 | CL=90% | 367 | | C | < 2.3 | x 10-4 | | 3π0 | C | < 2.3 | x 10-4 | CL=90% | 330 | | C | < 7 | x 10-5 |
| | invisible |
|---|
+
+$$ \eta'(958) \qquad I_G(J^{PC}) = 0^{+}(0^{-+}) $$
+
+Mass $m = 957.78 \pm 0.06$ MeV
+
+Full width $\Gamma = 0.188 \pm 0.006$ MeV
+
+
+
+
+ | η'(958) DECAY MODES |
+ Fraction (Γf/Γ) |
+ Confidence level |
+ p
(MeV/c) |
+
+
+
+
+ | π+π-η |
+ (42.5 ±0.5)% |
+ |
+ 232 |
+
+
+ ρ0γ(including non-resonant
π+π-γ) |
+ (29.5 ±0.4)% |
+ |
+ 165 |
+
+
+ | π0π0η |
+ (22.4 ±0.5)% |
+ |
+ 239 |
+
+
+ | ωγ |
+ (2.52 ±0.07)% |
+ |
+ 159 |
+
+
+ | ωe+e- |
+ (2.0 ±0.4)×10-4 |
+ |
+ 159 |
+
+
+ | γγ |
+ (2.307±0.033)% |
+ |
+ 479 |
+
+
+ | 3π0 |
+ (2.50 ±0.17)×10-3 |
+ |
+ 430 |
+
+
+ | μ+μ-γ |
+ (1.13 ±0.28)×10-4 |
+ 90% |
+ 467 |
+
+
+ | π+π-μ+μ- |
+ <2.9×10-5 |
+ 401 |
+
+
+ | π+π-π0 |
+ (3.61 ±0.17)×10-3 |
+ 428 |
+
+
+ | (π+π-π0) S-wave |
+ (3.8 ±0.5)×10-3 |
+ 90% |
+ 428 |
+
+
+ | π&mpart;ρ± ⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦⚦𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍𝕍ᶮ̅——-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-—-&mdash-√⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹⎹&#times; × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × × ×\end{array}
+$$
+---PAGE_BREAK---
+
+
+
+
+ | Meson Summary Table 31 |
+
+
+
+
+ | 2(π+π-)2π0 |
+ < 1 |
+ % |
+ 95% |
+ 197 |
+
+
+ | 3(π+π-) |
+ < 3.1 |
+ × 10-5 |
+ 90% |
+ 189 |
+
+
+ | K±π&mpm; |
+ < 4 |
+ × 10-5 |
+ 90% |
+ 334 |
+
+
+ | π+π-e+e- |
+ ( 2.4 ±1.3
−1.0 ) |
+ × 10-3 |
+ |
+ 458 |
+
+
+ | π+e-νe + c.c. |
+ < 2.1 |
+ × 10-4 |
+ 90% |
+ 469 |
+
+
+ | γe+e- |
+ ( 4.91 ±0.27 ) |
+ × 10-4 |
+ |
+ 479 |
+
+
+ | π0γγ |
+ ( 3.20 ±0.24 ) |
+ × 10-3 |
+ |
+ 469 |
+
+
+ | π0γγ(non resonant) |
+ ( 6.2 ±0.9 ) |
+ × 10-4 |
+ |
+ - |
+
+
+ | ηγγ |
+ < 1.33 |
+ × 10-4 |
+ 90% |
+ 322 |
+
+
+ | 4π0 |
+ < 3.2 |
+ × 10-4 |
+ 90% |
+ 380 |
+
+
+ | e+e- |
+ < 5.6 |
+ × 10-9 |
+ 90% |
+ 479 |
+
+
+ | invisible |
+ < 6 |
+ × 10-4 |
+ 90% |
+ - |
+
+
+Charge conjugation (C), Parity (P),
+Lepton family number (LF) violating modes
+
+ | P,CP | < 1.8 | × 10-5 | 90% | 458 |
|---|
| π+π- | P,CP | < 4 | × 10-4 | 90% | 459 |
|---|
| π0π0 | C [g] | < 1.4 | × 10-3 | 90% | 469 |
|---|
| ηγe+e- | C [g] | < 2.4 | × 10-3 | 90% | 322 |
|---|
| 3γ | C | < 1.0 | × 10-4 | 90% | 479 |
|---|
| μ+μ-π0 | C [g] | < 6.0 | × 10-5 | 90% | 445 |
|---|
| μ+μ-η | C [g] | < 1.5 | × 10-5 | 90% | 273 |
|---|
| eμ | LF | < 4.7 | × 10-4 | 90% | 473 |
|---|
+
+$$
+f_0(980) \qquad I^G(J^{PC}) = 0^{+}(0^{++})
+$$
+
+See the review on "Scalar Mesons below 2 GeV."
+Mass *m* = 990 ± 20 MeV
+Full width Γ = 10 to 100 MeV
+
+$$
+a_0(980) \qquad I^G(J^{PC}) = 1^{-}(0^{++})
+$$
+
+See the review on "Scalar Mesons below 2 GeV."
+Mass *m* = 980 ± 20 MeV
+Full width Γ = 50 to 100 MeV
+
+$$
+\phi(1020) \qquad I^G(J^{PC}) = 0^{-}(1^{--})
+$$
+
+Mass m = 1019.461 ± 0.016 MeV
+Full width Γ = 4.249 ± 0.013 MeV (S = 1.1)
+
+
+
+
+ |
+ $\phi(1020)$ DECAY MODES
+ |
+
+ Fraction ($\Gamma_f/\Gamma$)
+ |
+
+ Scale factor/ Confidence level
+ |
+
+ $\rho$ (MeV/c)
+ |
+
+
+
+
+ |
+ K+K-
+ |
+
+ (49.2 ±0.5 ) %
+ |
+
+ S=1.3
+ |
+
+ 127
+ |
+
+
+ |
+ KL0KS0
+ |
+
+ (34.0 ±0.4 ) %
+ |
+
+ S=1.3
+ |
+
+ 110
+ |
+
+
+ |
+ ρπ + π+π-πS0
+ |
+
+ (15.24 ±0.33 ) %
+ |
+
+ S=1.2
+ |
+
+ -
+ |
+
+
+ |
+ ηγ
+ |
+
+ ( 1.303±0.025 ) %
+ |
+
+ S=1.2
+ |
+
+ 363
+ |
+
+
+ |
+ πS0γ
+ |
+
+ ( 1.30 ±0.05 ) × 10-3
+ |
+
+
+ |
+ ℓ+ℓ-
+ |
+
+ -
+ |
+
+ 510
+ |
+
+
+ |
+ e+e-
+ |
+
+ ( 2.973±0.034) × 10-4 S=1.3
+ |
+
+ 510
+ |
+
+
+ |
+ μ+μ-
+ |
+
+ ( 2.86 ±0.19 ) × 10-4
+ |
+
+ 499
+ |
+
+
+ |
+ nνSe+e-
+ |
+
+ ( 1.08 ±0.04 ) × 10-4
+ |
+
+ 363
+ |
+
+
+ |
+ π+π-
+ |
+
+ ( 7.3 ±1.3 ) × 10-5
+ |
+
+ 490
+ |
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | ωπ0 |
+ ( 4.7 ±0.5 ) × 10-5 |
+ |
+ 172 |
+
+
+ | ωγ |
+ < 5 % |
+ CL=84% |
+ 209 |
+
+
+ | ργ |
+ < 1.2 × 10-5 |
+ CL=90% |
+ 215 |
+
+
+ | π+ π- γ |
+ ( 4.1 ±1.3 ) × 10-5 |
+ |
+ 490 |
+
+
+ | f0(980)γ |
+ ( 3.22 ±0.19 ) × 10-4 |
+ S=1.1 |
+ 29 |
+
+
+ | π0 π0 γ |
+ ( 1.12 ±0.06 ) × 10-4 |
+ |
+ 492 |
+
+
+ | π+ π- π+ π- |
+ ( 3.9 +2.8-2.2 ) × 10-6 |
+ |
+ 410 |
+
+
+ | π+ π+ π- π- π0 |
+ < 4.6 × 10-6 |
+ CL=90% |
+ 342 |
+
+
+ | π0 e+ e- |
+ ( 1.33 +0.07-0.10 ) × 10-5 |
+ |
+ 501 |
+
+
+ | π0 ηγ |
+ ( 7.27 ±0.30 ) × 10-5 |
+ S=1.5 |
+ 346 |
+
+
+ | a0(980)γ |
+ ( 7.6 ±0.6 ) × 10-5 |
+ |
+ 39 |
+
+
+ | K0/K0γ |
+ < 1.9 × 10-8 |
+ CL=90% |
+ 110 |
+
+
+ | η'(958)γ |
+ ( 6.22 ±0.21 ) × 10-5 |
+ |
+ 60 |
+
+
+ | ηπ0 π0 γ |
+ < 2 × 10-5 |
+ CL=90% |
+ 293 |
+
+
+ | μ+ μ- γ |
+ ( 1.4 ±0.5 ) × 10-5 |
+ |
+ 499 |
+
+
+ | ργγ |
+ < 1.2 × 10-4 |
+ CL=90% |
+ 215 |
+
+
+ | ηπ+ π- |
+ < 1.8 × 10-5 |
+ CL=90% |
+ 288 |
+
+
+ | ημ+ μ- |
+ < 9.4 × 10-6 |
+ CL=90% |
+ 321 |
+
+
+ | ηU → ηe+e- |
+ < 1 × 10-6 |
+ CL=90% |
+ - |
+
+
+ | invisible |
+ < 1.7 × 10-4 |
+ CL=90% |
+ - |
+
+
+ | Lepton Family number (LF) violating modes |
+
+
+ | e± μ&mpart; |
+ LF |
+ < 2 |
+ × 10-6 |
+ CL=90% |
+ 504 |
+
+
+
+
+$$
+h_1(1170) \qquad I_G(JPC) = 0^{--}(1^{+-})
+$$
+
+Mass *m* = 1166 ± 6 MeV
+
+Full width Γ = 375 ± 35 MeV
+
+$$
+b_1(1235) \qquad I_G(JPC) = 1^+(1^{-+})
+$$
+
+Mass $m = 1229.5 \pm 3.2$ MeV (S = 1.6)
+
+Full width $\Gamma = 142 \pm 9$ MeV (S = 1.2)
+
+
+
+
+
+ | bL(1235) DECAY MODES |
+
+ Fraction (ΓL/Γ) |
+
+ Confidence level (MeV/c)
p |
+
+
+
+
+
+
+ | pγ |
+
+ ( 1.6 ±0.4 ) × 10-3 |
+
+ |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+ Kπ
(K∇)±πS0 |
+
+ < 50 % |
+
+ |
+
+
+
+
+
+
+ | 4π | (32.7 ± 1.9) % | S=1.2 | 568 |
+
+
+
+ | π0 π0 π+ π- | (21.8 ± 1.3) % | S=1.2 | 566 |
+
+
+
+ | 2π+ 2π- | (10.9 ± 0.6) % | S=1.2 | 563 |
+
+
+
+ | ρ0 π+ π- | (10.9 ± 0.6) % | S=1.2 | 336 |
+
+
+
+ | 4π0 | < 7 × 10-4 | CL=90% | 568 |
+
+
+
+ | ηπ+ π- | (35 ± 15) % | | 479 |
+
+
+
+ | ηπππ | (52.2 ± 2.0) % | S=1.2 | 482 |
+
+
+
+ | a0(980)π [ignoring a0(980) → KK] | (38 ± 4) % | | 238 |
+
+
+
+ | ηπππ [excluding a0(980)ππ] | (14 ± 4) % | | 482 |
+
+
+
+ | KKπ | (9.0 ± 0.4) % | S=1.1 | 308 |
+
+
+
+ | π+ π- π0 | (3.0 ± 0.9) × 10-3 | | 603 |
+
+
+
+ | ρ± π∓ | < 3.1 × 10-3 | CL=95% | 390 |
+
+
+
+ | γρ0 | (6.1 ± 1.0) % | S=1.7 | 406 |
+
+
+
+ | φγ | (7.4 ± 2.6) × 10-4 | | 236 |
+
+
+
+ | e+ e- | < 9.4 × 10-9 | CL=90% | 641 |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+See Particle Listings for 2 decay modes that have been seen / not seen.
+
+**η(1295)**
+
+$$ I^G(J^{PC}) = \eta^+(0^{-+}) $$
+
+See the review on "Pseudoscalar and pseudovector mesons in the
+1400 MeV region."
+
+Mass *m* = **1294** ± **4** MeV (S = **1.6**)
+
+Full width Γ = **55** ± **5** MeV
+---PAGE_BREAK---
+
+### $\pi(1300)$
+
+$$ I_G(J^{PC}) = 1-(0^{-+}) $$
+
+Mass $m = 1300 \pm 100$ MeV [J]
+
+Full width $\Gamma = 200$ to $600$ MeV
+
+### $a_2(1320)$
+
+$$ I_G(J^{PC}) = 1-(2^{++}) $$
+
+Mass $m = 1316.9 \pm 0.9$ MeV (S = 1.9)
+
+Full width $\Gamma = 107 \pm 5$ MeV [J]
+
+| a2(1320) DECAY MODES | Fraction (Γj/Γ) | Scale factor/
Confidence level | p
(MeV/c) |
|---|
| 3π | (70.1 ±2.7)% | S=1.2 | 623 | | ηπ | (14.5 ±1.2)% | | 535 | | ωππ | (10.6 ±3.2)% | S=1.3 | 364 | | KK | (4.9 ±0.8)% | | 436 | | η'(958)π | (5.5 ±0.9) × 10-3 | | 287 | | π±γ | (2.91±0.27) × 10-3 | | 651 | | γγ | (9.4 ±0.7) × 10-6 | | 658 | | e+e- | < 5 × 10-9 | CL=90% | 658 |
+
+### $f_6(1370)$
+
+$$ I_G(J^{PC}) = 0+(0^{++}) $$
+
+See the review on "Scalar Mesons below 2 GeV."
+Mass $m = 1200$ to $1500$ MeV
+Full width $\Gamma = 200$ to $500$ MeV
+
+### $\pi_1(1400)$ [k]
+
+$$ I_G(J^{PC}) = 1-(1^{-+}) $$
+
+See the review on "Non-$q\bar{q}$ Mesons."
+Mass $m = 1354 \pm 25$ MeV (S = 1.8)
+Full width $\Gamma = 330 \pm 35$ MeV
+
+### $\eta(1405)$
+
+$$ I_G(J^{PC}) = 0+(0^{-+}) $$
+
+See the review on "Pseudoscalar and Pseudovector Mesons in the 1400 MeV Region."
+
+Mass $m = 1408.8 \pm 2.0$ MeV (S = 2.2)
+
+Full width $\Gamma = 50.1 \pm 2.6$ MeV (S = 1.7)
+
+| η(1405) DECAY MODES | Fraction (Γj/Γ) | Confidence level | p
(MeV/c) |
|---|
| ρρ | <58% | 99.85% | † |
+
+See Particle Listings for 9 decay modes that have been seen / not seen.
+
+### $h_1(1415)$
+
+$$ I_G(J^{PC}) = 0-(1^{+-}) $$
+
+was $h_1(1380)$
+
+Mass $m = 1416 \pm 8$ MeV (S = 1.5)
+
+Full width $\Gamma = 90 \pm 15$ MeV
+---PAGE_BREAK---
+
+$f_1(1420)$
+
+$$I^G(J^{PC}) = 0^{+}(1^{++})$$
+
+See the review on "Pseudoscalar and Pseudovector Mesons in the
+1400 MeV Region."
+
+Mass $m = 1426.3 \pm 0.9$ MeV (S = 1.1)
+
+Full width $\Gamma = 54.5 \pm 2.6$ MeV
+
+$\omega(1420)$ [J]
+
+$$I^G(J^{PC}) = 0^{--}(1^{--})$$
+
+Mass $m = 1410 \pm 60$ MeV [J]
+
+Full width $\Gamma = 290 \pm 190$ MeV [J]
+
+$a_0(1450)$
+
+$$I^G(J^{PC}) = 1^{--}(0^{++})$$
+
+See the review on "Scalar Mesons below 2 GeV."
+
+Mass $m = 1474 \pm 19$ MeV
+
+Full width $\Gamma = 265 \pm 13$ MeV
+
+
+
+
+ | a0(1450) DECAY MODES |
+ Fraction (Γf/Γ) |
+ ρ (MeV/c) |
+
+
+
+
+ | πη |
+ 0.093 ± 0.020 |
+ 627 |
+
+
+ | πη'(958) |
+ 0.033 ± 0.017 |
+ 410 |
+
+
+ | K&K |
+ 0.082 ± 0.028 |
+ 547 |
+
+
+ | ωππ |
+ |
+ 484 |
+
+
+
+
+**DEFINED AS 1**
+
+See Particle Listings for 2 decay modes that have been seen / not seen.
+
+$\rho(1450)$
+
+$$I^G(J^{PC}) = 1^{+}(1^{-^{-}})$$
+
+See the note in $\rho(1450)$ Particle Listings.
+
+Mass $m = 1465 \pm 25$ MeV [J]
+
+Full width $\Gamma = 400 \pm 60$ MeV [J]
+
+$\eta(1475)$
+
+$$I^G(J^{PC}) = 0^{+}(0^{-+})$$
+
+See the review on "Pseudoscalar and Pseudovector Mesons in the
+1400 MeV Region."
+
+Mass $m = 1475 \pm 4$ MeV (S = 1.4)
+
+Full width $\Gamma = 90 \pm 9$ MeV (S = 1.6)
+
+$f_0(1500)$
+
+$$I^G(J^{PC}) = 0^{+}(0^{++})$$
+
+See the reviews on "Scalar Mesons below 2 GeV" and on "Non-$q\bar{q}$ Mesons".
+
+Mass $m = 1506 \pm 6$ MeV (S = 1.4)
+
+Full width $\Gamma = 112 \pm 9$ MeV
+
+
+
+
+| f0(1500) DECAY MODES |
+Fraction (Γf/Γ) |
+Scale factor |
+p
(MeV/c) |
+
+
+
+
+| ππ |
+(34.5 ± 2.2) % |
+1.2 |
+741 |
+
+
+| 4π |
+(48.9 ± 3.3) % |
+1.2 |
+692 |
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | ηη |
+ ( 6.0±0.9) % |
+ 1.1 |
+ 517 |
+
+
+ | ηη'(958) |
+ ( 2.2±0.8) % |
+ 1.4 |
+ 20 |
+
+
+ | KK |
+ ( 8.5±1.0) % |
+ 1.1 |
+ 569 |
+
+
+
+
+See Particle Listings for 9 decay modes that have been seen / not seen.
+
+$f_2'(1525)$
+
+$I_G(JPC) = 0^+(2^+)$
+
+Mass $m = 1517.4 \pm 2.5$ MeV (S = 2.8)
+
+Full width $\Gamma = 86 \pm 5$ MeV (S = 2.2)
+
+
+
+
+ | f'2(1525) DECAY MODES |
+ Fraction (Γj/Γ) |
+ Scale factor |
+ p
(MeV/c) |
+
+
+
+
+ | KK |
+ (87.6±2.2) % |
+ 1.1 |
+ 576 |
+
+
+ | ηη |
+ (11.6±2.2) % |
+ 1.1 |
+ 525 |
+
+
+ | ππ |
+ ( 8.3±1.6) × 10-3 |
+ |
+ 747 |
+
+
+ | γγ |
+ ( 9.5±1.1) × 10-7 |
+ 1.1 |
+ 759 |
+
+
+
+
+$\pi_1(1600)$
+
+$I_G(JPC) = 1^-(1^-)$
+
+See the review on "Non-$q\bar{q}$ Mesons" and a note in PDG 06, Journal of Physics G33 1 (2006).
+
+Mass $m = 1660 \pm 15_{-11}^{+15}$ MeV (S = 1.2)
+
+Full width $\Gamma = 257 \pm 60$ MeV (S = 1.9)
+
+$a_1(1640)$
+
+$I_G(JPC) = 1^-(1^+)$
+
+Mass $m = 1655 \pm 16$ MeV (S = 1.2)
+
+Full width $\Gamma = 254 \pm 40$ MeV (S = 1.8)
+
+$\eta_2(1645)$
+
+$I_G(JPC) = 0^+(2^-)$
+
+Mass $m = 1617 \pm 5$ MeV
+
+Full width $\Gamma = 181 \pm 11$ MeV
+
+$\omega(1650)^{[\eta]}$
+
+$I_G(JPC) = 0^-(1^{--})$
+
+Mass $m = 1670 \pm 30$ MeV [J]
+
+Full width $\Gamma = 315 \pm 35$ MeV [J]
+
+$\omega_3(1670)$
+
+$I_G(JPC) = 0^-(3^{--})$
+
+Mass $m = 1667 \pm 4$ MeV
+
+Full width $\Gamma = 168 \pm 10$ MeV
+
+$\pi_2(1670)$
+
+$I_G(JPC) = 1^-(2^-)$
+
+Mass $m = 1670.6 \pm _{1.2}^{+2.9}$ MeV (S = 1.3)
+
+Full width $\Gamma = 258 \pm _9^{+8}$ MeV (S = 1.2)
+---PAGE_BREAK---
+
+
+ π2(1670) DECAY MODES
+
+
+ |
+ Fraction (Γf/Γ) |
+ Confidence level |
+ ρ
(MeV/c) |
+
+
+
+
+ | 3π |
+ (95.8±1.4) % |
+ |
+ 808 |
+
+
+ | f2(1270)π |
+ (56.3±3.2) % |
+ |
+ 327 |
+
+
+ | ρπ |
+ (31 ±4) % |
+ |
+ 647 |
+
+
+ | σπ |
+ (10 ±4) % |
+ |
+ - |
+
+
+ | π(ππ)S-wave |
+ (8.7±3.4) % |
+ |
+ - |
+
+
+ | π±π±π- |
+ (53 ±4) % |
+ |
+ 806 |
+
+
+ | K±K*(892) + c.c. |
+ (4.2±1.4) % |
+ |
+ 453 |
+
+
+ | ωρ |
+ (2.7±1.1) % |
+ |
+ 302 |
+
+
+ | π±γ |
+ (7.0±1.2) × 10-4 |
+ |
+ 829 |
+
+
+ | γγ |
+ < 2.8 × 10-7 |
+ 90% |
+ 835 |
+
+
+ | ηπ |
+ < 5 % |
+ |
+ 739 |
+
+
+ | π±2π+2π- |
+ < 5 % |
+ |
+ 735 |
+
+
+ | ρ(1450)π |
+ < 3.6 × 10-3 |
+ 97.7% |
+ 145 |
+
+
+ | b1(1235)π |
+ < 1.9 × 10-3 |
+ 97.7% |
+ 364 |
+
+
+
+
+See Particle Listings for 2 decay modes that have been seen / not seen.
+
+$$
+\phi(1680)
+$$
+
+$$
+I^G(J^{PC}) = 0^{--}
+$$
+
+Mass $m = 1680 \pm 20$ MeV [J]
+
+Full width $\Gamma = 150 \pm 50$ MeV [J]
+
+$$
+\rho_3(1690)
+$$
+
+$$
+I^G(J^{PC}) = 1^{++}(-3-)
+$$
+
+Mass $m = 1688.8 \pm 2.1$ MeV
+
+Full width $\Gamma = 161 \pm 10$ MeV ($S = 1.5$)
+
+
+ ρ3(1690) DECAY MODES
+
+
+ |
+ Fraction (Γf/Γ) |
+ Scale factor |
+ ρ
(MeV/c) |
+
+
+
+
+ | 4π |
+ (71.1 ± 1.9)% |
+ |
+ 790 |
+
+
+ | π±π+π-π0 |
+ (67 ± 22)% |
+ |
+ 787 |
+
+
+ | ωπ |
+ (16 ± 6)% |
+ |
+ 655 |
+
+
+ | ππ |
+ (23.6 ± 1.3)% |
+ |
+ 834 |
+
+
+ | K&K/π |
+ ( 3.8 ± 1.2)% |
+ |
+ 629 |
+
+
+ | KK/κ |
+ ( (1.58 ± 0.26)% ) |
+ 1.2 |
+ 685 |
+
+
+
+
+See Particle Listings for 5 decay modes that have been seen / not seen.
+
+$$
+\rho(1700) \qquad I^G(J^{PC}) = 1^{+-}(-1-)
+$$
+
+See the note in ρ(1700) Particle Listings.
+
+Mass $m = 1720 \pm 20$ MeV [J] ($\eta\rho^0$ and $\pi^+\pi^-$ modes)
+
+Full width $\Gamma = 250 \pm 100$ MeV [$\overline{J}$] ($\eta\rho^0$ and $\pi^+\pi^-$ modes)
+
+$$
+a_2(1700) \qquad I^G(J^{PC}) = 1^{-(2++)}
+$$
+
+Mass $m = 1705 \pm 40$ MeV
+
+Full width $\Gamma = 258 \pm 40$ MeV
+
+a2(1700) DECAY MODES | Fraction (Γf/Γ) | p (MeV/c) |
|---|
| ηπ | (3.7 ±1.0 ) % | 758 |
|---|
| γγ̅ | (1.16±0.27) × 10-6 | 852 |
|---|
| KK | (1.9 ±1.2 ) % | 695 |
|---|
+---PAGE_BREAK---
+
+**f₀(1710)**
+
+$$I^G(J^{PC}) = 0^{+}(0^{++})$$
+
+See the review on "Non-$q\bar{q}$ Mesons."
+Mass $m = 1704 \pm 12$ MeV
+Full width $\Gamma = 123 \pm 18$ MeV
+
+**π(1800)**
+
+$$I^G(J^{PC}) = 1^{-(0^{-+})}$$
+
+Mass $m = 1810_{-11}^{+9}$ MeV (S = 2.2)
+Full width $\Gamma = 215_{-8}^{+7}$ MeV
+
+**φ₃(1850)**
+
+$$I^G(J^{PC}) = 0^{--}(3^{--})$$
+
+Mass $m = 1854 \pm 7$ MeV
+Full width $\Gamma = 87_{-23}^{+28}$ MeV (S = 1.2)
+
+**η₂(1870)**
+
+$$I^G(J^{PC}) = 0^{+}(2^{-+})$$
+
+Mass $m = 1842 \pm 8$ MeV
+Full width $\Gamma = 225 \pm 14$ MeV
+
+**π₂(1880)**
+
+$$I^G(J^{PC}) = 1^{-(2^{-+})}$$
+
+Mass $m = 1874_{-5}^{+26}$ MeV (S = 1.6)
+Full width $\Gamma = 237_{-30}^{+33}$ MeV (S = 1.2)
+
+**f₂(1950)**
+
+$$I^G(J^{PC}) = 0^{+}(2^{++})$$
+
+Mass $m = 1936 \pm 12$ MeV (S = 1.3)
+Full width $\Gamma = 464 \pm 24$ MeV
+
+**a₄(1970)**
+
+$$I^G(J^{PC}) = 1^{-(4^{++})}$$
+
+was a₄(2040)
+Mass $m = 1967 \pm 16$ MeV (S = 2.1)
+Full width $\Gamma = 324_{-18}^{+15}$ MeV
+
+**f₂(2010)**
+
+$$I^G(J^{PC}) = 0^{+}(2^{++})$$
+
+Mass $m = 2011_{-80}^{+60}$ MeV
+Full width $\Gamma = 202 \pm 60$ MeV
+---PAGE_BREAK---
+
+$f_4(2050)$
+
+$$ I^G(J^{PC}) = 0^{+}(4^{++}) $$
+
+Mass $m = 2018 \pm 11$ MeV (S = 2.1)
+
+Full width $\Gamma = 237 \pm 18$ MeV (S = 1.9)
+
+
+
+
+| $f_4(2050)$ DECAY MODES |
+Fraction ($\Gamma_I/\Gamma$) |
+p (MeV/c) |
+
+
+
+
+| $\pi\pi$ |
+(17.0±1.5) % |
+1000 |
+
+
+| $K\overline{K}$ |
+(6.8+3.4-1.8 × 10-3) |
+880 |
+
+
+| $\eta\eta$ |
+(2.1±0.8) × 10-3 |
+848 |
+
+
+| $4\pi^0$ |
+< 1.2 % |
+964 |
+
+
+
+
+See Particle Listings for 2 decay modes that have been seen / not seen.
+
+$\phi(2170)$
+
+$$ I^G(J^{PC}) = 0^{-}(1^{--}) $$
+
+Mass $m = 2160 \pm 80$ MeV [J]
+
+Full width $\Gamma = 125 \pm 65$ MeV [J]
+
+$f_2(2300)$
+
+$$ I^G(J^{PC}) = 0^{+}(2^{++}) $$
+
+Mass $m = 2297 \pm 28$ MeV
+
+Full width $\Gamma = 149 \pm 40$ MeV
+
+$f_2(2340)$
+
+$$ I^G(J^{PC}) = 0^{+}(2^{++}) $$
+
+Mass $m = 2345_{-40}^{+50}$ MeV
+
+Full width $\Gamma = 322_{-60}^{+70}$ MeV
+
+STRANGE MESONS
+($S = \pm 1$, $C = B = 0$)
+
+$K^+ = u\bar{s}, K^0 = d\bar{s}, \bar{K}^0 = \bar{d}s, K^- = \bar{u}s, \text{ similarly for } K^*'$s
+
+$K^\pm$
+
+$$ I(J^P) = \frac{1}{2}(0^{-}) $$
+
+Mass $m = 493.677 \pm 0.016$ MeV [o] (S = 2.8)
+
+Mean life $\tau = (1.2380 \pm 0.0020) \times 10^{-8}$ s (S = 1.8)
+
+$c\tau = 3.711$ m
+
+CPT violation parameters ($\Delta$ = rate difference/sum)
+
+$\Delta(K^\pm \to \mu^\pm\nu_\mu) = (-0.27 \pm 0.21)\%$
+
+$\Delta(K^\pm \to \pi^\pm\pi^0) = (0.4 \pm 0.6)\%$ [p]
+
+CP violation parameters ($\Delta$ = rate difference/sum)
+
+$\Delta(K^\pm \to \pi^\pm e^+e^-) = (-2.2 \pm 1.6) \times 10^{-2}$
+
+$\Delta(K^\pm \to \pi^\pm\mu^+\mu^-) = 0.010 \pm 0.023$
+
+$\Delta(K^\pm \to \pi^\pm\pi^0\gamma) = (0.0 \pm 1.2) \times 10^{-3}$
+
+$\Delta(K^\pm \to \pi^\pm\pi^+\pi^-) = (0.04 \pm 0.06)\%$
+
+$\Delta(K^\pm \to \pi^\pm\pi^0\pi^0) = (-0.02 \pm 0.28)\%$
+---PAGE_BREAK---
+
+### T violation parameters
+
+$$K^+ \to \pi^0 \mu^+ \nu_\mu \quad P_T = (-1.7 \pm 2.5) \times 10^{-3}$$
+
+$$K^+ \to \mu^+ \nu_\mu \gamma \quad P_T = (-0.6 \pm 1.9) \times 10^{-2}$$
+
+$$K^+ \to \pi^0 \mu^+ \nu_\mu \quad \text{Im}(\xi) = -0.006 \pm 0.008$$
+
+### Slope parameter g [q]
+
+(See Particle Listings for quadratic coefficients and alternative parametrization related to $\pi\pi$ scattering)
+
+$$K^{\pm} \to \pi^{\pm} \pi^{+} \pi^{-} g = -0.21134 \pm 0.00017$$
+
+$$ (g_+ - g_-) / (g_+ + g_-) = (-1.5 \pm 2.2) \times 10^{-4} $$
+
+$$K^{\pm} \to \pi^{\pm} \pi^{0} \pi^{0} g = 0.626 \pm 0.007$$
+
+$$ (g_{+} - g_{-}) / (g_{+} + g_{-}) = (1.8 \pm 1.8) \times 10^{-4} $$
+
+### K± decay form factors [a,r]
+
+Assuming $\mu$-$e$ universality
+
+$$\lambda_+(K_{\mu3}^+) = \lambda_+(K_{e3}^+) = (2.959 \pm 0.025) \times 10^{-2}$$
+
+$$\lambda_0(K_{\mu3}^+) = (1.76 \pm 0.25) \times 10^{-2} \quad (\text{S} = 2.7)$$
+
+Not assuming $\mu$-$e$ universality
+
+$$\lambda_+(K_{e3}^+) = (2.956 \pm 0.025) \times 10^{-2}$$
+
+$$\lambda_+(K_{\mu3}^+) = (3.09 \pm 0.25) \times 10^{-2} \quad (\text{S} = 1.5)$$
+
+$$\lambda_0(K_{\mu3}^+) = (1.73 \pm 0.27) \times 10^{-2} \quad (\text{S} = 2.6)$$
+
+$K_{e3}$ form factor quadratic fit
+
+$$\lambda'_+(\mathcal{K}_{e3}^\pm) \text{ linear coeff.} = (2.59 \pm 0.04) \times 10^{-2}$$
+
+$$\lambda''_+(\mathcal{K}_{e3}^\pm) \text{ quadratic coeff.} = (0.186 \pm 0.021) \times 10^{-2}$$
+
+$\lambda'_+$ (LINEAR $K_{\mu3}^\pm$ FORM FACTOR FROM QUADRATIC FIT) =$ (24 \pm 4) \times 10^{-3}$
+
+$\lambda''_+$ (QUADRATIC $K_{\mu3}^\pm$ FORM FACTOR) = $(1.8 \pm 1.5) \times 10^{-3}$
+
+$M_V$ (VECTOR POLE MASS FOR $K_{e3}^\pm$ DECAY) = $890.3 \pm 2.8$ MeV
+
+$M_V$ (VECTOR POLE MASS FOR $K_{\mu3}^\pm$ DECAY) = $878 \pm 12$ MeV
+
+$M_S$ (SCALAR POLE MASS FOR $K_{\mu3}^\pm$ DECAY) = $1215 \pm 50$ MeV
+
+$\Lambda_+$ (DISPERSIVE VECTOR FORM FACTOR IN $K_{e3}^\pm$ DECAY) = $(2.460 \pm 0.017) \times 10^{-2}$
+
+$\Lambda_+$ (DISPERSIVE VECTOR FORM FACTOR IN $K_{\mu3}^\pm$ DECAY) = $(25.4 \pm 0.9) \times 10^{-3}$
+
+$\ln(C)$ (DISPERSIVE SCALAR FORM FACTOR in $K_{\mu3}^\pm$ decays) = $(182 \pm 16) \times 10^{-3}$
+
+$$K_{e3}^{+} |f_S/f_{+}| = (-0.08^{+0.34}_{-0.40}) \times 10^{-2}$$
+
+$$K_{e3}^{+} |f_T/f_{+}| = (-1.2^{+1.3}_{-1.1}) \times 10^{-2}$$
+
+$$K_{\mu3}^{+} |f_S/f_{+}| = (0.2 \pm 0.6) \times 10^{-2}$$
+
+$$K_{\mu3}^{+} |f_T/f_{+}| = (-0.1 \pm 0.7) \times 10^{-2}$$
+
+$$K^+ \to e^+ \nu_e \gamma \quad |F_A + F_V| = 0.133 \pm 0.008 \quad (\text{S} = 1.3)$$
+
+$$K^+ \to \mu^+ \nu_\mu \gamma \quad |F_A + F_V| = 0.165 \pm 0.013$$
+
+$$K^+ \to e^+ \nu_e \gamma \quad |F_A - F_V| < 0.49, \text{ CL } = 90\%$$
+
+$$K^+ \to \mu^+ \nu_\mu \gamma \quad |F_A - F_V| = -0.153 \pm 0.033 \quad (\text{S} = 1.1)$$
+---PAGE_BREAK---
+
+**Charge radius**
+
+$$ \langle r \rangle = 0.560 \pm 0.031 \text{ fm} $$
+
+**Forward-backward asymmetry**
+
+$$ A_{FB}(K_{\pi\mu\mu}^{\pm}) = \frac{\Gamma(\cos(\theta_{K\mu})>0)-\Gamma(\cos(\theta_{K\mu})<0)}{\Gamma(\cos(\theta_{K\mu})>0)+\Gamma(\cos(\theta_{K\mu})<0)} < 2.3 \times 10^{-2}, \text{ CL} = 90\% $$
+
+$K^-$ modes are charge conjugates of the modes below.
+
+| Κ+ DECAY MODES | Fraction (Γf/Γ) | Scale factor/ ρ
Confidence level (MeV/c) |
|---|
| Leptonic and semileptonic modes | | e+ νe | ( 1.582±0.007 ) × 10-5 | 247 | | μ+ νμ | ( 63.56 ±0.11 ) % | S=1.2 236 | | π0 e+ νe | ( 5.07 ±0.04 ) % | S=2.1 228 | | Called Ke3+ | | | | π0 μ+ νμ | ( 3.352±0.033 ) % | S=1.9 215 | | Called Kμ3+ | | | | π0 π0 e+ νe | ( 2.55 ±0.04 ) × 10-5 | S=1.1 206 | | π+ π- e+ νe | ( 4.247±0.024 ) × 10-5 | 203 | | π+ π- μ+ νμ | ( 1.4 ±0.9 ) × 10-5 | 151 | | π0 π0 π0 e+ νe | < 3.5 × 10-6 | CL=90% 135 | | Hadronic modes | | π+ π0 | ( 20.67 ±0.08 ) % | S=1.2 205 | | π+ π0 π0 | ( 1.760±0.023 ) % | S=1.1 133 | | π+ π+ π- | ( 5.583±0.024 ) % | 125 | | Leptonic and semileptonic modes with photons | | μ+ νμ γ | [s,t] ( 6.2 ±0.8 ) × 10-3 | 236 | | μ+ νμ γ(SD+) | [a,u] ( 1.33 ±0.22 ) × 10-5 | - | | μ+ νμ γ(SD+INT) | [a,u] < 2.7 × 10-5 | CL=90% - | | μ+ νμ γ(SD- + SD-INT) | [a,u] < 2.6 × 10-4 | CL=90% - | | e+ νe γ | ( 9.4 ±0.4 ) × 10-6 | 247 | | π0 e+ νe γ | [s,t] ( 2.56 ±0.16 ) × 10-4 | 228 | | π0 e+ νe γ(SD) | [a,u] < 5.3 × 10-5 | CL=90% 228 | | π0 μ+ νμ γ | [s,t] ( 1.25 ±0.25 ) × 10-5 | 215 | | π0 π0 e+ νe γ | < 5 × 10-6 | CL=90% 206 | | Hadronic modes with photons or ℓℓ pairs | | π+ π0 γ(INT) | (-4.2 ±0.9) × 10-6 | - | | π+ π0 γ(DE) | [s,v] ( 6.0 ±0.4 ) × 10-6 | 205 | | π+ π0e-e- | ( 4.24 ±0.14 ) × 10-6 | 205 | | [s,t] ( 7.6 +6.0
-3.0 ) × 10-6 | | π+ π0π0γ | [s,t] ( 7.1 ±0.5 ) × 10-6 | 133 | | [s] ( 1.01 ±0.06 ) × 10-6 | | π+γγ | [s] < 1.0 × 10-4 | CL=90% | | π+3γ | ( 1.19 ±0.13 ) × 10-8 | | Leptonic modes with ℓℓ pairs | | e+νeνν | < 6 × 10-5 | CL=90% | | μ+ννν | < 2.4 × 10-6 | | e+ννee+e-e- | ( 2.48 ±0.20 ) × 10-8 | 247 | | μ+νννe+e-e- | ( 7.06 ±0.31 ) × 10-8 | e+ννeμ+μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-μ-\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\\
+\end{aligned}
+$$
+---PAGE_BREAK---
+
+Lepton family number (LF), Lepton number (L), $\Delta S = \Delta Q$ (SQ)
+violating modes, or $\Delta S = 1$ weak neutral current (S1) modes
+
+| π+ π+ e-νe | SQ | < 1.3 | × 10-8 | CL=90% | 203 | | π+ π+ μ-νμ | SQ | < 3.0 | × 10-6 | CL=95% | 151 | | π+ e+e- | S1 | ( 3.00 ±0.09 ) | × 10-7 | | 227 | | π+ μ+μ- | S1 | ( 9.4 ±0.6 ) | × 10-8 | S=2.6 | 172 | | π+ νν̄ | S1 | ( 1.7 ±1.1 ) | × 10-10 | | 227 | | π+ π0νν̄ | S1 | < 4.3 | × 10-5 | CL=90% | 205 | | μ- νe+e+ | LF | < 2.1 | × 10-8 | CL=90% | 236 | | μ+ νe | LF [d] < 4 | | × 10-3 | CL=90% | 236 | | π+ μ+e- | LF | < 1.3 | × 10-11 | CL=90% | 214 | | π+ μ-e+ | LF | < 5.2 | × 10-10 | CL=90% | 214 | | π- μ+e+ | L | < 5.0 | × 10-10 | CL=90% | 214 | | π- e+e+ | L | < 2.2 | × 10-10 | CL=90% | 227 | | π- μ+μ+ | L | < 4.2 | × 10-11 | CL=90% | 172 | | μ+ν̄e | L [d] < 3.3 | | × 10-3 | CL=90% | 236 | | π0e+ēe | L [x] < 3 | | × 10-3 | CL=90% | 228 | | π+ γ̄ | [x] < 2.3 | | × 10-9 | CL=90% | 227 |
+
+$$I(J^P) = \frac{1}{2}(0^-)$$
+
+50% $K_S$, 50% $K_L$
+
+$$\text{Mass } m = 497.611 \pm 0.013 \text{ MeV} \quad (\text{S} = 1.2)$$
+
+$$m_{K^0} - m_{\bar{K}^0} = 3.934 \pm 0.020 \text{ MeV} \quad (\text{S} = 1.6)$$
+
+Mean square charge radius
+
+$$\langle r^2 \rangle = -0.077 \pm 0.010 \text{ fm}^2$$
+
+T-violation parameters in $K^0-\bar{K}^0$ mixing [r]
+
+Asymmetry $A_T$ in $K^0-\bar{K}^0$ mixing = $(6.6 \pm 1.6) \times 10^{-3}$
+
+CP-violation parameters
+
+$$\mathrm{Re}(\epsilon) = (1.596 \pm 0.013) \times 10^{-3}$$
+
+CPT-violation parameters [r]
+
+$$\mathrm{Re}\,\delta = (2.5 \pm 2.3) \times 10^{-4}$$
+
+$$\mathrm{Im}\,\delta = (-1.5 \pm 1.6) \times 10^{-5}$$
+
+$\mathrm{Re}(y)$, $K_{e3}$ parameter = $(0.4 \pm 2.5) \times 10^{-3}$
+
+$\mathrm{Re}(x_−)$, $K_{e3}$ parameter = $(-2.9 \pm 2.0) \times 10^{-3}$
+
+$$|m_{K^0} - m_{\bar{K}^0}| / m_{\text{average}} < 6 \times 10^{-19}, \text{ CL} = 90\% [\text{V}]$$
+
+$$(\Gamma_{K^0} - \Gamma_{\bar{K}^0})/m_{\text{average}} = (8 \pm 8) \times 10^{-18}$$
+
+Tests of $\Delta S = \Delta Q$
+
+$$\mathrm{Re}(x_+), K_{e3} \text{ parameter} = (-0.9 \pm 3.0) \times 10^{-3}$$
+
+$$I(J^P) = \frac{1}{2}(0^-)$$
+
+Mean life $\tau = (0.8954 \pm 0.0004) \times 10^{-10}$ s (S = 1.1) Assuming CPT
+
+Mean life $\tau = (0.89564 \pm 0.00033) \times 10^{-10}$ s Not assuming CPT
+$c\tau = 2.6844 \text{ cm}$ Assuming CPT
+---PAGE_BREAK---
+
+CP-violation parameters [z]
+
+$$
+\begin{align*}
+\operatorname{Im}(\eta_{+-0}) &= -0.002 \pm 0.009 \\
+\operatorname{Im}(\eta_{000}) &= -0.001 \pm 0.016
+\end{align*}
+$$
+
+$$
+|\eta_{000}| = |A(K_S^0 \rightarrow 3\pi^0)/A(K_L^0 \rightarrow 3\pi^0)| < 0.0088, \text{ CL} = 90\%
+$$
+
+CP asymmetry A in π⁺π⁻ e⁺e⁻ = (-0.4 ± 0.8)%
+
+
+
+
+
+
+ | K0S DECAY MODES |
+ Fraction (Γf/Γ) |
+ Scale factor/
Confidence level |
+ ρ
(MeV/c) |
+
+
+
+
+ | Hadronic modes |
+
+
+ | π0π0 |
+ (30.69±0.05) % |
+ |
+ 209 |
+
+
+ | π+π- |
+ (69.20±0.05) % |
+ |
+ 206 |
+
+
+ | π+π-π0 |
+ (3.5 +1.1-0.9) × 10-7 |
+ |
+ 133 |
+
+
+ | Modes with photons or lℓ pairs |
+
+
+ | π+π-γ |
+ [t,aa] (1.79±0.05) × 10-3 |
+ |
+ 206 |
+
+
+ | π+π-e+e- |
+ (4.79±0.15) × 10-5 |
+ |
+ 206 |
+
+
+ | π0γγ |
+ [aa] (4.9 ± 1.8) × 10-8 |
+ |
+ 230 |
+
+
+ | γγ |
+ (2.63±0.17) × 10-6 |
+ S=3.0 |
+ 249 |
+
+
+ | Semileptonic modes |
+
+
+ | π±e&mpart;νe |
+ [bb] (7.04±0.08) × 10-4 |
+ |
+ 229 |
+
+
+ | CP violating (CP) and ΔS = 1 weak neutral current (S1) modes |
+
+
+ | 3π0 |
+ CP < 2.6 × 10-8 |
+ CL=90% |
+ 139 |
+
+
+ | μ+μ- |
+ S1 < 8 × 10-10 |
+ CL=90% |
+ 225 |
+
+
+ | e+e- |
+ S1 < 9 × 10-9 |
+ CL=90% |
+ 249 |
+
+
+ | π0e+e- |
+ S1 [aa] (3.0 +1.5-1.2) × 10-9 |
+ |
+ 230 |
+
+
+ | π0μ+μ- |
+ S1 (2.9 +1.5-1.2) × 10-9 |
+ |
+ 177 |
+
+
+
+
+$$
+I(J^P) = \frac{1}{2}(0^{-})
+$$
+
+$m_{K_L} - m_{K_S}$
+
+$$
+\begin{align*}
+&= (0.5293 \pm 0.0009) \times 10^{10} \, \hbar \, \text{s}^{-1} && (\text{S} = 1.3) \quad \text{Assuming CPT} \\
+&= (3.484 \pm 0.006) \times 10^{-12} \, \text{MeV} && \text{Assuming CPT} \\
+&= (0.5289 \pm 0.0010) \times 10^{10} \, \hbar \, \text{s}^{-1} && \text{Not assuming CPT}
+\end{align*}
+$$
+
+Mean life $\tau = (5.116 \pm 0.021) \times 10^{-8}$ s ($S = 1.1$)
+
+$c\tau = 15.34 \text{ m}$
+
+**Slope parameters** $^{[q]}$
+
+(See Particle Listings for other linear and quadratic coefficients)
+
+$$
+\begin{align*}
+K_L^0 &\rightarrow \pi^+\pi^-\pi^0: g = 0.678 \pm 0.008 && (S = 1.5) \\
+K_L^b &\rightarrow \pi^+\pi^-\pi^0: h = 0.076 \pm 0.006 \\
+K_L^c &\rightarrow \pi^+\pi^-\pi^0: k = 0.0099 \pm 0.0015 \\
+K_L^d &\rightarrow \pi^0\pi^0\pi^0: h = (0.6 \pm 1.2) \times 10^{-3}
+\end{align*}
+$$
+
+$K_L$ decay form factors [r]
+
+Linear parametrization assuming $\mu-e$ universality
+
+$$
+\lambda_+(K_{\mu 3}^0) = \lambda_+(K_{e3}^0) = (2.82 \pm 0.04) \times 10^{-2} \quad (\text{S} = 1.1)
+$$
+
+$$
+\lambda_0(K_{\mu 3}^0) = (1.38 \pm 0.18) \times 10^{-2} \quad (\text{S} = 2.2)
+$$
+---PAGE_BREAK---
+
+### Quadratic parametrization assuming $\mu$-e universality
+
+$$ \lambda'_+(\mathcal{K}_{\mu 3}^0) = \lambda'_+(\mathcal{K}_{e3}^0) = (2.40 \pm 0.12) \times 10^{-2} \quad (\text{S} = 1.2) $$
+
+$$ \lambda''_+(\mathcal{K}_{\mu 3}^0) = \lambda''_+(\mathcal{K}_{e3}^0) = (0.20 \pm 0.05) \times 10^{-2} \quad (\text{S} = 1.2) $$
+
+$$ \lambda_0(\mathcal{K}_{\mu 3}^0) = (1.16 \pm 0.09) \times 10^{-2} \quad (\text{S} = 1.2) $$
+
+### Pole parametrization assuming $\mu$-e universality
+
+$$ M_V^\mu(\mathcal{K}_{\mu 3}^0) = M_V^e(\mathcal{K}_{e3}^0) = 878 \pm 6 \text{ MeV} \quad (\text{S} = 1.1) $$
+
+$$ M_S^\mu(\mathcal{K}_{\mu 3}^0) = 1252 \pm 90 \text{ MeV} \quad (\text{S} = 2.6) $$
+
+### Dispersive parametrization assuming $\mu$-e universality
+
+$$ \Lambda_+ = (2.51 \pm 0.06) \times 10^{-2} \quad (\text{S} = 1.5) $$
+
+$$ \ln(C) = (1.75 \pm 0.18) \times 10^{-1} \quad (\text{S} = 2.0) $$
+
+$$ K_{e3}^{0} |f_{5}/f_{+}| = (1.5^{+1.4}_{-1.6}) \times 10^{-2} $$
+
+$$ K_{e3}^{0} |f_{T}/f_{+}| = (5^{+4}_{-5}) \times 10^{-2} $$
+
+$$ K_{\mu 3}^{0} |f_{T}/f_{+}| = (12 \pm 12) \times 10^{-2} $$
+
+$$ K_L \rightarrow \ell^+\ell^-\gamma, K_L \rightarrow \ell^+\ell^-\ell'^+\ell'^- : \alpha_{K^*} = -0.205 \pm 0.022 \quad (\text{S} = 1.8) $$
+
+$$ K_L^0 \rightarrow \ell^+\ell^-\gamma, K_L^0 \rightarrow \ell^+\ell^-\ell'^+\ell'^- : \alpha_{DIP} = -1.69 \pm 0.08 \quad (\text{S} = 1.7) $$
+
+$$ K_L \rightarrow \pi^+\pi^- e^+e^- : a_1/a_2 = -0.737 \pm 0.014 \text{ GeV}^2 $$
+
+$$ K_L \rightarrow \pi^0 2\gamma: \quad a_V = -0.43 \pm 0.06 \quad (\text{S} = 1.5) $$
+
+### CP-violation parameters [z]
+
+$$ A_L = (0.332 \pm 0.006)\% $$
+
+$$ |\eta_{00}| = (2.220 \pm 0.011) \times 10^{-3} \quad (\text{S} = 1.8) $$
+
+$$ |\eta_{+-}| = (2.232 \pm 0.011) \times 10^{-3} \quad (\text{S} = 1.8) $$
+
+$$ |\epsilon| = (2.228 \pm 0.011) \times 10^{-3} \quad (\text{S} = 1.8) $$
+
+$$ |\eta_{00}/\eta_{+-}| = 0.9950 \pm 0.0007 \quad [\text{cc}] \quad (\text{S} = 1.6) $$
+
+$$ \mathrm{Re}(\epsilon'/\epsilon) = (1.66 \pm 0.23) \times 10^{-3} \quad [\mathrm{cc}] \quad (\text{S} = 1.6) $$
+
+### Assuming CPT
+
+$$ \phi_{+-} = (43.51 \pm 0.05)^{\circ} \quad (\text{S} = 1.2) $$
+
+$$ \phi_{00} = (43.52 \pm 0.05)^{\circ} \quad (\text{S} = 1.3) $$
+
+$$ \phi_e = \phi_{SW} = (43.52 \pm 0.05)^{\circ} \quad (\text{S} = 1.2) $$
+
+$$ \mathrm{Im}(\epsilon'/\epsilon) = -(a_{00} - a_{+-})/3 = (-0.002 \pm 0.005)^{\circ} \quad (\text{S} = 1.7) $$
+
+### Not assuming CPT
+
+$$ \phi_{+-} = (43.4 \pm 0.5)^{\circ} \quad (\text{S} = 1.2) $$
+
+$$ a_{\phi(5)} = (43.7 \pm 0.6)^{\circ} \quad (\text{S} = 1.2) $$
+
+$$ a_e = (43.5 \pm 0.5)^{\circ} \quad (\text{S} = 1.3) $$
+
+### CP asymmetry A in $K_L^0$
+$\pi^+\pi^- e^+e^- = (13.7 \pm 1.5)\%$
+
+$$ \beta_{CP} \text{ from } K_L^0 \rightarrow e^+e^- e^+e^- = -0.19 \pm 0.07 $$
+
+$$ \gamma_{CP} \text{ from } K_L^L \rightarrow e^+e^- e^+e^- = 0.01 \pm 0.11 \quad (\text{S} = 1.6) $$
+
+### j for $K_L^L$
+$\pi^+\pi^-\pi^0 = 0.0012 \pm 0.0008$
+
+### f for $K_L^L$
+$\pi^+\pi^-\pi^0 = 0.004 \pm 0.006$
+
+$$ |\eta_{+-\gamma}| = (2.35 \pm 0.07) \times 10^{-3} $$
+
+$$ \phi_{+-\gamma} = (44 \pm 4)^{\circ} $$
+---PAGE_BREAK---
+
+$$
+\begin{gather*}
+|\epsilon'_{+-\gamma}|/\epsilon < 0.3, \text{ CL} = 90\% \\
+|g_{E1}| \text{ for } K_L^0 \rightarrow \pi^+\pi^-\gamma < 0.21, \text{ CL} = 90\%
+\end{gather*}
+$$
+
+**T-violation parameters**
+
+$$
+\operatorname{Im}(\xi) \text{ in } K_{\mu 3}^{0}=-0.007 \pm 0.026
+$$
+
+CPT invariance tests
+
+$$
+\phi_{00} - \phi_{+-} = (0.34 \pm 0.32)^{\circ} \\
+\mathrm{Re}(\frac{2}{3}\eta_{+-} + \frac{1}{3}\eta_{00}) - \frac{\Delta\mu}{2} = (-3 \pm 35) \times 10^{-6}
+$$
+
+$\Delta S = -\Delta Q$ in $K_{e3}^0$ decay
+
+$$
+\begin{align*}
+\operatorname{Re} x &= -0.002 \pm 0.006 \\
+\operatorname{Im} x &= 0.0012 \pm 0.0021
+\end{align*}
+$$
+
+
+
+
+ | K0L DECAY MODES |
+ Fraction (Γf/Γ) |
+ Scale factor/ p |
+ Confidence level (MeV/c) |
+
+
+
+
+ | Semileptonic modes |
+
+
+ π±e∓νe
Called K0e3. |
+ [bb] (40.55 ± 0.11 ) % |
+ S=1.7 |
+ 229 |
+
+
+ π±μ∓νμ
Called K0μ3. |
+ [bb] (27.04 ± 0.07 ) % |
+ S=1.1 |
+ 216 |
+
+
+ (πμatom)ν
π0π±e∓ν
π±e∓νe+e- |
+ ( 1.05 ± 0.11 ) × 10-7
[bb] ( 5.20 ± 0.11 ) × 10-5
[bb] ( 1.26 ± 0.04 ) × 10-5 |
+ |
+ 188
207
229 |
+
+
+ | Hadronic modes, including Charge conjugation × Parity Violating (CPV) modes |
+
+
+ | 3π0 |
+ (19.52 ± 0.12 ) % |
+ S=1.6 |
+ 139 |
+
+
+ | π+π-π0 |
+ (12.54 ± 0.05 ) % |
+ |
+ 133 |
+
+
+ | π+π- |
+ CPV [dd] ( 1.967±0.010 ) × 10-3 |
+ S=1.5 |
+ 206 |
+
+
+ | π0π0 |
+ CPV ( 8.64 ± 0.06 ) × 10-4 |
+ S=1.8 |
+ 209 |
+
+
+ | Semileptonic modes with photons |
+
+
+ π±e∓νeγ
π±μ∓νμγ |
+ [t,bb,ee] ( 3.79 ± 0.06 ) × 10-3
( 5.65 ± 0.23 ) × 10-4 |
+ |
+ 229
216 |
+
+
+ | Hadronic modes with photons or lℓ pairs |
+
+
+ π0π0γ
π+π-γ
π+π-γ(DE)
π02γ
π0γe+e- |
+ < 2.43 × 10-7
[t,ee] ( 4.15 ± 0.15 ) × 10-5
( 2.84 ± 0.11 ) × 10-5
[ee] ( 1.273±0.033 ) × 10-6
( 1.62 ± 0.17 ) × 10-8 |
+ CL=90%
S=2.8
S=2.0
S=2.0
S=1.1 |
+ 209
206
206
230
230
249
249
249
225
225 |
+
+
+ | Other modes with photons or lℓ pairs |
+
+
+ 2γ
3γ
e+e-γ
μ+μ-γ
e+e-γγ
μ+μ-γγ |
+ ( 5.47 ± 0.04 ) × 10-4
< 7.4 × 10-8
( 9.4 ± 0.4 ) × 10-6
( 3.59 ± 0.11 ) × 10-7
[ee] ( 5.95 ± 0.33 ) × 10-7
[ee] ( 1.0 +0.8 -0.6 ) × 10-8 |
+ S=1.1
CL=90%
S=2.0
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
S=1.3
( 6.84 ± 0.11 ) × 10-9
( +6 -4 ) × 10-12
( 9 +6 -4 ) × 10-7 |
+ 249
|
+
+
+ Charge conjugation × Parity (CP) or Lepton Family number (LF)
violating modes, or D S = 1 weak neutral current (SI) modes |
+
+
+ μ+μ-
e+e-
π+π-e+e- |
+ SI ( ( +6 -4 ) × 10-9
( +6 -4 ) × 10-7
( +6 -4 ) × 10-7)
( ( 6.84 ± 0.11 ) × 10-9
( +6 -4 ) × 10-7
( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7)
( ( +6 -4 ) × 10-7 SI is a weakly charged lepton. |
+ 225
SI is a weakly charged lepton.
\n249
\n225
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\nSI is a weakly charged lepton.
\n\\textbf{Note: SI's are usually chargeless particles, so their charge should be zero in these cases and not appear in the table above as 'chargeless' or 'zero charge'. |
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | π0π0 e+e- |
+ S1 |
+ < 6.6 |
+ × 10-9 |
+ CL=90% |
+ 209 |
+
+
+ | π0π0 μ+μ- |
+ S1 |
+ < 9.2 |
+ × 10-11 |
+ CL=90% |
+ 57 |
+
+
+ | μ+μ- e+e- |
+ S1 |
+ ( 2.69 ±0.27 ) |
+ × 10-9 |
+ |
+ 225 |
+
+
+ | e+e- e+e- |
+ S1 |
+ ( 3.56 ±0.21 ) |
+ × 10-8 |
+ |
+ 249 |
+
+
+ | π0 μ+μ- |
+ CP,S1 [π-] |
+ < 3.8 |
+ × 10-10 |
+ CL=90% |
+ 177 |
+
+
+ | π0 e+e- |
+ CP,S1 [π-] |
+ < 2.8 |
+ × 10-10 |
+ CL=90% |
+ 230 |
+
+
+ | π0νν̄ |
+ CP,S1 [gg] |
+ < 3.0 |
+ × 10-9 |
+ CL=90% |
+ 230 |
+
+
+ | π0π0ν̄ν̄ |
+ S1 |
+ < 8.1 |
+ × 10-7 |
+ CL=90% |
+ 209 |
+
+
+ | e±μ∓ |
+ LF [bb] |
+ < 4.7 |
+ × 10-12 |
+ CL=90% |
+ 238 |
+
+
+ | e±e±μ∓μ∓ |
+ LF [bb] |
+ < 4.12 |
+ × 10-11 |
+ CL=90% |
+ 225 |
+
+
+ | π0μ±e∓ |
+ LF [bb] |
+ < 7.6 |
+ × 10-11 |
+ CL=90% |
+ 217 |
+
+
+ | π0π0 μ±e∓ |
+ LF |
+ < 1.7 |
+ × 10-10 |
+ CL=90% |
+ 159 |
+
+
+
+
+$K_0^*(700)$
+
+$$
+I(J^P) = \frac{1}{2}(0^+)
+$$
+
+also known as κ; was $K_0^*(800)$
+
+Mass (T-Matrix Pole $\sqrt{s}$) = (630–730) – i (260–340) MeV
+
+Mass (Breit-Wigner) = 824 ± 30 MeV
+
+Full width (Breit-Wigner) = 478 ± 50 MeV
+
+| K⁰(700) DECAY MODES | Fraction (Γᵢ/Γ) | p (MeV/c) |
|---|
| Kπ | 100 % | 240 |
+
+$K^*(892)$
+
+$$
+I(J^P) = \frac{1}{2}(1^-)
+$$
+
+$K^*(892)^{\pm}$ hadroproduced mass $m = 891.66 \pm 0.26$ MeV
+
+$K^*(892)^{\pm}$ in $\tau$ decays mass $m = 895.5 \pm 0.8$ MeV
+
+$K^*(892)^{0}$ mass $m = 895.55 \pm 0.20$ MeV (S = 1.7)
+
+$K^*(892)^{\pm}$ hadroproduced full width $\Gamma = 50.8 \pm 0.9$ MeV
+
+$K^*(892)^{\pm}$ in $\tau$ decays full width $\Gamma = 46.2 \pm 1.3$ MeV
+
+$K^*(892)^{0}$ full width $\Gamma = 47.3 \pm 0.5$ MeV (S = 1.9)
+
+| K*(892) DECAY MODES | Fraction (Γᵢ/Γ) | Confidence level | p
(MeV/c) |
|---|
| Kπ | ~ 100 % | | 289 | | K⁰γ | ( 2.46±0.21 ) × 10⁻³ | | 307 | | K∓γ | ( 9.9 ±0.9 ) × 10⁻⁴ | | 309 | | Kππ | < 7 × 10⁻⁴ | 95% | 223 |
+
+$K_1(1270)$
+
+$$
+I(J^P) = \frac{1}{2}(1^+)
+$$
+
+Mass $m = 1253 \pm 7$ MeV [$\not{J}$] (S = 2.2)
+
+Full width $\Gamma = 90 \pm 20$ MeV [$\not{J}$]
+
+| K₁(1270) DECAY MODES | Fraction (Γᵢ/Γ) | p (MeV/c) |
|---|
|
| Kρ | (42 ±6)% | † |
|---|
| K₀*(1430)π | (28 ±4)% | † |
|---|
| K*(892)π | (16 ±5)% | ‡† |
|---|
| Kω | (11.0±2.0)% | †† |
|---|
| Kf₀(1370) | (3.0±2.0)% | †† |
|---|
+
+See Particle Listings for 1 decay modes that have been seen / not seen.
+---PAGE_BREAK---
+
+### $K_1(1400)$
+
+$$I(J^P) = \frac{1}{2}(1^+)$$
+
+Mass $m = 1403 \pm 7$ MeV
+Full width $\Gamma = 174 \pm 13$ MeV (S = 1.6)
+
+| K1(1400) DECAY MODES | Fraction (Γf/Γ) | p (MeV/c) |
|---|
| K*(892) π | (94 ±6) % | 402 | | Kρ | (3.0±3.0) % | 293 | | Kf0(1370) | (2.0±2.0) % | † | | Kω | (1.0±1.0) % | 284 |
+
+See Particle Listings for 2 decay modes that have been seen / not seen.
+
+### $K^*(1410)$
+
+$$I(J^P) = \frac{1}{2}(1^-)$$
+
+Mass $m = 1414 \pm 15$ MeV (S = 1.3)
+Full width $\Gamma = 232 \pm 21$ MeV (S = 1.1)
+
+| K*(1410) DECAY MODES | Fraction (Γf/Γ) | Confidence level | p (MeV/c) |
|---|
| K*(892) π | > 40 % | 95% | 410 | | Kπ | (6.6±1.3) % | | 612 | | Kρ | < 7 % | 95% | 305 | | γK0 | < 2.3 × 10-4 | 90% | 619 |
+
+### $K_0^*(1430)^{[hh]}$
+
+$$I(J^P) = \frac{1}{2}(0^+)$$
+
+Mass $m = 1425 \pm 50$ MeV
+Full width $\Gamma = 270 \pm 80$ MeV
+
+| K0* (1430) DECAY MODES | Fraction (Γf/Γ) | p (MeV/c) |
|---|
| Kπ | (93 ±10)% | 619 | | Kη | (8.6+/3.4)% | 486 |
+
+See Particle Listings for 1 decay mode that has been seen / not seen.
+
+### $K_2^*(1430)$
+
+$$I(J^P) = \frac{1}{2}(2^+)$$
+
+$K_2^*(1430)^{\pm}$ mass $m = 1427.3 \pm 1.5$ MeV (S = 1.3)
+$K_2^*(1430)^{0}$ mass $m = 1432.4 \pm 1.3$ MeV
+$K_2^*(1430)^{\pm}$ full width $\Gamma = 100.0 \pm 2.1$ MeV
+$K_2^*(1430)^{0}$ full width $\Gamma = 109 \pm 5$ MeV (S = 1.9)
+
+| K2* (1430) DECAY MODES | Fraction (Γf/Γ) | Scale factor/
Confidence level | p
(MeV/c) |
|---|
| Kπ | (49.9±1.2) % | | 620 | | K*(892) π | (24.7±1.5) % | | 420 | | K*(892) ππ | (13.4±2.2) % | | 373 | | Kρ | (8.7±0.8) % | S=1.2 | 320 | | Kω | (2.9±0.8) % | | 313 | | K+γ | (2.4±0.5) × 10-3 | S=1.1 | 628 | | Kη | (1.5+3.4/1.0) × 10-3 | S=1.3 | 488 |
+---PAGE_BREAK---
+
+
+
+
+ | Kωπ |
+ < 7.2 |
+ × 10-4 |
+ CL=95% |
+ 106 |
+
+
+ | K0γ |
+ < 9 |
+ × 10-4 |
+ CL=90% |
+ 627 |
+
+
+
+
+$$
+\begin{array}{l}
+K^*(1680) \\
+\quad \text{Mass } m = 1718 \pm 18 \text{ MeV} \\
+\quad \text{Full width } \Gamma = 322 \pm 110 \text{ MeV (S = 4.2)}
+\end{array}
+$$
+
+$$
+I(J^P) = \frac{1}{2}(1^{-})
+$$
+
+
+
+
+ |
+ K*(1680) DECAY MODES
+ |
+
+ Fraction (Γ
+
+ f
+
+ /Γ)
+ |
+
+ p (MeV/c)
+ |
+
+
+
+
+ |
+ Kπ
+ |
+
+ (38.7±2.5) %
+ |
+
+ 782
+ |
+
+
+ |
+ Kρ
+ |
+
+ (31.4
+
+ +5.0
+
+
+ −2.1
+
+ ) %
+ |
+
+ 571
+ |
+
+
+ |
+ K*(892)π
+ |
+
+ (29.9
+
+ +2.2
+
+
+ −5.0
+
+ ) %
+ |
+
+ 618
+ |
+
+
+
+
+See Particle Listings for 1 decay modes that have been seen / not seen.
+
+$$
+\begin{array}{l}
+K_2(1770) [ii] \\
+\quad \text{Mass } m = 1773 \pm 8 \text{ MeV} \\
+\quad \text{Full width } \Gamma = 186 \pm 14 \text{ MeV}
+\end{array}
+$$
+
+$$
+I(J^P) = \frac{1}{2}(2^{-})
+$$
+
+
+
+
+ |
+ K2(1770) DECAY MODES
+ |
+
+ Fraction (Γf/Γ)
+ |
+
+ p (MeV/c)
+ |
+
+
+
+
+ |
+ Kππ
+ |
+
+ |
+
+ 794
+ |
+
+
+ |
+ See Particle Listings for 5 decay modes that have been seen / not seen.
+ |
+
+
+
+
+$$
+\begin{array}{l}
+K_3^*(1780) \\
+\quad \text{Mass } m = 1776 \pm 7 \text{ MeV (S = 1.1)} \\
+\quad \text{Full width } \Gamma = 159 \pm 21 \text{ MeV (S = 1.3)}
+\end{array}
+$$
+
+$$
+I(J^P) = \frac{1}{2}(3^{-})
+$$
+
+
+
+
+| K3*(1780) DECAY MODES |
+Fraction (Γf/Γ) |
+Confidence level |
+p (MeV/c) |
+
+
+
+
+| Kρ |
+(31 ± 9 ) % |
+ |
+613 |
+
+
+| K* (892) π |
+(20 ± 5 ) % |
+ |
+656 |
+
+
+| Kπ |
+(18.8± 1.0 ) % |
+ |
+813 |
+
+
+| Kη |
+(30 ±13 ) % |
+ |
+719 |
+
+
+| K*2(1430) π |
+< 16 % |
+95% |
+290 |
+
+
+
+
+$$
+K_2(1820) [Jl]
+\qquad I(J^P) = \frac{1}{2}(2^{-})
+$$
+
+$$
+\begin{array}{l}
+\text{Mass } m = 1819 \pm 12 \text{ MeV} \\
+\text{Full width } \Gamma = 264 \pm 34 \text{ MeV}
+\end{array}
+$$
+
+$$
+K_4^*(2045) \\
+I(J^P) = \frac{1}{2}(4^{+})
+$$
+
+$$
+\begin{array}{l}
+\text{Mass } m = 2048_{-9}^{+8} \text{ MeV (S = 1.1)} \\
+\text{Full width } \Gamma = 199_{-19}^{+27} \text{ MeV}
+\end{array}
+$$
+
+
+
+
+ | K*4(2045) DECAY MODES |
+ Fraction (Γf/Γ) |
+ p (MeV/c) |
+
+
+
+
+ | Kπ |
+ (9.9±1.2) % |
+ 960 |
+
+
+ | K*(892)π�� |
+ (9 ±5 ) % |
+ 804 |
+
+
+
+---PAGE_BREAK---
+
+
+
+ |
+ K*(892) πππ
+ |
+
+ (7 ±5 ) %
+ |
+
+ 770
+ |
+
+
+ |
+ ρKπ
+ |
+
+ (5.7±3.2) %
+ |
+
+ 744
+ |
+
+
+ |
+ ωKπ
+ |
+
+ (5.0±3.0) %
+ |
+
+ 740
+ |
+
+
+ |
+ φKπ
+ |
+
+ (2.8±1.4) %
+ |
+
+ 597
+ |
+
+
+ |
+ φK*(892)
+ |
+
+ (1.4±0.7) %
+ |
+
+ 368
+ |
+
+
+
+CHARMED MESONS
+
+(C = ±1)
+
+$D^+ = c\bar{d}, D^0 = c\bar{u}, \bar{D}^0 = \bar{c}u, D^- = \bar{c}d,$
+
+similarly for D*'s
+
+$$
+D^{\pm} \qquad I(J^{P}) = \frac{1}{2}(0^{-})
+$$
+
+Mass $m = 1869.65 \pm 0.05$ MeV
+
+Mean life $\tau = (1040 \pm 7) \times 10^{-15}$ s
+
+$c\tau = 311.8~\mu m$
+
+c-quark decays
+
+$$
+\Gamma(c \rightarrow \ell^{+} anything)/\Gamma(c \rightarrow anything) = 0.096 \pm 0.004 [kk]
+$$
+
+$$
+\Gamma(c \rightarrow D^{*}(2010)^{+} anything)/\Gamma(c \rightarrow anything) = 0.255 \pm 0.017
+$$
+
+CP-violation decay-rate asymmetries
+
+$$
+A_{CP}(\mu^{\pm}\nu) = (8 \pm 8)\%
+$$
+
+$$
+A_{CP}(K_L^0 e^{\pm}\nu) = (-0.6 \pm 1.6)\%
+$$
+
+$$
+A_{CP}(K_S^0 \pi^{\pm}) = (-0.41 \pm 0.09)\%
+$$
+
+$$
+A_{CP}(K_L^0 K^{\pm}) \text{ in } D^{\pm} \rightarrow K_L^0 K^{\pm} = (-4.2 \pm 3.4) \times 10^{-2}
+$$
+
+$$
+A_{CP}(K^{\mp}2\pi^{\pm}) = (-0.18 \pm 0.16)\%
+$$
+
+$A_{CP}(K^{\mp}\pi^{\pm}\pi^0) = (-0.3 \pm 0.7)\%$
+
+$A_{CP}(K_0^0 \pi^{\pm} \pi^0) = (-0.1 \pm 0.7)\%$
+
+$A_{CP}(K_5^0 \pi^{\pm} \pi^+ \pi^-) = (0.0 \pm 1.2)\%$
+
+$A_{CP}(\pi^{\pm}\pi^0) = (2.4 \pm 1.2)\%$
+
+$A_{CP}(\pi^{\pm}\eta) = (1.0 \pm 1.5)\% \ (S = 1.4)$
+
+$A_{CP}(\pi^{\pm}\eta'(958)) = (-0.6 \pm 0.7)\%$
+
+$A_{CP}(K_0^0/K^0 K^{\pm}) = (0.11 \pm 0.17)\%$
+
+$A_{CP}(K_5^0 K^\pm) = (-0.01 \pm 0.07)\%$
+
+$A_{CP}(K_S^0 K^\pm \pi^0) \text{ in } D^\pm \to K_S^0 K^\pm \pi^0 = (1 \pm 4) \times 10^{-2}$
+
+$A_{CP}(K_5^0 K^\pm \pi^0) \text{ in } D^\pm \to K_5^0 K^\pm \pi^0 = (-1 \pm 4) \times 10^{-2}$
+
+$A_{CP}(K^+ K^- \pi^+) = (0.37 \pm 0.29)\%$
+
+$A_{CP}(K^+ K^{*0}) = (-0.3 \pm 0.4)\%$
+
+$A_{CP}(\phi\pi^\pm) = (0.01 \pm 0.09)\% \ (S = 1.8)$
+
+$A_{CP}(K^\pm K_0^\ast(1430)^0) = (8^{+7}_{-6})\%$
+
+$A_{CP}(K^\pm K_2^\ast(1430)^0) = (43^{+20}_{-26})\%$
+
+$A_{CP}(K^\pm K_0^\ast(700)) = (-12^{+18}_{-13})\%$
+
+$A_{CP}(a_0(1450)^0\pi^\pm) = (-19^{+14}_{-16})\%$
+
+$A_{CP}(\phi(1680)\pi^\pm) = (-9 \pm 26)\%$
+
+$A_{CP}(\pi^+\pi^-\pi^\pm) = (-2 \pm 4)\%$
+
+$A_{CP}(K_5^0 K^\pm \pi^+ \pi^-) = (-4 \pm 7)\%$
+
+$A_{CP}(K^\pm \pi^0) = (-4 \pm 11)\%$
+
+$\chi^2$ tests of CP-violation (CPV)
+
+Local CPV in $D^\pm \to \pi^+\pi^-\pi^\pm = 78.1\%$
+
+Local CPV in $D^\pm \to K^+K^-\pi^\pm = 31\%$
+---PAGE_BREAK---
+
+CP violating asymmetries of P-odd (T-odd) moments
+
+$$A_T(K_S^0 K^\pm \pi^+ \pi^-) = (-12 \pm 11) \times 10^{-3} [M]$$
+
+D⁺ form factors
+
+$$f_+(0)|V_{cs}| \text{ in } \bar{K}^0 \ell^+ \nu_\ell = 0.719 \pm 0.011 \quad (\text{S} = 1.6)$$
+
+$$r_1 \equiv a_1/a_0 \text{ in } \bar{K}^0 \ell^+ \nu_\ell = -2.13 \pm 0.14$$
+
+$$r_2 \equiv a_2/a_0 \text{ in } \bar{K}^0 \ell^+ \nu_\ell = -3 \pm 12 \quad (\text{S} = 1.5)$$
+
+$$f_+(0)|V_{cd}| \text{ in } \pi^0 \ell^+ \nu_\ell = 0.1407 \pm 0.0025$$
+
+$$r_1 \equiv a_1/a_0 \text{ in } \pi^0 \ell^+ \nu_\ell = -2.00 \pm 0.13$$
+
+$$r_2 \equiv a_2/a_0 \text{ in } \pi^0 \ell^+ \nu_\ell = -4 \pm 5$$
+
+$$f_+(0)|V_{cd}| \text{ in } D^+ \to \eta e^+ \nu_e = (8.3 \pm 0.5) \times 10^{-2}$$
+
+$$r_1 \equiv a_1/a_0 \text{ in } D^+ \to \eta e^+ \nu_e = -5.3 \pm 2.7 \quad (\text{S} = 1.9)$$
+
+$$r_v \equiv V(0)/A_1(0) \text{ in } D^+ \to \omega e^+ \nu_e = 1.24 \pm 0.11$$
+
+$$r_2 \equiv A_2(0)/A_1(0) \text{ in } D^+ \to \omega e^+ \nu_e = 1.06 \pm 0.16$$
+
+$$r_v \equiv V(0)/A_1(0) \text{ in } D^+, D^0 \to \rho e^+ \nu_e = 1.64 \pm 0.10 \quad (\text{S} = 1.2)$$
+
+$$r_2 \equiv A_2(0)/A_1(0) \text{ in } D^+, D^0 \to \rho e^+ \nu_e = 0.84 \pm 0.06$$
+
+$$r_v \equiv V(0)/A_1(0) \text{ in } K^*(892)^0 \ell^+ \nu_\ell = 1.49 \pm 0.05 \quad (\text{S} = 2.1)$$
+
+$$r_2 \equiv A_2(0)/A_1(0) \text{ in } K^*(892)^0 \ell^+ \nu_\ell = 0.802 \pm 0.021$$
+
+$$r_3 \equiv A_3(0)/A_1(0) \text{ in } K^*(892)^0 \ell^+ \nu_\ell = 0.04$$
+
+$$\Gamma_L/\Gamma_T \text{ in } K^*(892)^0 \ell^+ \nu_\ell = 1.13 \pm 0.08$$
+
+$$\Gamma_+/(\Gamma_-) \text{ in } K^*(892)^0 \ell^+ \nu_\ell = 0.22 \pm 0.06 \quad (\text{S} = 1.6)$$
+
+Most decay modes (other than the semileptonic modes) that involve a neutral K meson are now given as $K_S^0$ modes, not as $\bar{K}^0$ modes. Nearly always it is a $K_S^0$ that is measured, and interference between Cabibbo-allowed and doubly Cabibbo-suppressed modes can invalidate the assumption that $2\Gamma(K_S^0) = \Gamma(\bar{K}^0)$.
+
+| D+ DECAY MODES | Fraction (Γj/Γ) | Scale factor / Confidence level | ρ |
|---|
| Inclusive modes | | e+ semileptonic | (16.07 ± 0.30 )% | | - | | μ+ anything | (17.6 ± 3.2 )% | | - | | K- anything | (25.7 ± 1.4 )% | | - | | K0 anything + K0 anything | (61 ± 5 )% | | - | | K+ anything | (5.9 ± 0.8 )% | | - | | K*(892)- anything | (6 ± 5 )% | | - | | K*(892)0 anything | (23 ± 5 )% | | - | | K*(892)0 anything | < 6.6 % | CL=90% | - | | η anything | (6.3 ± 0.7 )% | | - | | η' anything | (1.04 ± 0.18 )% | | - | | φ anything | (1.12 ± 0.04 )% | | - | | Leptonic and semileptonic modes | | e+ νe | < 8.8 × 10-6 | CL=90% | 935 | | γe+νe | < 3.0 × 10-5 | CL=90% | 935 | | μ+νμ | (3.74 ± 0.17 ) × 10-4 | | 932 | | τ+ντ | (1.20 ± 0.27 ) × 10-3 | | 90 | | K0e+νe | (8.73 ± 0.10 )% | | 869 | | K0μ+νμ | (8.76 ± 0.19 )% | | 865 | | K-π+e+νe | (4.02 ± 0.18 )% | S=3.2 | 864 | | K-π+ (892)0e+νe, K*(892)0 → K-π+ (892)0e+νe | (3.77 ± 0.17 )% | | 722 | | (K-π+)[0.8-1.0]GeV e+νe | (3.39 ± 0.09 )% | | 864 |
+---PAGE_BREAK---
+
+
+
+
+ | (K-π+)S-wave e+νe |
+ ( 2.28 ± 0.11 ) × 10-3 |
+ - |
+
+
+ | K*(1410)0 e+νe, |
+ < 6 |
+ × 10-3 CL=90% |
+ - |
+
+
+ | K*(1410)0 → K-π+ |
+ |
+ |
+ |
+
+
+ | K̅2(1430)0 e+νe, |
+ < 5 |
+ × 10-4 CL=90% |
+ - |
+
+
+ | K*2(1430)0 → K-π+ |
+ |
+ |
+ |
+
+
+ | K-π+ e+νe nonresonant |
+ < 7 |
+ × 10-3 CL=90% |
+ 864 |
+
+
+ | K*(892)0 e+νe |
+ ( 5.40 ± 0.10 ) % |
+ S=1.1 |
+ 722 |
+
+
+ | K-π+μ+νμ |
+ ( 3.65 ± 0.34 ) % |
+ |
+ 851 |
+
+
+ | K*(892)0 μ+νμ, |
+ ( 3.52 ± 0.10 ) % |
+ |
+ 717 |
+
+
+ | K*(892)0 → K-π+ |
+ |
+ |
+ |
+
+
+ | K-π+μ+νμ nonresonant |
+ ( 1.9 ± 0.5 ) × 10-3 |
+ |
+ 851 |
+
+
+ | K*(892)0 μ+νμ |
+ ( 5.27 ± 0.15 ) % |
+ |
+ 717 |
+
+
+ | K-π+π0μ+νμ |
+ < 1.5 |
+ × 10-3 CL=90% |
+ 825 |
+
+
+ | K̅1(1270)0 e+νe, K̅10 → |
+ ( 1.06 ± 0.15 ) × 10-3 |
+ |
+ - |
+
+
+ | K-π+π0 |
+ |
+ |
+ |
+
+
+ | K*0(1430)0μ+νμ |
+ < 2.3 |
+ × 10-4 CL=90% |
+ 380 |
+
+
+ | K*(1680)0 μ+νμ |
+ < 1.5 |
+ × 10-3 CL=90% |
+ 105 |
+
+
+ | π0e+νe |
+ ( 3.72 ± 0.17 ) × 10-3 |
+ S=2.0 |
+ 930 |
+
+
+ | π0μ+νμ |
+ ( 3.50 ± 0.15 ) × 10-3 |
+ |
+ 927 |
+
+
+ | ηe+νe |
+ ( 1.11 ± 0.07 ) × 10-3 |
+ |
+ 855 |
+
+
+ | π-π+e+νe |
+ ( 2.45 ± 0.10 ) × 10-3 |
+ |
+ 924 |
+
+
+ | f0(500)0e+νe, f0(500)0 → |
+ ( 6.3 ± 0.5 ) × 10-4 |
+ |
+ - |
+
+
+ | π±± |
+ |
+ |
+ |
+
+
+ | ρ0e+νe |
+ ( 2.18 ± 0.17) × 10-3 |
+ |
+ 774 |
+
+
+ | ρ0μ+νμ |
+ ( 2.4 ± 0.4 ) × 10-3 |
+ |
+ 770 |
+
+
+ | ωe+νe |
+ ( 1.69 ± 0.11 ) × 10-3 |
+ |
+ 771 |
+
+
+ | η'(958)e+νe |
+ ( 2.0 ± 0.4 ) × 10-4 |
+ |
+ 690 |
+
+
+ | a(980)0e+νe, a(980)0 → ηπ0 |
+ ( 1.7 ± 0.8) × 10-4 |
+ |
+ - |
+
+
+ | φe+νe |
+ < 1.3 |
+ × 10-5 |
+ CL=90% |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
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+
+ Hadronic modes with a K̄ or KK̄̄ | | KS0π+- | ( .562±.03 ) % | | S=. | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . | . |
|---|
+
+
+---PAGE_BREAK---
+
+
+
+
+ | K̅0(1680)0π+, K̅00 → KS0π0 |
+ (10 ± 7 / -10) × 10-4 |
+ - |
+
+
+ | π̅0π+, π̅0 → KS0π0 |
+ (6 ± 5 / -4) × 10-3 |
+ - |
+
+
+ | KS0π+π0 nonresonant |
+ (3 ± 4) × 10-3 |
+ 845 |
+
+
+ KS0π+π0 nonresonant and
π̅0π+ |
+ (1.37 ± 0.21 / -0.40) % |
+ - |
+
+
+ | (KS0π0)S-waveπ+ |
+ (1.27 ± 0.27 / -0.33) % |
+ 845 |
+
+
+ | KS0π+η'(958) |
+ (1.90 ± 0.21) × 10-3 |
+ 481 |
+
+
+ | K-2π+π0 |
+ [pp] (6.25 ± 0.18) % |
+ 816 |
+
+
+ | KS02π+π- |
+ [pp] (3.10 ± 0.09) % |
+ 814 |
+
+
+ | K-3π+π- |
+ [nn] (5.7 ± 0.5) × 10-3
(1.2 ± 0.4) × 10-3 |
+ S=1.1 772
645 |
+
+
+ K̂*(892)02π+π-,
(2.3 ± 0.4) × 10-3 |
+ |
+ 239 |
+
+
+ | K̂*(892)0 → K-π+ |
+ (9.3 ± 1.9) × 10-3 |
+ † |
+
+
+ | K̂*(892)0 → K-π+ |
+ (1.72 ± 0.28) × 10-3 |
+ 524 |
+
+
+ | K-3π+π- nonresonant |
+ (4.0 ± 2.9) × 10-4 |
+ 772 |
+
+
+ | K+2KS0 |
+ (2.54 ± 0.13) × 10-3 |
+ 545 |
+
+
+ | K+K-KS0π+ |
+ (2.4 ± 0.5) × 10-4 |
+ 436 |
+
+
+ | Pionic modes |
+
+
+ | π+π0 |
+ (1.247 ± 0.033) × 10-3 |
+ 925 |
+
+
+ | 2π+π- |
+ (3.27 ± 0.18) × 10-3 |
+ 909 |
+
+
+ | ρ0π+ |
+ (8.3 ± 1.5) × 10-4 |
+ 767 |
+
+
+ | π+(πS-πS-)S-wave |
+ (1.83 ± 0.16) × 10-3 |
+ 909 |
+
+
+ | σ̂̂, σ → π+π- |
+ (1.38 ± 0.12) × 10-3 |
+ - |
+
+
+ f0(980)πS+,
(f0(980))S-wave |
+ (1.56 ± 0.33) × 10-4 |
+ 669 |
+
+
+ f0(1370)πS+,
(f0(1370))S-wave |
+ (8 ± 4) × 10-5 |
+ - |
+
+
+ f2(1270)πS+,
(f2(1270))S-wave |
+ (5.0 ± 0.9) × 10-4 |
+ 485 |
+
+
+ ρ(1450)0πS+,
(rho(1450))S-wave |
+ < 8 × 10-5 |
+ CL=95% |
+
+
+ f0(1500)πS+,
(f0(1500))S-wave |
+ (1.1 ± 0.4) × 10-4 |
+ - |
+
+
+ f0(1710)πS+,
(f0(1710))S-wave |
+ < 5 × 10-5 |
+ CL=95% |
+
+
+ f0(1790)πS+,
(f0(1790))S-wave |
+ < 7 × 10-5 |
+ CL=95% |
+
+
+ | (πS-πS-)S-waveπ- |
+ < 1.2 × 10-4 |
+ CL=95% |
+
+
+ | Nonresonant modes with a KℬKℬ pair CL=95% |
+
+
+ | Hadronic modes with a KℬKℬ pair CL=95% |
+
+
+ | Nonresonant modes with a Kℬ |
+
+
+
+
+
+
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+
+
+
+
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | KS0K+π0 |
+ ( 5.07 ± 0.30 ) × 10-3 |
+ 744 |
+
+
+ | KS0K+π0 |
+ ( 5.24 ± 0.31 ) × 10-3 |
+ 744 |
+
+
+ | K+K-π+ |
+ [nn] ( 9.68 ± 0.18 ) × 10-3 |
+ 744 |
+
+
+ | φπ+ |
+ ( 5.70 ± 0.14 ) × 10-3 |
+ 647 |
+
+
+ | φπ+, φ → K+K- |
+ ( 2.69 + 0.07− 0.08 ) × 10-3 |
+ 647 |
+
+
+ K+K*(892)0,
K*(892)0 → K-π+ |
+ ( 2.49 + 0.08− 0.13 ) × 10-3 |
+ 613 |
+
+
+ K+K0*(1430)0,
K0*(1430)0 →
K-π+ |
+ ( 1.82 ± 0.35 ) × 10-3 |
+ - |
+
+
+ K+K2*(1430)0,
K2* → K-π+ |
+ ( 1.6 + 1.2− 0.8 ) × 10-4 |
+ - |
+
+
+ K+K0*(700),
K0* → K-π+ |
+ ( 6.8 + 3.5− 2.1 ) × 10-4 |
+ - |
+
+
+ a0(1450)0π+,
a0* → K+K- |
+ ( 4.5 + 7.0− 1.8 ) × 10-4 |
+ - |
+
+
+ | φ(1680)π+, φ → K+K- |
+ ( 4.9 + 4.0− 1.9 ) × 10-5 |
+ - |
+
+
+ | KS0KS0π+ |
+ ( 2.70 ± 0.13 ) × 10-3 |
+ 741 |
+
+
+ | KS+KS0π+π- |
+ ( 1.74 ± 0.18 ) × 10-3 |
+ 678 |
+
+
+ | KS0K-2π+ |
+ ( 2.38 ± 0.17 ) × 10-3 |
+ 678 |
+
+
+ | KS+K-2π+π- |
+ ( 2.3 ± 1.2 ) × 10-4 |
+ 601 |
+
+
+ | A few poorly measured branching fractions: |
+
+
+ | φπ+π0 |
+ ( 2.3 ± 1.0 ) % |
+ CL=90% |
+ 619 |
+
+
+ | φρ+ |
+ < 1.5 ± % |
+
+
+ | K+K-π+π0 non-φ |
+ ( 1.5 + 0.7− 0.6 ) % |
+ |
+ 682 |
+
+
+ | K*(892)+KS0 |
+ ( 1.7 ± 0.8 ) % |
+
+
+ | Doubly Cabibbo-suppressed modes |
+
+
+ | KS+π0 |
+ ( 2.08 ± 0.21 ) × 10-4 |
+ S=1.4 |
+ 864 |
+
+
+ | KS+η |
+ ( 1.25 ± 0.16 ) × 10-4 |
+ S=1.1 |
+
+
+ | KS+η'(958) |
+ ( 1.85 ± 0.20 ) × 10-4 |
+ |
+ 776
571
846
679
714 |
+
+
+ | KS+πs+πs- |
+ ( 4.91 ± 0.09 ) × 10-4 |
+
+
+ KS*+ρ*
(892)**
π**
KS*+π*
KS*+ρ*
(f0(980), fs(980) → π**
KS*+ρ*
(fs(980), fs⃝(980) → π**
KS⃝*+ρ*
(fs⃝(980), fs⃝⃗(980) → π**
KS⃝⃗*+ρ* |
+
+$\Delta C = 1$ weak neutral current (C1) modes, or Lepton Family number (LF) or Lepton number (L) violating modes
+
+
+
+
+ | $\pi^+ e^+ e^-$, $C_1$ |
+ < 1.1 |
+ $\times 10^{-6}$ CL=90% |
+ 930 |
+
+
+ | $\pi^+ \pi^0 e^+ e^-$, $C_1$ |
+ < 1.4 |
+ $\times 10^{-5}$ CL=90% |
+ 925 |
+
+
+ | $\pi^+ \phi, \phi \rightarrow e^+ e^-$, $[rr]$ |
+ (1.7 $\pm$ 1.4) |
+ $\times 10^{-6}$ CL=90% |
+ - |
+
+
+ | $\pi^+ \mu^+ \mu^-$, $C_1$ |
+ < 7.3 |
+ $\times 10^{-8}$ CL=90% |
+ 918 |
+
+
+ | $\pi^+ \phi, \phi \rightarrow \mu^+ \mu^-$, $[rr]$ |
+ (1.8 $\pm$ 0.8) |
+ $\times 10^{-6}$ CL=90% |
+ - |
+
+
+ | $\rho^+ \mu^+ \mu^-$, $C_1$ |
+ < 5.6 |
+ $\times 10^{-4}$ CL=90% |
+ 757 |
+
+
+ | $K^+ e^+ e^-$, $[ss]$ |
+ < 1.0 |
+ $\times 10^{-6}$ CL=90% |
+ 870 |
+
+
+ | $K^+ \pi^0 e^+ e^-$, $[ss]$ |
+ < 1.5 |
+ $\times 10^{-5}$ CL=90% |
+ 864 |
+
+
+ | $K_S^0 \pi^+ e^+ e^-$, $[ss]$ |
+ < 2.6 |
+ $\times 10^{-5}$ CL=90% |
+ - |
+
+
+
+
+
+ | KS⃝K⃝*K⃝(892)*K⃝*K⃝ | (5.77 ± 0.12) | × | 1e-5 CL=90% |
|---|
| KS⃝K⃝*K⃝(1430)*K⃝*K⃝ | (4.4 ± 2.6) | × | 1e-5 CL=90% |
|---|
| KS⃝K⃝(700), K⃝*K⃝ | (3.9 ± 2.7) | × | 1e-5 CL=90% |
|---|
+
+
+ | KS⃝K⃝*K⃝(892)*K⃝ | (2.70 ± 0.13) | × | 1e-3 CL=90% |
|---|
| KS⃝K⃝*K⃝(1430)*K⃝ | (1.74 ± 0.18) | × | 1e-3 CL=90% |
|---|
| KS⃝K⃝*K⃝(70) | (6.8 ± 3.5) | × | 1e-4 CL=90% |
|---|
+
+
+
+ | Branching fraction / Process / Notation / Unit / Sign / Precision / Range / Reference / Source / Notes / Example / Limitations / Implications / Other Information / Source / References / etc. | Value / Precision / Range / etc. |
|---|
φπ⁺π⁺π⁺ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ ��� K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K⁺K⁻ → K＋＋S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-Wave to S-WAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAVE TO SWAYAGE
+
+---PAGE_BREAK---
+
+
+
+
+ | K0S K+ e+ e- |
+ |
+ < 1.1 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | K+ μ+ μ- |
+ [ss] < 4.3 |
+ |
+ × 10-6 |
+ CL=90% |
+ 856 |
+
+
+ | π+ e+ μ- |
+ LF |
+ < 2.9 |
+ × 10-6 |
+ CL=90% |
+ 927 |
+
+
+ | π+ e- μ+ |
+ LF |
+ < 3.6 |
+ × 10-6 |
+ CL=90% |
+ 927 |
+
+
+ | K+ e+ μ- |
+ LF |
+ < 1.2 |
+ × 10-6 |
+ CL=90% |
+ 866 |
+
+
+ | K+ e- μ+ |
+ LF |
+ < 2.8 |
+ × 10-6 |
+ CL=90% |
+ 866 |
+
+
+ | π- 2e+ |
+ L |
+ < 1.1 |
+ × 10-6 |
+ CL=90% |
+ 930 |
+
+
+ | π- 2μ+ |
+ L |
+ < 2.2 |
+ × 10-8 |
+ CL=90% |
+ 918 |
+
+
+ | π- e+ μ+ |
+ L |
+ < 2.0 |
+ × 10-6 |
+ CL=90% |
+ 927 |
+
+
+ | ρ- 2μ+ |
+ L |
+ < 5.6 |
+ × 10-4 |
+ CL=90% |
+ 757 |
+
+
+ | K- 2e+ |
+ L |
+ < 9 |
+ × 10-7 |
+ CL=90% |
+ 870 |
+
+
+ | K0S π- 2e+ |
+ |
+ < 3.3 |
+ × 10-6 |
+ CL=90% |
+ 863 |
+
+
+ | K- π0 2e+ |
+ |
+ < 8.5 |
+ × 10-6 |
+ CL=90% |
+ 864 |
+
+
+ | K- 2μ+ |
+ L |
+ < 1.0 |
+ × 10-5 |
+ CL=90% |
+ 856 |
+
+
+ | K- e+ μ+ |
+ L |
+ < 1.9 |
+ × 10-6 |
+ CL=90% |
+ 866 |
+
+
+ | K* (892)- 2μ+ |
+ L |
+ < 8.5 |
+ × 10-4 |
+ CL=90% |
+ 703 |
+
+
+
+
+See Particle Listings for 2 decay modes that have been seen / not seen.
+
+$$
+\begin{array}{l}
+I(J^P) = \frac{1}{2}(0^{-}) \\
+\\
+\text{Mass } m = 1864.83 \pm 0.05 \text{ MeV} \\
+m_{D^{\pm}} - m_{D^{0}} = 4.822 \pm 0.015 \text{ MeV} \\
+\text{Mean life } \tau = (410.1 \pm 1.5) \times 10^{-15} \text{ s} \\
+c\tau = 122.9 \, \mu\text{m}
+\end{array}
+$$
+
+### Mixing and related parameters
+
+$$
+|m_{D_1^0} - m_{D_2^0}| = (0.95^{+0.41}_{-0.44}) \times 10^{10} \, \hbar \, s^{-1}
+$$
+
+$$
+(\Gamma_{D_1^0} - \Gamma_{D_2^0})/\Gamma = 2y = (1.29^{+0.14}_{-0.18}) \times 10^{-2}
+$$
+
+$$
+|q/p| = 0.92^{+0.12}_{-0.09}
+$$
+
+$$
+A_{\Gamma} = (-0.125 \pm 0.526) \times 10^{-3}
+$$
+
+$$
+\phi^{K_S^0 \pi \pi} = -0.09^{+0.10}_{-0.13}
+$$
+
+$K^+ \pi^- $ relative strong phase: $\cos \delta = 0.97 \pm 0.11$
+
+$K^- \pi^+ \pi^0$ coherence factor $R_{K\pi\pi^0} = 0.82 \pm 0.06$
+
+$K^- \pi^+ \pi^0$ average relative strong phase $\delta^{K\pi\pi^0} = (199 \pm 14)^{\circ}$
+
+$K^- \pi^- 2\pi^+$ coherence factor $R_{K3\pi} = 0.53^{+0.18}_{-0.21}$
+
+$K^- \pi^- 2\pi^+$ average relative strong phase $\delta^{K3\pi} = (125^{+22}_{-14})^\circ$
+
+$D^0 \rightarrow K^- \pi^- 2\pi^+, R_{K3\pi} (\text{y cos}\delta^{K3\pi} - \text{x sin}\delta^{K3\pi}) = (-3.0 \pm 0.7) \times 10^{-3} \text{ TeV}^{-1}$
+
+$K_S^0 K^+ \pi^- $ coherence factor $R_{K_S^0 K\pi} = 0.70 \pm 0.08$
+
+$K_S^0 K^+ \pi^-$ average relative strong phase $\delta^{K_S^0 K\pi} = (0 \pm 16)^\circ$
+
+$K^* K$ coherence factor $R_{K^* K} = 0.94 \pm 0.12$
+
+$K^* K$ average relative strong phase $\delta^{K^* K} = (-17 \pm 18)^\circ$
+
+### CP-violation decay-rate asymmetries (labeled by the D⁰ decay)
+
+$$
+A_{CP}(K^{+} K^{-}) = (-0.07 \pm 0.11)\%
+$$
+
+$$
+A_{CP}(2K_S^0) = (0.4 \pm 1.4)\%
+$$
+
+$$
+A_{CP}(\pi^+ \pi^-) = (0.13 \pm 0.14)\%
+$$
+
+$A_{CP}(\pi^0 \pi^0) = (0.0 \pm 0.6)\%$
+
+$$
+A_{CP}(\rho\gamma) = (6 \pm 15) \times 10^{-2}
+$$
+
+$$
+A_{CP}(\phi\gamma) = (-9 \pm 7) \times 10^{-2}
+$$
+
+$$
+A_{CP}(\overline{K^*}(892)^{0}\gamma) = (-0.3 \pm 2.0) \times 10^{-2}
+$$
+---PAGE_BREAK---
+
+$$A_{CP}(\pi^+\pi^-\pi^0) = (0.3 \pm 0.4)\%$$
+
+$$A_{CP}(\rho(770)^+\pi^- \rightarrow \pi^+\pi^-\pi^0) = (1.2 \pm 0.9)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(770)^0\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (-3.1 \pm 3.0)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(770)^-\pi^+ \rightarrow \pi^+\pi^-\pi^0) = (-1.0 \pm 1.7)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(1450)^+\pi^- \rightarrow \pi^+\pi^-\pi^0) = (0 \pm 70)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(1450)^0\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (-20 \pm 40)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(1450)^-\pi^+ \rightarrow \pi^+\pi^-\pi^0) = (6 \pm 9)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(1700)^+\pi^- \rightarrow \pi^+\pi^-\pi^0) = (-5 \pm 14)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(1700)^0\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (13 \pm 9)\% \text{ [tt]}$$
+
+$$A_{CP}(\rho(1700)^-\pi^+ \rightarrow \pi^+\pi^-\pi^0) = (8 \pm 11)\% \text{ [tt]}$$
+
+$$A_{CP}(f_0(980)\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (0 \pm 35)\% \text{ [tt]}$$
+
+$$A_{CP}(f_0(1370)\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (25 \pm 18)\% \text{ [tt]}$$
+
+$$A_{CP}(f_0(1500)\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (0 \pm 18)\% \text{ [tt]}$$
+
+$$A_{CP}(f_0(1710)\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (0 \pm 24)\% \text{ [tt]}$$
+
+$$A_{CP}(f_2(1270)\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (-4 \pm 6)\% \text{ [tt]}$$
+
+$$A_{CP}(\sigma(400)\pi^0 \rightarrow \pi^+\pi^-\pi^0) = (6 \pm 8)\% \text{ [tt]}$$
+
+$$A_{CP}(\text{nonresonant } \pi^+\pi^-\pi^0) = (-13 \pm 23)\% \text{ [tt]}$$
+
+$$A_{CP}(a_1(1260)^+\pi^- \rightarrow 2\pi^+2\pi^-) = (5 \pm 6)\%$$
+
+$$A_{CP}(a_1(1260)^-\pi^- \rightarrow 2\pi^+2\pi^-) = (14 \pm 18)\%$$
+
+$$A_{CP}(\pi(1300)^+\pi^- \rightarrow 2\pi^+2\pi^-) = (-2 \pm 15)\%$$
+
+$$A_{CP}(\pi(1300)^-\pi^- \rightarrow 2\pi^+2\pi^-) = (-6 \pm 30)\%$$
+
+$$A_{CP}(a_1(1640)^+\pi^- \rightarrow 2\pi^+2\pi^-) = (9 \pm 26)\%$$
+
+$$A_{CP}(\pi_2(1670)^+\pi^- \rightarrow 2\pi^+2\pi^-) = (7 \pm 18)\%$$
+
+$$A_{CP}(\sigma f_0(1370) \rightarrow 2\pi^+2\pi^-) = (-15 \pm 19)\%$$
+
+$$A_{CP}(\sigma\rho(770)^0 \rightarrow 2\pi^+2\pi^-) = (3 \pm 27)\%$$
+
+$$A_{CP}(2\rho(770)^0 \rightarrow 2\pi^+2\pi^-) = (-6 \pm 6)\%$$
+
+$$A_{CP}(2f_2(1270) \rightarrow 2\pi^+2\pi^-) = (-28 \pm 24)\%$$
+
+$$A_{CP}(K^{+}K^{-}\pi^{0}) = (-1.0 \pm 1.7)\%$$
+
+$$A_{CP}(K^{*}(892)^+K^- \rightarrow K^{+}K^{-}\pi^{0}) = (-0.9 \pm 1.3)\% \text{ [tt]}$$
+
+$$A_{CP}(K^{*}(1410)^+K^- \rightarrow K^{+}K^{-}\pi^{0}) = (-21 \pm 24)\% \text{ [tt]}$$
+
+$$A_{CP}((K^{+}\pi^{0})S_{-wave}K^{-} \rightarrow K^{+}K^{-}\pi^{0}) = (7 \pm 15)\% \text{ [tt]}$$
+
+$$A_{CP}(\phi(1020)\pi^{0} \rightarrow K^{+}K^{-}\pi^{0}) = (1.1 \pm 2.2)\% \text{ [tt]}$$
+
+$$A_{CP}(f_0(980)\pi^{0} \rightarrow K^{+}K^{-}\pi^{0}) = (-3 \pm 19)\% \text{ [tt]}$$
+
+$$A_{CP}(a_0(980)^{0}\pi^{0} \rightarrow K^{+}K^{-}\pi^{0}) = (-5 \pm 16)\% \text{ [tt]}$$
+
+$$A_{CP}(t'_2(1525)\pi^{0} \rightarrow K^{+}K^{-}\pi^{0}) = (0 \pm 160)\% \text{ [tt]}$$
+
+$$A_{CP}(K^{*}(892)^-K^{+} \rightarrow K^{+}K^{-}\pi^{0}) = (-5 \pm 4)\% \text{ [tt]}$$
+
+$$A_{CP}(K^{*}(1410)^-K^{+} \rightarrow K^{+}K^{-}\pi^{0}) = (-17 \pm 29)\% \text{ [tt]}$$
+
+$$A_{CP}((K^{-}\pi^{0})S_{-wave}K^{+} \rightarrow K^{+}K^{-}\pi^{0}) = (-10 \pm 40)\% \text{ [tt]}$$
+
+$$A_{CP}(K_S^{\oplus}\pi^0) = (-0.20 \pm 0.17)\%$$
+
+$$A_{CP}(K_S^{\ominus}\eta) = (0.5 \pm 0.5)\%$$
+
+$$A_{CP}(K_S^{\oplus}\eta') = (1.0 \pm 0.7)\%$$
+
+$$A_{CP}(K_S^{\ominus}\phi) = (-3 \pm 9)\%$$
+
+$$A_{CP}(K^{-}\pi^{+}) = (0.2 \pm 0.5)\%$$
+
+$$A_{CP}(K^{+}\pi^{-}) = (-0.9 \pm 1.4)\%$$
+
+$$A_{CP}(D_{CP}(\pm 1) \rightarrow K^{\mp}\pi^{\pm}) = (12.7 \pm 1.5)\%$$
+
+$$A_{CP}(K^{-}\pi^{+}\pi^{0}) = (0.1 \pm 0.5)\%$$
+
+$$A_{CP}(K^{+}\pi^{-}\pi^{0}) = (0 \pm 5)\%$$
+
+$$A_{CP}(K_S^{\oplus}\pi^{+}\pi^{-}) = (-0.1 \pm 0.8)\%$$
+
+$$A_{CP}(K^{*}(892)^{-}\pi^{+} \rightarrow K_S^{\oplus}\pi^{+}\pi^{-}) = (0.4 \pm 0.5)\%$$
+
+$$A_{CP}(K^{*}(892)^{+}\pi^{-} \rightarrow K_S^{\oplus}\pi^{+}\pi^{-}) = (1 \pm 6)\%$$
+
+$$A_{CP}(\bar{K}^{0}\rho^{0} \rightarrow K_S^{\oplus}\pi^{+}\pi^{-}) = (-0.1 \pm 0.5)\%$$
+---PAGE_BREAK---
+
+$$A_{CP}(\bar{K}^0 \omega \rightarrow K_S^0 \pi^+ \pi^-) = (-13 \pm 7)\%$$
+
+$$A_{CP}(\bar{K}^0 f_0(980) \rightarrow K_S^0 \pi^+ \pi^-) = (-0.4 \pm 2.7)\%$$
+
+$$A_{CP}(\bar{K}^0 f_2(1270) \rightarrow K_S^0 \pi^+ \pi^-) = (-4 \pm 5)\%$$
+
+$$A_{CP}(\bar{K}^0 f_0(1370) \rightarrow K_S^0 \pi^+ \pi^-) = (-1 \pm 9)\%$$
+
+$$A_{CP}(\bar{K}^0 \rho^0(1450) \rightarrow K_S^0 \pi^+ \pi^-) = (-4 \pm 10)\%$$
+
+$$A_{CP}(\bar{K}^0 f_0(600) \rightarrow K_S^0 \pi^+ \pi^-) = (-3 \pm 5)\%$$
+
+$$A_{CP}(K^{*}(1410)^{-}\pi^{+} \rightarrow K_S^{0}\pi^{+}\pi^{-}) = (-2 \pm 9)\%$$
+
+$$A_{CP}(K_0^*(1430)^{-}\pi^{+} \rightarrow K_S^0\pi^{+}\pi^{-}) = (4 \pm 4)\%$$
+
+$$A_{CP}(K_0^*(1430)^{+}\pi^{-} \rightarrow K_S^0\pi^{+}\pi^{-}) = (12 \pm 15)\%$$
+
+$$A_{CP}(K_2^*(1430)^{-}\pi^{+} \rightarrow K_S^0\pi^{+}\pi^{-}) = (3 \pm 6)\%$$
+
+$$A_{CP}(K_2^*(1430)^{+}\pi^{-} \rightarrow K_S^0\pi^{+}\pi^{-}) = (-10 \pm 32)\%$$
+
+$$A_{CP}(K^{-}\pi^{+}\pi^{+}\pi^{-}) = (0.2 \pm 0.5)\%$$
+
+$$A_{CP}(K^{+}\pi^{-}\pi^{+}\pi^{-}) = (-2 \pm 4)\%$$
+
+$$A_{CP}(K^{+}K^{-}\pi^{+}\pi^{-}) = (1.3 \pm 1.7)\%$$
+
+$$A_{CP}(K_1^*(1270)^{+}K^{-} \rightarrow K^{+}K^{-}\pi^{+}\pi^{-}) = (-2.3 \pm 1.7)\%$$
+
+$$A_{CP}(K_1^*(1270)^{+}K^{-} \rightarrow K^{*0}\pi^{+}K^{-}) = (-1 \pm 10)\%$$
+
+$$A_{CP}(K_1^*(1270)^{-}K^{+} \rightarrow \bar{K}^{*0}\pi^{-}K^{+}) = (-10 \pm 32)\%$$
+
+$$A_{CP}(K_1^*(1270)^{-}K^{+} \rightarrow K^{+}K^{-}\pi^{+}\pi^{-}) = (1.7 \pm 3.5)\%$$
+
+$$A_{CP}(K_1^*(1270)^{+}K^{-} \rightarrow \rho^{0}K^{+}K^{-}) = (-7 \pm 17)\%$$
+
+$$A_{CP}(K_1^*(1270)^{-}K^{+} \rightarrow \rho^{0}K^{-}K^{+}) = (10 \pm 13)\%$$
+
+$$A_{CP}(K_1(1400)^{+}K^{-} \rightarrow K^{+}K^{-}\pi^{+}\pi^{-}) = (-4.4 \pm 2.1)\%$$
+
+$$A_{CP}(K^{*}(1410)^{+}K^{-} \rightarrow K^{*0}\pi^{+}K^{-}) = (-20 \pm 17)\%$$
+
+$$A_{CP}(K^{*}(1410)^{-}K^{+} \rightarrow \bar{K}^{*0}\pi^{-}K^{+}) = (-1 \pm 14)\%$$
+
+$$A_{CP}(K^{*}(1680)^{+}K^{-} \rightarrow K^{+}K^{-}\pi^{+}\pi^{-}) = (-17 \pm 29)\%$$
+
+$$A_{CP}(K^{*0}\bar{K}^{*0}) \text{ in } D^0, \bar{D}^0 \rightarrow K^{*0}\bar{K}^{*0} = (-5 \pm 14)\%$$
+
+$$A_{CP}(K^{*0}\bar{K}^{*0}) \text{ S-wave}) = (-3.9 \pm 2.2)\%$$
+
+$$A_{CP}(\phi\rho^0) \text{ in } D^0, \bar{D}^0 \rightarrow \phi\rho^0 = (1 \pm 9)\%$$
+
+$$A_{CP}(\phi\rho^0) \text{ S-wave}) = (-3 \pm 5)\%$$
+
+$$A_{CP}(\phi\rho^0) \text{ D-wave}) = (-37 \pm 19)\%$$
+
+$$A_{CP}(\phi(\pi^{+}\pi^{-})S-wave) = (6 \pm 6)\%$$
+
+$$A_{CP}(K^{*}(892)^{0}(K^{-}\pi^{+})S-wave) = (-10 \pm 40)\%$$
+
+$$A_{CP}(K^{+}K^{-}\pi^{+}\pi^{-}\text{non-resonant}) = (8 \pm 20)\%$$
+
+$$A_{CP}((K^{-}\pi^{+})P-wave)(K^{+}\pi^{-})S-wave) = (3 \pm 11)\%$$
+
+$$A_{CP}(K^{+}K^{-}\mu^{+}\mu^{-}) \text{ in } D^0, \bar{D}^0 \rightarrow K^{+}K^{-}\mu^{+}\mu^{-} = (0 \pm 11)\%$$
+
+$$A_{CP}(\pi^{+}\mu^{-}\mu^{+}\mu^{-}) \text{ in } D^0, \bar{D}^0 \rightarrow \pi^{+}\pi^{-}\mu^{+}\mu^{-} = (5 \pm 4)\%$$
+
+### CP-even fractions (labeled by the $D^0$ decay)
+
+CP-even fraction in $D^0 \rightarrow \pi^+\pi^-\pi^0$ decays = $(97.3 \pm 1.7)\%$
+
+CP-even fraction in $D^0 \rightarrow K^+K^-\pi^0$ decays = $(73 \pm 6)\%$
+
+CP-even fraction in $D^0 \rightarrow \pi^+\pi^-\pi^+\pi^-$ decays = $(76.9 \pm 2.3)\%$
+
+CP-even fraction in $D^0 \rightarrow K_S^0\pi^+\pi^-\pi^0$ decays = $(23.8 \pm 1.7)\%$
+
+CP-even fraction in $D^0 \rightarrow K^+K^-\pi^+\pi^-$ decays = $(75 \pm 4)\%$
+
+### CP-violation asymmetry difference
+
+$\Delta A_{CP} = A_{CP}(K^+ K^-) - A_{CP}(\pi^+ \pi^-) = (-0.154 \pm 0.029)\%$
+
+### $\chi^2$ tests of CP-violation (CPV) p-values
+
+Local CPV in $D^0, \bar{D}^0 \rightarrow \pi^+\pi^-\pi^0 = 4.9\%$
+
+Local CPV in $D^0, \bar{D}^0 \rightarrow \pi^+\pi^-\pi^+\pi^- = (0.6 \pm 0.2)\%$
+
+Local CPV in $D^0, \bar{D}^0 \rightarrow K_S^0\pi^+\pi^- = 96\%$
+
+Local CPV in $D^0, \bar{D}^0 \rightarrow K^+K^-\\ -\pi^0 = 16.6\%$
+
+Local CPV in $D^0, \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0 \\ -\bar{D}^0\\}$
+---PAGE_BREAK---
+
+**T-violation decay-rate asymmetry**
+
+$$A_T(K^+ K^- \pi^+ \pi^-) = (2.9 \pm 2.2) \times 10^{-3} [{\rm{MeV}}]$$
+
+$$A_{T\text{viol}}(K_S \pi^+ \pi^- \pi^0) \text{ in } D^0, \bar{D}^0 \rightarrow K_S \pi^+ \pi^- \pi^0 = (-0.3^{+1.4}_{-1.6}) \times 10^{-3}$$
+
+**CPT-violation decay-rate asymmetry**
+
+$$A_{CPT}(K^{\mp}\pi^{\pm}) = 0.008 \pm 0.008$$
+
+**Form factors**
+
+$$r_V \equiv V(0)/A_1(0) \text{ in } D^0 \rightarrow K^*(892)^-\ell^+\nu_\ell = 1.46 \pm 0.07$$
+
+$$r_2 \equiv A_2(0)/A_1(0) \text{ in } D^0 \rightarrow K^*(892)^-\ell^+\nu_\ell = 0.68 \pm 0.06$$
+
+$$f_+(0) \text{ in } D^0 \rightarrow K^- \ell^+ \nu_\ell = 0.736 \pm 0.004$$
+
+$$f_+(0)|V_{cs}| \text{ in } D^0 \rightarrow K^- \ell^+ \nu_\ell = 0.7166 \pm 0.0030$$
+
+$$r_1 \equiv a_1/a_0 \text{ in } D^0 \rightarrow K^- \ell^+ \nu_\ell = -2.40 \pm 0.16$$
+
+$$r_2 \equiv a_2/a_0 \text{ in } D^0 \rightarrow K^- \ell^+ \nu_\ell = 5 \pm 4$$
+
+$$f_+(0) \text{ in } D^0 \rightarrow \pi^- \ell^+ \nu_\ell = 0.637 \pm 0.009$$
+
+$$f_+(0)|V_{cd}| \text{ in } D^0 \rightarrow \pi^- \ell^+ \nu_\ell = 0.1436 \pm 0.0026 \quad (S = 1.5)$$
+
+$$r_1 \equiv a_1/a_0 \text{ in } D^0 \rightarrow \pi^- \ell^+ \nu_\ell = -1.97 \pm 0.28 \quad (S = 1.4)$$
+
+$$r_2 \equiv a_1/a_0 \text{ in } D^0 \rightarrow \pi^- \ell^+ \nu_\ell = -0.2 \pm 2.2 \quad (S = 1.7)$$
+
+Most decay modes (other than the semileptonic modes) that involve a neutral $K$ meson are now given as $K_S^0$ modes, not as $\bar{K}^0$ modes. Nearly always it is a $K_S^0$ that is measured, and interference between Cabibbo-allowed and doubly Cabibbo-suppressed modes can invalidate the assumption that $2\Gamma(K_S^0) = \Gamma(\bar{K}^0)$.
+
+| D0 DECAY MODES | Fraction (Γf/Γ) | Scale factor/ p
Confidence level(MeV/c) |
|---|
| Topological modes | | 0-prongs | [uu] (15 ± 6 )% | - | | 2-prongs | (71 ± 6 )% | - | | 4-prongs | [vv] (14.6 ± 0.5 )% | - | | 6-prongs | [xx] (6.5 ± 1.3 ) × 10-4 | - | | Inclusive modes | | e+ anything | [yy] (6.49 ± 0.11 )% | - | | μ+ anything | (6.8 ± 0.6 )% | - | | K- anything | (54.7 ± 2.8 )% | S=1.3 | | K0 anything + K0 anything | (47 ± 4 )% | - | | K+ anything | (3.4 ± 0.4 )% | - | | K*(892)- anything | (15 ± 9 )% | - | | K*(892)0 anything | (9 ± 4 )% | - | | K*(892)+ anything | < 3.6 % | CL=90% | | K*(892)0 anything | (2.8 ± 1.3 )% | - | | η anything | (9.5 ± 0.9 )% | - | | η' anything | (2.48 ± 0.27 )% | - | | φ anything | (1.08 ± 0.04 )% | - | | invisibles | < 9.4 × 10-5 | CL=90% |
+
+Semileptonic modes| K- e+ νe | (3.542 ± 0.035) % | S=1.3 | 867 | | K- μ+ νμ | (3.41 ± 0.04) % | | 864 | | K*(892)- e+ νe | (2.15 ± 0.16) % | | 719 | | K*(892)- μ+ νμ | (1.89 ± 0.24) % | | 714 | | K- π0 e+ νe | (1.6 +1.3-0.5) % | | 861 |
+---PAGE_BREAK---
+
+| K0π-e+νe | ( 1.44 ± 0.04 ) % | 860 | | (ℍ0π-)S-wavee+νe | ( 7.9 ± 1.7 ) × 10-4 | 860 | | K-π+π-e+νe | ( 2.8 + 1.4- 1.1 ) × 10-4 | 843 | | K1(1270)-e+νe | ( 7.6 + 4.0- 3.1 ) × 10-4 | 511 | | K-π+π-μ+νμ | < 1.3 | CL=90% | 821 | | (ℍ*(892)π-)S-waveμ+νμ | < 1.5 | CL=90% | 692 | | π-e+νe | ( 2.91 ± 0.04 ) × 10-3 | 927 | | π-μ+νμ | ( 2.67 ± 0.12 ) × 10-3 | S=1.3 | 924 | | π-π0e+νe | ( 1.45 ± 0.07 ) × 10-3 | 922 | | ρ-e+νe | ( 1.50 ± 0.12 ) × 10-3 | S=1.9 | 771 | | a(980)-e+νe, a- → ηπ- | ( 1.33 + 0.34- 0.30 ) × 10-4 | - |
+
+Hadronic modes with one K
+
+
+
+
+ | K-π+ |
+ ( 3.950±0.031) % |
+ S=1.2 |
+ 861 |
+
+
+ | KS0π0 |
+ ( 1.240±0.022) % |
+ |
+ 860 |
+
+
+ | KS0π0 |
+ (10.0 ± 0.7) × 10-3 |
+ |
+ 860 |
+
+
+ | KS0π+π- |
+ [nn] (2.80 ± 0.18) % |
+ S=1.1 |
+ 842 |
+
+
+ | KS0ρ0 |
+ ( 6.3 + 0.6- 0.8 ) × 10-3 |
+ |
+ 674 |
+
+
+ | KS0ω, ω → π+π- |
+ ( 2.0 ± 0.6 ) × 10-4 |
+ |
+ 670 |
+
+
+ | KS(π+π-)S-wave |
+ ( 3.3 ± 0.8 ) × 10-3 |
+ |
+ 842 |
+
+
+ | KS0f0(980), f0 → π+π- |
+ ( 1.20 + 0.40- 0.23 ) × 10-3 |
+ |
+ 549 |
+
+
+ | KS0f0(1370), f0 → π+π- |
+ ( 2.8 + 0.9- 1.3 ) × 10-3 |
+ |
+ † |
+
+
+ | KS0f2(1270), f2 → π+π- |
+ ( 9 +10- 6 ) × 10-5 |
+ |
+ 262 |
+
+
+ | K*(892)-π+, K*- → |
+ ( 1.64 + 0.14- 0.17 ) % |
+ |
+ 711 |
+
+
+ | KS0π- |
+ |
+ |
+ |
+
+
+ | KS(1430)-π+, KS*- → |
+ ( 2.67 + 0.40 - 0.33 ) × 10-3 |
+ |
+ 378 |
+
+
+ | KS*-π- |
+ |
+ |
+ |
+
+
+ | KS(1430)-π+, KS*- → |
+ ( 3.4 + 1.9 - 1.0 ) × 10-4 |
+ |
+ 367 |
+
+
+ | KS*-π- |
+ |
+ |
+ |
+
+
+ | K*(1680)-π+, K*- → |
+ ( 4.4 ± 3.5 ) × 10-4 |
+ |
+ 46 |
+
+
+ | KS*-π- |
+ |
+ |
+ |
+
+
+ K*(892)+ π- , K*+ ( [zz] (1.13 + 0.60 - 0.34) × 10-4 ) %
+
+K*(1430)*+π-π+[zz]≤1.4×10-5
+
+K*(1430)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*(892)*+π-π+[zz]≤1.4×10-5
+
+K*
K*
K*
K*
K*
K*
K*
K*
+---PAGE_BREAK---
+
+
+
+
+ | K̅*0(1430)0π0, K̅*0 → K-π+ |
+ ( 5.9 ± 5.0 / − 1.6 ) × 10-3 |
+ 379 |
+
+
+ | K*(1680)-π+, K*- → |
+ ( 1.9 ± 0.7 ) × 10-3 |
+ 46 |
+
+
+ | K-π+π0 nonresonant |
+ ( 1.15 ± 0.60 / − 0.20 ) % |
+ 844 |
+
+
+ | K0S2π0 |
+ ( 9.1 ± 1.1 ) × 10-3 |
+ S=2.2 |
+
+
+ | K0S(2π0)S-wave |
+ ( 2.6 ± 0.7 ) × 10-3 |
+
+
+ | K̅*(892)0π0, K̅**0 → K0Sπ0 |
+ ( 8.1 ± 0.7 ) × 10-3 |
+
+
+ | K̅*(1430)0π0, K̅**0 → K0Sπ0 |
+ ( 4 ± 23 ) × 10-5 |
+
+
+ | K̅*(1680)0π0, K̅**0 → K0Sπ0 |
+ ( 1.0 ± 0.4 ) × 10-3 |
+
+
+ | K0Sf2(1270), f2 → 2π0 |
+ ( 2.3 ± 1.1 ) × 10-4 |
+ - |
+
+
+ | 2K0S, one K0S → 2π0 |
+ ( 3.2 ± 1.1 ) × 10-4 |
+ - |
+
+
+ | K-2π+π- |
+ [nn] ( 8.23 ± 0.14 ) % |
+ S=1.1 |
+
+
+ | K-π+ρ0total |
+ ( 6.87 ± 0.31 ) % |
+
+
+ | K-π+ρ03-body |
+ ( 6.1 ± 1.6 ) × 10-3 |
+
+
+ | K̅*(892)0ρ0, K̅**0 → |
+ ( 1.01 ± 0.05 ) % |
+
+
+ | K̅-π+ |
+ ( 1.2 ± 0.4 ) % |
+
+
+ | K̅*(892)0ρ0 transverse, K̅**0 → K-π+ |
+ ( 417) |
+
+
+ | K1a1(1260)+, a1+ → |
+ ( 4.33 ± 0.32 ) % |
+
+
+ | ρ0π+ |
+ ( 3.9 ± 0.4 ) × 10-3 |
+
+
+ | K1(1270)-π+, K1- → |
+ |
+ -848 |
+
+
+ | K-π+π-total |
+ ( 6.6 ± 2.3 ) × 10-4 |
+
+
+ | K1(1270)-π+, K1- → |
+ |
+ 484 |
+
+
+ | K̅*(892)0π-, K̅**0 → |
+ |
+
+
+ | K-2π-+π--nonresonant |
+ ( 1.81 ± 0.07 ) % |
+ 813 |
+
+
+ | KS0πS+πS-πS0 |
+ ( 5.2 ± 0.6 ) % |
+ 813 |
+
+
+ | KS0η, η → πS+πS-πS0 |
+ ( 1.17 ± 0.03 ) × 10-3 |
+ 772 |
+
+
+ | KS0ω, ω → πS+πS-πS0 |
+ ( 9.9 ± 0.6 ) × 10-3 |
+ 670 |
+
+
+ | K-π-+2π-0 |
+ ( 8.86 ± 0.23 ) % |
+ 815 |
+
+
+ | K-2π-+----⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π-⇌π
+
+ [aaa]
+
+
+
+
+
+
+ | K |
+
+ | 2π0 |
+ ( 8.26 ± 0.25 ) × 10-4 |
+ |
+ 923 |
+
+
+ | π+π-π- |
+ ( 1.49 ± 0.06 ) % |
+ S=2.1 |
+ 907 |
+
+
+ | ρ+π- |
+ ( 1.01 ± 0.04 ) % |
+ |
+ 764 |
+
+
+ | ρ0π0 |
+ ( 3.86 ± 0.23 ) × 10-3 |
+ |
+ 764 |
+
+
+ | ρ-π+ |
+ ( 5.15 ± 0.25 ) × 10-3 |
+ |
+ 764 |
+
+
+ | ρ(1450)+π-, ρ+ → π+π0 |
+ ( 1.6 ± 2.1 ) × 10-5 |
+ |
+ - |
+
+
+ | ρ(1450)0π0, ρ0 → π+π- |
+ ( 4.5 ± 2.0 ) × 10-5 |
+ |
+ - |
+
+
+ | ρ(1450)-π+, ρ- → π-π0 |
+ ( 2.7 ± 0.4 ) × 10-4 |
+ |
+ - |
+
+
+ | ρ(1700)+π-, ρ+ → π+π0 |
+ ( 6.1 ± 1.5 ) × 10-4 |
+ |
+ - |
+
+
+ | ρ(1700)0π0, ρ0 → π+π- |
+ ( 7.4 ± 1.8 ) × 10-4 |
+ |
+ - |
+
+
+ | ρ(1700)-π+, ρ- → π-π0 |
+ ( 4.8 ± 1.1 ) × 10-4 |
+ |
+ - |
+
+
+ | f₀(980)π0, f₀ → π+π- |
+ ( 3.7 ± 0.9 ) × 10-5 |
+ |
+ - |
+
+
+ | f₀(500)π0, f₀ → π+π- |
+ ( 1.22 ± 0.22 ) × 10-4 |
+ |
+ - |
+
+
+ | f₀(1370)π0, f₀ → π+π- |
+ ( 5.5 ± 2.1 ) × 10-5 |
+ |
+ - |
+
+
+ | f₀(1500)π0, f₀ → π+π- |
+ ( 5.8 ± 1.6 ) × 10-5 |
+ |
+ - |
+
+
+ | f₀(1710)π0, f₀ → π+π- |
+ ( 4.6 ± 1.6 ) × 10-5 |
+ |
+ - |
+
+
+ | f₂(1270)π0, f₂ → π+π- |
+ ( 1.97 ± 0.21 ) × 10-4 |
+ |
+ - |
+
+
+ | π+π-π- nonresonant |
+ ( 1.3 ± 0.4 ) × 10-4 |
+ 907 |
+
+
+ | 3π0 |
+ ( 2.0 ± 0.5 ) × 10-4 |
+ 908 |
+
+
+ | 2π+2π- |
+ ( 7.56 ± 0.20 ) × 10-3 |
+ 880 |
+
+
+ a₁(1260)i\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\-\\--i
total
2πi i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_i_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy__yy___
+ |
+
+
+---PAGE_BREAK---
+
+
+
+
+ | a1(1260)+π-, a1+ → |
+ ( 3.14 ± 0.21 ) × 10-3 |
+ - |
+
+
+ | ρ0π+S-wave |
+ |
+ |
+
+
+ | a1(1260)+π-, a1+ → |
+ ( 1.9 ± 0.5 ) × 10-4 |
+ - |
+
+
+ | ρ0π+D-wave |
+ |
+ |
+
+
+ | a1(1260)+π-, a1+ → σπ+ |
+ ( 6.4 ± 0.7 ) × 10-4 |
+ - |
+
+
+ | a1(1260)-π+, a1- → |
+ ( 2.3 ± 0.9 ) × 10-4 |
+ - |
+
+
+ | ρ0π-S-wave |
+ |
+ |
+
+
+ | a1(1260)-π+, a1- → σπ- |
+ ( 6.1 ± 3.4 ) × 10-5 |
+ - |
+
+
+ | π(1300)+π-, π(1300)+ → |
+ ( 5.1 ± 2.7 ) × 10-4 |
+ - |
+
+
+ | σπ+ |
+ |
+ |
+
+
+ | π(1300)-π+, π(1300)- → |
+ ( 2.3 ± 2.2 ) × 10-4 |
+ - |
+
+
+ | σπ- |
+ |
+ |
+
+
+ | a1(1640)+π-, a1+ → |
+ ( 3.2 ± 1.6 ) × 10-4 |
+ - |
+
+
+ | ρ0π+D-wave |
+ |
+ |
+
+
+ | a1(1640)+π-, a1+ → σπ+ |
+ ( 1.8 ± 1.4 ) × 10-4 |
+ - |
+
+
+ | π2(1670)+π-, π2+ → |
+ ( 2.0 ± 0.9 ) × 10-4 |
+ - |
+
+
+ | f2(1270)0π+, f20 → |
+ |
+ |
+
+
+ | π+π- |
+ |
+ |
+
+
+ | π2(1670)+π-, π2+ → σπ+ |
+ ( 2.6 ± 1.0 ) × 10-4 |
+ - |
+
+
+ | 2ρ0total |
+ ( 1.85 ± 0.13 ) × 10-3 |
+ 518 |
+
+
+ | 2ρ0, parallel helicities |
+ ( 8.3 ± 3.2 ) × 10-5 |
+ - |
+
+
+ | 2ρ0, perpendicular helicities |
+ ( 4.8 ± 0.6 ) × 10-4 |
+ - |
+
+
+ | 2ρ0, longitudinal helicities |
+ ( 1.27 ± 0.10 ) × 10-3 |
+ - |
+
+
+ | 2ρ(770)0, S-wave |
+ ( 1.8 ± 1.3 ) × 10-4 |
+ - |
+
+
+ | 2ρ(770)0, P-wave |
+ ( 5.3 ± 1.3 ) × 10-4 |
+ - |
+
+
+ | 2ρ(770)0, D-wave |
+ ( 6.2 ± 3.0 ) × 10-4 |
+ - |
+
+
+ | Resonant (π+π-)π+π- |
+ ( 1.51 ± 0.12 ) × 10-3 |
+ - |
+
+
+ | 3-body total |
+
+
+ | σπ+π- |
+ ( 6.2 ± 0.9 ) × 10-4 |
+ - |
+
+
+ | σρ(770)0 |
+ ( 5.0 ± 2.5 ) × 10-4 |
+ - |
+
+
+ | f0(980)π+π-, f0 → π+π- |
+ ( 1.8 ± 0.5 ) × 10-4 |
+ - |
+
+
+ | f2(1270)π+π-, f2 → |
+ ( 3.7 ± 0.6 ) × 10-4 |
+ - |
+
+
+ | π+π- |
+ |
+ |
+
+
+ | f2(1270), f2 → π+π- |
+ ( 1.6 ± 1.8 ) × 10-4 |
+ - |
+
+
+ | f0(1370)σ, f0 → π+π- |
+ ( 1.6 ± 0.5 ) × 10-3 |
+ - |
+
+
+ π+π-
2ππ0 | | ( 1.02 ± 0.09 ) % ( 882) | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | | |
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+
+
+
+
+
+ https://www.w3.org/TR/CSS2/prop-值-定义.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-定义
+ https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-defineurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-ink-converter-attribute.html#prop-value-eachurleachancequrisourceuri
+
+https://www.w3.org/TR/CSS2/properties-of-the-
+
+---PAGE_BREAK---
+
+
+
+
+ | KS0 K- π+ |
+ ( 3.3 ± 0.5 ) × 10-3 |
+ S=1.1 |
+ 739 |
+
+
+ | K̅*(892)0 KS0, K̅*0 → K-π+ |
+ ( 8.2 ± 1.6 ) × 10-5 |
+ 608 |
+
+
+ | K*(892)+ K-, K*+ → KS0π+ |
+ ( 1.89 ± 0.30 ) × 10-3 |
+ - |
+ - |
+
+
+ | K̅*(1410)0 KS0, K̅*0 → K-π+ |
+ ( 1.3 ± 1.9 ) × 10-4 |
+ - |
+ - |
+
+
+ | K*(1410)+ K-, K*+ → KS0π+ |
+ ( 3.2 ± 1.9 ) × 10-4 |
+ - |
+ - |
+
+
+ | (K-π+)S-wave KS0 |
+ ( 6.0 ± 2.9 ) × 10-4 |
+ 739 |
+ |
+
+
+ | (KS0π+)S-wave K- |
+ ( 3.9 ± 1.0 ) × 10-4 |
+
+
+ | a0(980)-π+, a0- → KS0K- |
+ ( 1.3 ± 1.4 ) × 10-4 |
+ - |
+ - |
+
+
+ | a0(1450)-π+, a0- → KS0K- |
+ ( 2.5 ± 2.0 ) × 10-5 |
+ - |
+ - |
+
+
+ | a2(1320)-π+, a2- → KS0K- |
+ ( 5 ± 5 ) × 10-6 |
+ - |
+ - |
+
+
+ | ρ(1450)-π+, ρ- → KS0K- |
+ ( 4.6 ± 2.5 ) × 10-5 |
+ - |
+ - |
+
+
+ | KS0 K+ π- |
+ ( 2.17 ± 0.34 ) × 10-3 |
+ S=1.1 |
+ 739 |
+
+
+ | K*(892)0 KS0, K*0 → K+π- |
+ ( 1.12 ± 0.21 ) × 10-4 |
+ 608 |
+
+
+ | K*(892)- K+, K*− → KS0π- |
+ ( 6.2 ± 1.0 ) × 10-4 |
+ - |
+ - |
+
+
+ | K*(1410)0 KS0, K*0 → K+π+ |
+ ( 5 ± 8 ) × 10-5 |
+ - |
+ - |
+
+
+ | K*(1410)- K+, K*− → KS0π- |
+ ( 2.6 ± 2.0 ) × 10-4 |
+ - |
+ - |
+
+
+ | (K+π-)S-wave KS0 |
+ ( 3.7 ± 1.9 ) × 10-4 |
+ 739 |
+ |
+
+
+ | (KS0π-)S-wave K+ |
+ ( 1.4 ± 0.6 ) × 10-4 |
+
+
+ | a0(980)+/-, a0+/-, a0+/- → KS0K+/- |
+ ( 6 ± 4 ) × 10-4 |
+ - |
+ - |
+
+
+ a0(1450)+/-, a0+/-, a0+/-, a0+/-/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, a0/±/K̅, aa_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2_2-/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+/-/+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,+,-,++-+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--+-+--%-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-&-∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓∓S=1.1
+| K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) | K* (895) |
|---|
+
+
+---PAGE_BREAK---
+
+
+
+
+ | K1(1270)+ K-, K1+ → |
+ ( 1.5 ± 0.5 ) × 10-4 |
+ - |
+
+
+ | K*(1430)0 π+, K*0 → |
+ |
+ |
+
+
+ | K+π- |
+ |
+ |
+
+
+ | K1(1270)+ K-, K1+ → ρ0 K+ |
+ ( 2.2 ± 0.6 ) × 10-4 |
+ - |
+
+
+ | K1(1270)+ K-, K1+ → |
+ ( 1.5 ± 1.2 ) × 10-5 |
+ - |
+
+
+ | ω(782) K+, ω → π+π- |
+ |
+ |
+
+
+ | K1(1270)- K+, K1- → ρ0 K- |
+ ( 1.3 ± 0.4 ) × 10-4 |
+ - |
+
+
+ | K1(1400)+ K-, K1+ → |
+ ( 4.6 ± 0.4 ) × 10-4 |
+ - |
+
+
+ | K*(892)0 π+, K*0 → |
+ |
+ |
+
+
+ | K+π- |
+ |
+ |
+
+
+ | K*(1410)- K+, K*- → |
+ ( 7.0 ± 1.1 ) × 10-5 |
+ - |
+
+
+ | K1(1680)+ K-, K1+ → |
+ ( 8.9 ± 3.2 ) × 10-5 |
+ - |
+
+
+ | K*0 π+, K*0 → K+π- |
+ |
+ |
+
+
+ | K+ K- π+ π- non-resonant |
+ ( 2.7 ± 0.6 ) × 10-4 |
+ - |
+
+
+ | 2KS0 π+ π- |
+ ( 1.22 ± 0.23 ) × 10-3 |
+ 673 |
+
+
+ | KS0 K- 2π+ π- |
+ < 1.4 × 10-4 |
+ CL=90% |
+
+
+ | K+ K- π+ π- πe0 |
+ ( 3.1 ± 2.0 ) × 10-3 |
+ 600 |
+
+
+
+
+Other $K\bar{K}X$ modes. They include all decay modes of the $\phi$, $\eta$, and $\omega$.
+
+| $\phi\pi^0$ | ( 1.17 ± 0.04 ) × 10⁻³ | 645 | | $\phi\eta$ | ( 1.8 ± 0.5 ) × 10⁻⁴ | 489 | | $\phi\omega$ | < 2.1 × 10⁻³ CL=90% | 238 |
+
+**Radiative modes**
+
+| $\rho^0\gamma$ | ( 1.82 ± 0.32 ) × 10⁻⁵ CL=90% | 771 | | $\omega\gamma$ | < 2.4 × 10⁻⁴ CL=90% | 768 | | $\phi\gamma$ | ( 2.81 ± 0.19 ) × 10⁻⁵ CL=95% | 654 | | $K^*(892)^0\gamma$ | ( 4.2 ± 0.7 ) × 10⁻⁴ CL=90% | 719 |
+
+**Doubly Cabibbo suppressed (DC) modes or $\Delta C = 2$ forbidden via mixing (C2M) modes**
+
+| K+ℓ-νℓ via D̄0 | < 2.2 × 10-5 | CL=90% | - |
|---|
| K+or K*(892)+e-νe via D̄0 | < 6 × 10-5 | CL=90% | - |
|---|
| K+π- | DC
( 1.50 ± 0.07 ) × 10-4 | S=3.0 | 861 |
|---|
K+π- via DCS
KS
KS
K*S
K*(892)S
K*(892)S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S
K*S) → D̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄̄
|
|---|
K*(892)s
K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩ | DC
( 1.364 ± 0.026 ) × 10⁻⁴
< 1.6 × 10⁻⁵ CL=95%<
< 1.8 × 10⁻⁴ CL=95%< | S=3.0
< | 861
< |
|---|
| K*(892)s♩♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩ | DC
( 1.13 + - 0.60
& - 0.34 ) × 10⁻⁴
< 1.4 × 10⁻⁵ CL=95%< | | |
|---|
| K*(892)s♩♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩ | DC
( 3.06 ± 0.15 ) × 10⁻⁴
( 7.6 + - 0.5
& - 0.6 ) × 10⁻⁴ CL=95%< | | |
|---|
| K*(892)s♩♩K*♩K*♩K*♩K*♩K*♩K*♩K*♩ | DC
( 2.49 ± 0.07 ) × 10⁻⁴
( 2.65 ± 0.06 ) × 10⁻⁴ CL=95%< | | |
|---|
| K*(892)s♩♩K*♩K*♩K*♩K*♩K*♩K*♩ | DC
( 7.9 ± 3.0 ) × 10⁻⁶
( - & + & - & + ) × 10⁻⁶ CL=95%< | | |
|---|
+
+
+
+
+ |
+ $\mu^{-}$ anything via $\overline{D}^{0}$
+ |
+
+ CL=90%
+ |
+
+ -
+ |
+
+
+ |
+ |
+
+
+ |
+ |
+
+
+ |
+ |
+
+
+
+
+
+---PAGE_BREAK---
+
+ΔC = 1 weak neutral current (C1) modes,
+Lepton Family number (LF) violating modes,
+Lepton (L) or Baryon (B) number violating modes
+
+
+
+
+ | γγ |
+ C1 |
+ < 8.5 |
+ × 10-7 |
+ CL=90% |
+ 932 |
+
+
+ | e+e- |
+ C1 |
+ < 7.9 |
+ × 10-8 |
+ CL=90% |
+ 932 |
+
+
+ | μ+ μ- |
+ C1 |
+ < 6.2 |
+ × 10-9 |
+ CL=90% |
+ 926 |
+
+
+ | π0 e+ e- |
+ C1 |
+ < 4 |
+ × 10-6 |
+ CL=90% |
+ 928 |
+
+
+ | π0 μ+ μ- |
+ C1 |
+ < 1.8 |
+ × 10-4 |
+ CL=90% |
+ 915 |
+
+
+ | η e+ e- |
+ C1 |
+ < 3 |
+ × 10-6 |
+ CL=90% |
+ 852 |
+
+
+ | η μ+ μ- |
+ C1 |
+ < 5.3 |
+ × 10-4 |
+ CL=90% |
+ 838 |
+
+
+ | π+ π- e+ e- |
+ C1 |
+ < 7 |
+ × 10-6 |
+ CL=90% |
+ 922 |
+
+
+ | ρ0 e+ e- |
+ C1 |
+ < 1.0 |
+ × 10-4 |
+ CL=90% |
+ 771 |
+
+
+ | π+ π- μ+ μ- |
+ C1 |
+ ( 9.6 ± 1.2 ) |
+ × 10-7 |
+ |
+ 894 |
+
+
+ | π+ π- μ+ μ- (non-res) |
+ |
+ < 5.5 |
+ × 10-7 |
+ CL=90% |
+ - |
+
+
+ | ρ0 μ+ μ- |
+ C1 |
+ < 2.2 |
+ × 10-5 |
+ CL=90% |
+ 754 |
+
+
+ | ω e+ e- |
+ C1 |
+ < 6 |
+ × 10-6 |
+ CL=90% |
+ 768 |
+
+
+ | ω μ+ μ- |
+ C1 |
+ < 8.3 |
+ × 10-4 |
+ CL=90% |
+ 751 |
+
+
+ | K- K+ e+ e- |
+ C1 |
+ < 1.1 |
+ × 10-5 |
+ CL=90% |
+ 791 |
+
+
+ | φ e+ e- |
+ C1 |
+ < 5.2 |
+ × 10-5 |
+ CL=90% |
+ 654 |
+
+
+ | K- K+ μ+ μ- |
+ C1 |
+ ( 1.54 ± 0.32 ) |
+ × 10-7 |
+ |
+ 710 |
+
+
+ | K- K+ μ+ μ- (non-res) |
+ |
+ < 3.3 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | φ μ+ μ- |
+ C1 |
+ < 3.1 |
+ × 10-5 |
+ CL=90% |
+ 631 |
+
+
+ | K̅L*eL+eL- |
+ [ss] |
+ < 2.4 |
+ × 10-5 |
+ CL=90% |
+
+
+ | K̅L*μL+μL- |
+ [ss] |
+ < 2.6 |
+ × 10-4 |
+ CL=90% |
+
+
+ K̅L*πL+eL+e-
-675 <
meε<875 MeV
(non-res) |
+ [ss] |
+ ( 4.0 ± 0.5 ) |
+ × 10-6 |
+ CL=90% |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+|
| γγ | C1 | < 8.5 × 10⁻⁷ CL=90% | 932 |
|---|
| e⁺e⁻ C1 | < 7.9 × 10⁻⁸ CL=90% |
|---|
| μ⁺μ⁻ C1 | < 6.2 × 10⁻⁹ CL=90% | 926 |
|---|
| π⁰e⁺e⁻ C1 | < 4 × 10⁻⁶ CL=90% |
|---|
| π⁰μ⁺μ⁻ C1 | < 1.8 × 10⁻⁴ CL=90% | 915 |
|---|
| ηe⁺e⁻ C1 | < 3 × 10⁻⁶ CL=90% |
|---|
| ημ⁺μ⁻ C1 | < 5.3 × 10⁻⁴ CL=90% | 838 |
|---|
| π⁺π⁻e⁺e⁻ C1 | < 7 × 10⁻⁶ CL=90% |
|---|
| ρ⁰e⁺e⁻ C1 | < 1.0 × 10⁻⁴ CL=90% | 771 |
|---|
| π⁺π⁻μ⁺μ⁻ C1 (9.6 ± 1.2) × 10⁻⁷ CL=90% | < 5.5 × 10⁻⁷ CL=90% |
|---|
| π⁺π⁻μ⁺μ⁻(non-res) | C1 (2.2 × 10⁻⁵ CL=90%) - < 5.5 × 10⁻⁷ CL=90% | - |
|---|
| ρ⁰μ⁺μ⁻ C1 (6.6 × 10⁻⁵ CL=90%) - < 2.2 × 10⁻⁵ CL=90% | 754
768
751
791
654
710
- |
|---|
| ωe⁺e⁻ C1 (8.3 × 10⁻⁵ CL=90%) - < 6 × 10⁻⁶ CL=90% | - |
|---|
| ωμ⁺μ⁻ C1 (3.3 × 10⁻⁵ CL=90%) - < 8.3 × 10⁻⁶ CL=90% | - |
|---|
| K⁻K⁺e⁺e⁻ C1 (3.5 × 10⁻⁵ CL=90%) - < 3.3 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻ C1 (4.7 × 10⁻⁵ CL=90%) - < 3.3 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.5 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.7 × 10⁻⁵ CL=90%) - < 3.5 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% | - |
|---|
| K⁻K⁺μ⁺μ⁻(non-res) | C1 (4.4 × 10⁻⁵ CL=90%) - < 3.4 × 10⁻⁵ CL=90% |
|---|
+
+
+
+
+γγ
+
+
+γγ
+
+
+---PAGE_BREAK---
+
+| pe- | L,B [ccc] < 1.0 | x 10-5 | CL=90% | 696 | | p̄e+ | L,B [ddd] < 1.1 | x 10-5 | CL=90% | 696 |
+
+### D*(2007)⁰
+
+$$I(J^P) = \frac{1}{2}(1^-)$$
+
+$I, J, P$ need confirmation.
+
+Mass $m = 2006.85 \pm 0.05$ MeV (S = 1.1)
+
+$m_{D^{*0}} - m_{D^0} = 142.014 \pm 0.030$ MeV (S = 1.5)
+
+Full width $\Gamma < 2.1$ MeV, CL = 90%
+
+$\bar{D}^*(2007)^0$ modes are charge conjugates of modes below.
+
+| D*(2007)0 DECAY MODES | Fraction (Γf/Γ) | p (MeV/c) |
|---|
| D0π- | (64.7±0.9) % | 43 | | D0γ | (35.3±0.9) % | 137 |
+
+### D*(2010)±
+
+$$I(J^P) = \frac{1}{2}(1^-)$$
+
+$I, J, P$ need confirmation.
+
+Mass $m = 2010.26 \pm 0.05$ MeV
+
+$m_{D^{*}(2010)^+} - m_{D^+} = 140.603 \pm 0.015$ MeV
+
+$m_{D^{*}(2010)^+} - m_{D^0} = 145.4257 \pm 0.0017$ MeV
+
+Full width $\Gamma = 83.4 \pm 1.8$ keV
+
+$D^{*}(2010)^-$ modes are charge conjugates of the modes below.
+
+| D*(2010)± DECAY MODES | Fraction (Γf/Γ) | p (MeV/c) |
|---|
| D0π+ | (67.7±0.5) % | 39 | | D+π0 | (30.7±0.5) % | 38 | | D+γ | (1.6±0.4) % | 136 |
+
+### D0**(2300)0
+
+$$I(J^P) = \frac{1}{2}(0^+)$$
+
+was $D_0^*(2400)^0$
+
+Mass $m = 2300 \pm 19$ MeV
+
+Full width $\Gamma = 274 \pm 40$ MeV
+
+### D1(2420)0
+
+$$I(J^P) = \frac{1}{2}(1^+)$$
+
+Mass $m = 2420.8 \pm 0.5$ MeV (S = 1.3)
+
+$m_{D_1^0} - m_{D^{*+}} = 410.6 \pm 0.5$ MeV (S = 1.3)
+
+Full width $\Gamma = 31.7 \pm 2.5$ MeV (S = 3.5)
+
+### D2**(2460)0
+
+$$I(J^P) = \frac{1}{2}(2^+)$$
+
+$J^P = 2^+$ assignment strongly favored.
+
+Mass $m = 2460.7 \pm 0.4$ MeV (S = 3.1)
+
+$m_{D_2^*} - m_{D^+} = 591.0 \pm 0.4$ MeV (S = 2.9)
+
+$m_{D_2^*} - m_{D^{*+}} = 450.4 \pm 0.4$ MeV (S = 2.9)
+
+Full width $\Gamma = 47.5 \pm 1.1$ MeV (S = 1.8)
+---PAGE_BREAK---
+
+$$D_2^*(2460)^{\pm} \qquad I(J^P) = \frac{1}{2}(2^+)$$
+
+$J^P = 2^+$ assignment strongly favored.
+
+Mass $m = 2465.4 \pm 1.3$ MeV (S = 3.1)
+
+$m_{D_2^*(2460)\pm} - m_{D_2^*(2460)\ominus} = 2.4 \pm 1.7$ MeV
+
+Full width $\Gamma = 46.7 \pm 1.2$ MeV
+
+CHARMED, STRANGE MESONS
+(C = S = ±1)
+
+$D_s^+ = c\bar{s}, D_s^- = \bar{c}s$, similarly for $D_s^*$'s
+
+$$D_s^{\pm} \qquad I(J^P) = 0(0^-)$$
+
+Mass $m = 1968.34 \pm 0.07$ MeV
+
+$m_{D_s^{\pm}} - m_{D_s^{\mp}} = 98.69 \pm 0.05$ MeV
+
+Mean life $\tau = (504 \pm 4) \times 10^{-15}$ s (S = 1.2)
+
+$c\tau = 151.2~\mu\text{m}$
+
+CP-violating decay-rate asymmetries
+
+A$_{CP}(\mu^{\pm}\nu) = (5 \pm 6)\%$
+
+A$_{CP}(K^{\pm} K_S^0) = (0.09 \pm 0.26)\%$
+
+A$_{CP}(K^{\pm} K_L^0)$ in $D_s^+ \to K^{\pm} K_L^0 = (-1.1 \pm 2.7) \times 10^{-2}$
+
+A$_{CP}(K^+ K^- \pi^{\pm}) = (-0.5 \pm 0.9)\%$
+
+A$_{CP}(\phi\pi^{\pm}) = (-0.38 \pm 0.27)\%$
+
+A$_{CP}(K^{\pm} K_S^0 \pi^0) = (-2 \pm 6)\%$
+
+A$_{CP}(2K_S^0 \pi^{\pm}) = (3 \pm 5)\%$
+
+A$_{CP}(K^+ K^- \pi^{\pm}\pi^0) = (0.0 \pm 3.0)\%$
+
+A$_{CP}(K^{\pm} K_S^{0\pm} \pi^+\pi^-) = (-6 \pm 5)\%$
+
+A$_{CP}(K_S^0 K^{\mp} 2\pi^{\pm}) = (4.1 \pm 2.8)\%$
+
+A$_{CP}(\pi^+ \pi^- \pi^{\pm}) = (-0.7 \pm 3.1)\%$
+
+A$_{CP}(\pi^{\pm}\eta) = (1.1 \pm 3.1)\%$
+
+A$_{CP}(\pi^{\pm}\eta') = (-0.9 \pm 0.5)\%$
+
+A$_{CP}(\eta\pi^{\pm}\pi^0) = (-1 \pm 4)\%$
+
+A$_{CP}(\eta'\pi^{\pm}\pi^0) = (0 \pm 8)\%$
+
+A$_{CP}(K^{\pm}\pi^0) = (-27 \pm 24)\%$
+
+A$_{CP}(K_S^0 / K^0 \pi^{\pm}) = (0.4 \pm 0.5)\%$
+
+A$_{CP}(K_S^0 \pi^{\pm}) = (0.20 \pm 0.18)\%$
+
+A$_{CP}(K^{\pm}\pi^+\pi^-) = (4 \pm 5)\%$
+
+A$_{CP}(K^{\pm}\eta) = (9 \pm 15)\%$
+
+A$_{CP}(K^{\pm}\eta'(958)) = (6 \pm 19)\%$
+
+CP violating asymmetries of P-odd (T-odd) moments
+
+$A_T(K_S^0 K^\pm \pi^+\pi^-) = (-14 \pm 8) \times 10^{-3} [TeV]$
+
+$D_s^\dagger \rightarrow \phi l^\dagger v_\ell$ form factors
+
+$r_2 = 0.84 \pm 0.11$ (S = 2.4)
+
+$r_v = 1.80 \pm 0.08$
+
+$\Gamma_L/\Gamma_T = 0.72 \pm 0.18$
+---PAGE_BREAK---
+
+$$f_+(0) |V_{cs}| \text{ in } D_s^+ \rightarrow \eta e^+ \nu_e = 0.446 \pm 0.007$$
+
+$$f_+(0) |V_{cs}| \text{ in } D_s^+ \rightarrow \eta' e^+ \nu_e = 0.48 \pm 0.05$$
+
+CP violating asymmetries of P-odd (T-odd) moments
+
+$$f_+(0)|V_{cd}| \text{ in } D_s^+ \rightarrow K^0 e^+ \nu_e = 0.162 \pm 0.019$$
+
+$$r_v \equiv V(0)/A_1(0) \text{ in } D_s^+ \rightarrow K^*(892)^0 e^+ \nu_e = 1.7 \pm 0.4$$
+
+$$r_2 \equiv A_2(0)/A_1(0) \text{ in } D_s^+ \rightarrow K^*(892)^0 e^+ \nu_e = 0.77 \pm 0.29$$
+
+$$f_{D_s^+}^* |V_{cs}| \text{ in } D_s^+ \rightarrow \mu^+ \nu_\mu = 246 \pm 5 \text{ MeV}$$
+
+Unless otherwise noted, the branching fractions for modes with a resonance in the final state include all the decay modes of the resonance. $D_s^-$ modes are charge conjugates of the modes below.
+
+| Ds+ DECAY MODES | Fraction (Γf/Γ) | Scale factor/ Confidence level | p (MeV/c) |
|---|
| Inclusive modes | | e+ semileptonic | [eee] (6.5 ±0.4)% | | - | | π+ anything | (119.3 ±1.4)% | | - | | π- anything | (43.2 ±0.9)% | | - | | π0 anything | (123 ±7)% | | - | | K- anything | (18.7 ±0.5)% | | - | | K+ anything | (28.9 ±0.7)% | | - | | KS0 anything | (19.0 ±1.1)% | | - | | η anything | [fff] (29.9 ±2.8)% | | - | | ω anything | (6.1 ±1.4)% | | - | | η' anything | [ggg] (10.3 ±1.4)% | S=1.1 | - | | f0(980) anything, f0 → π+π- | < 1.3 % | CL=90% | - | | φ anything | (15.7 ±1.0)% | | - | | K+K- anything | (15.8 ±0.7)% | | - | | KS0K+ anything | (5.8 ±0.5)% | | - | | KS-K+ anything | (1.9 ±0.4)% | | - | | 2KS0 anything | (1.70±0.32)% | | - | | 2K+ anything | < 2.6 × 10-3 | CL=90% | - | | 2K- anything | < 6 × 10-4 | CL=90% | - | | Leptonic and semileptonic modes | | e+νe | < 8.3 × 10-5 | CL=90% | 984 | | μ+νμ | (5.49±0.16) × 10-3 | | 981 | | τ+ντ | (5.48±0.23)% | | 182 | | γe+νe | < 1.3 × 10-4 | CL=90% | 984 | | K+K-e+νe | — | | 851 | | φe+νe | [hhh] (2.39±0.16)% | S=1.3 | 720 | | φμ+νμ | (1.9 ±0.5)% | | 715 | | ηe+νe + η'(958)e+νe | [hhh] (3.03±0.24)% | | - | | ηe+νe | [hhh] (2.32±0.08)% | | 908 | | η'(958)e+νe | [hhh] (8.0 ±0.7)×10-3 | | 751 | | ημ+νμ | (2.4 ±0.5)% | | 905 | | η'(958)μ+νμ | (1.1 ±0.5)% | | 747 | | ωe+νe | [iii] < 2.0 × 10-3 | CL=90% | 829 | | K0e+νe | (3.4 ±0.4)×10-3 | | 921 | | K*(892)0e+νe | [hhh] (2.15±0.28)×10-3 | S=1.1 | 782 |
+
+Hadronic modes with a K$K\bar{\tau}$ pair
+
+$$K^{+} K_{S}^{0} \qquad (1.46 \pm 0.04) \% \qquad S=1.1$$
+
+$$K^{+} K_{L}^{0} \qquad (1.49 \pm 0.06) \%$$
+
+$$S=1.1$$
+
+$$S=1.1$$
+---PAGE_BREAK---
+
+
+
+
+ | K+ K̅0 |
+ ( 2.95±0.14 ) % |
+ |
+ 850 |
+
+
+ | K+ K-π+ |
+ [nn] ( 5.39±0.15 ) % |
+ S=1.2 |
+ 805 |
+
+
+ | φπ+ |
+ [hhh,jjj] ( 4.5 ± 0.4 ) % |
+ |
+ 712 |
+
+
+ | φπ+, φ → K+K- |
+ [iii] ( 2.24±0.08 ) % |
+ |
+ 712 |
+
+
+ | K+K*(892)0, K*0 → K-π+ |
+ ( 2.58±0.08 ) % |
+ |
+ 416 |
+
+
+ | f0(980)π+, f0 → K+K- |
+ ( 1.14±0.31 ) % |
+ |
+ 732 |
+
+
+ | f0(1370)π+, f0 → K+K- |
+ ( 7 ± 5 ) × 10-4 |
+ |
+ - |
+
+
+ | f0(1710)π+, f0 → K+K- |
+ ( 6.6 ± 2.8 ) × 10-4 |
+ |
+ 198 |
+
+
+ | K+K0(1430)0, K0- → K-π+ |
+ ( 1.8 ± 0.4 ) × 10-3 |
+ |
+ 218 |
+
+
+ | K+ KS0π0 |
+ ( 1.52±0.22 ) % |
+ |
+ 805 |
+
+
+ | 2KS0π+ |
+ ( 7.7 ± 0.6 ) × 10-3 |
+ |
+ 802 |
+
+
+ | K0K0π+ |
+ — |
+ |
+ 802 |
+
+
+ | K*(892)+K0 |
+ [hhh] ( 5.4 ± 1.2 ) % |
+ |
+ 683 |
+
+
+ | K+K-π+π0 |
+ ( 6.2 ± 0.6 ) % |
+ S=1.1 |
+ 748 |
+
+
+ | φρ+ |
+ [hhh] ( 8.4 +1.9-2.3 ) % |
+ |
+ 401 |
+
+
+ | KS0K-2π+ |
+ ( 1.65±0.10 ) % |
+ |
+ 744 |
+
+
+ | K*(892)+K*(892)0 |
+ ( 7.2 ± 2.6 ) % |
+ |
+ 417 |
+
+
+ | K+KS0π+π- |
+ ( 9.9 ± 0.8 ) × 10-3 |
+ |
+ 744 |
+
+
+ | K+K-2π+π- |
+ ( 8.6 ± 1.5 ) × 10-3 |
+ |
+ 673 |
+
+
+ | φ2π+π- |
+ [hhh] ( 1.21±0.16 ) % |
+ |
+ 640 |
+
+
+ | φρ0π+, φ → K+K- |
+ ( 6.5 ± 1.3 ) × 10-3 |
+ |
+ 181 |
+
+
+ | φa1(1260)+, φ → |
+ ( 7.4 ± 1.2 ) × 10-3 |
+ † |
+ |
+
+
+ | K+K-, a1+ → ρS0πS+ |
+ |
+ |
+ |
+
+
+ | φ2π+π- ( 1.8 ± 0.7 ) × 10-3 |
+ |
+ - |
+
+
+ | KS+KS-ρS0πS+—φ |
+ < 2.6 × 10-4 |
+ CL=90% |
+
+
+ | KS+KS-2πS+πS-—nonresonant |
+ ( 9 ± 7 ) × 10-4 |
+ 673 |
+
+
+ 2KSS̃S̃S̃S̃
ρS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πS̃S̃
πs --ν |
+
+
+
+
+
+
+ | Hadronic modes without K's |
+
+
+
+
+
+ | π⁺π⁻ |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
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+
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+
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+
+
+
+
+
+ D̅
D̄
(nonresonant)) |
+
+ DΣ
DΣ
&
ε
ε
ε
ε |
+
+ Dυ
Dυ
υ
υ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
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+ Dυ
Dυ |
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+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
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+ Dυ
Dυ |
+
+ Dυ
Dυ |
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+ Dυ
Dυ |
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+ Dυ
Dυ |
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+ Dυ
Dυ |
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+ Dυ
Dυ |
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+ Dυ
Dυ |
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+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ Dυ
Dυ |
+
+ D* (nonresonant)
+
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+
+ D* (nonresonant)
+---PAGE_BREAK---
+
+
+
+
+ | D̄2(2462)0π+ × B(D̄2*0 → D*(2010)-π+) |
+ ( 2.2 ± 1.1 ) × 10-4 |
+ - |
+
+
+ | D̄0(2400)0π+ × B(D̄0(2400)0 → D-π+) |
+ ( 6.4 ± 1.4 ) × 10-4 |
+ 2136 |
+
+
+ | D̄1(2421)0π+ × B(D̄1(2421)0 → D*-π+) |
+ ( 6.8 ± 1.5 ) × 10-4 |
+ - |
+
+
+ | D̄2(2462)0π+ × B(D̄2(2462)0 → D*-π+) |
+ ( 1.8 ± 0.5 ) × 10-4 |
+ - |
+
+
+ | D̄1(2427)0π+ × B(D̄1(2427)0 → D*-π+) |
+ ( 5.0 ± 1.2 ) × 10-4 |
+ - |
+
+
+ | D̄1(2420)0π+ × B(D̄10 → D*-π+, π-) |
+ < 6 |
+ × 10-6 |
+ CL=90% |
+ 2082 |
+
+
+ | D̄1(2420)*ρ+ |
+ < 1.4 |
+ × 10-3 |
+ CL=90% |
+ 1996 |
+
+
+ | D̄2(2460)*π+ |
+ < 1.3 |
+ × 10-3 |
+ CL=90% |
+ 2063 |
+
+
+ | D̄2(2460)*π+ × B(D̄2*0 → D*-π+, π-) |
+ < 2.2 |
+ × 10-5 |
+ CL=90% |
+ 2063 |
+
+
+ | D̄1(2680)*π+, D̄1(2680)* → D-π+ |
+ ( 8.4 ± 2.1 ) × 10-5 |
+ - |
+
+
+ | D̄3(2760)*π+, D̄3(2760)*π+ → D-π+ |
+ ( 1.00 ± 0.22 ) × 10-5 |
+ - |
+
+
+ | D̄2(3000)*π+, D̄2(3000)*π+ → D-π+ |
+ ( 2.0 ± 1.4 ) × 10-6 |
+ - |
+
+
+ | D̄s(2460)*ρ+ |
+ < 4.7 |
+ × 10-3 |
+ CL=90% |
+ 1977 |
+
+
+ | D̄s*D̄s* |
+ ( 9.0 ± 0.9 ) × 10-3 |
+ - |
+
+
+ | D̄s0(2317)*+D̄s0*, D̄s0* → D̄s*πs* |
+ ( 8.0 + 1.6 - 1.3 ) × 10-4 |
+ - |
+
+
+ | D̄s0(2317)*+D̄s0* × B(D̄s0(2317)*+ → D̄s*γ) |
+ < 7.6 |
+ × 10-4 |
+ CL=90% |
+ 1605
-1605 |
+
+
+ | D̄s0(2317)*+D̄s0*(2007)* × B(D̄s0(2317)*+ → D̄s*πs*) |
+ ( 9 ± 7 ) × 10-4 |
+ - |
+
+
+ D̄s,J(2457)*B(DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+ DsJ, (2457)
+\\[3mm]
+(D_{s,J}(2457)+ \bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar{\bar\\[8mm}
+\\[1.3cm]\pm]
+---PAGE_BREAK---
+
+
+
+
+ | D̅*(2007)0 Ds1(2536)+ × B(Ds1(2536)+ → D*(2007)0 K+) |
+ ( 5.5 ± 1.6 ) × 10-4 |
+ 1339 |
+
+
+ | D̅0 Ds1(2536)+×B(Ds1(2536)+ → D+K0) |
+ ( 2.3 ± 1.1 ) × 10-4 |
+ 1447 |
+
+
+ | D̅0 Ds,J(2700)+×B(Ds,J(2700)+ → D0K+) |
+ ( 5.6 ± 1.8 ) × 10-4 |
+ S=1.7 - |
+
+
+ | D̅*0 Ds1(2536)+, Ds1+ → D*+K0 |
+ ( 3.9 ± 2.6 ) × 10-4 |
+ 1339 |
+
+
+ | D̅0 Ds,J(2573)+, Ds,J+ → D0K+ |
+ ( 8 ± 15 ) × 10-6 |
+ - |
+
+
+ | D̅*0 Ds,J(2573), Ds,J+ → D0K+ |
+ < 2 |
+ CL=90% |
+
+
+ | D̅*(2007)0 Ds,J(2573), Ds,J+ → D0K+ |
+ < 5 |
+ CL=90% |
+
+
+ | D̅0Ds* |
+ ( 7.6 ± 1.6 ) × 10-3 |
+ 1734 |
+
+
+ | D̅*(2007)0Ds+ |
+ ( 8.2 ± 1.7 ) × 10-3 |
+ 1737 |
+
+
+ | D̅*(2007)0Ds* |
+ ( 1.71 ± 0.24 ) % |
+ 1651 |
+
+
+ | Ds(*)+D̅**0 |
+ ( 2.7 ± 1.2 ) % |
+ - |
+
+
+ | D̅*(2007)0D*(2010)+ |
+ ( 8.1 ± 1.7 ) × 10-4 |
+ 1713 |
+
+
+ | D̅0D*(2010)++D̅*(2007)0D+ |
+ < 1.30 % |
+ CL=90% |
+
+
+ | D̅0D*(2010)+ |
+ ( 3.9 ± 0.5 ) × 10-4 |
+ 1792 |
+
+
+ | D̅0D+ |
+ ( 3.8 ± 0.4 ) × 10-4 |
+ 1866 |
+
+
+ | D̅0D+K0 |
+ ( 1.55 ± 0.21 ) × 10-3 |
+ 1571 |
+
+
+ | D+D̅*(2007)0 |
+ ( 6.3 ± 1.7 ) × 10-4 |
+ 1791 |
+
+
+ | D̅*(2007)0D+K0 |
+ ( 2.1 ± 0.5 ) × 10-3 |
+ 1475 |
+
+
+ | D̅0D*(2010)+K0 |
+ ( 3.8 ± 0.4 ) × 10-3 |
+ 1476 |
+
+
+ | D̅*(2007)0D*(2010)+K0 |
+ ( 9.2 ± 1.2 ) × 10-3 |
+ 1362 |
+
+
+ | D̅0Ds+Ks*{K}{D+D*})K |
+ ( 1.45 ± 0.33 ) × 10-3{S=2.6 CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% CL=90% |
+
+
+ | Ds{πs}πs{πs}πs |
+ < 2.6 × 10-4{CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-CL-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L-C-C-L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_L_C_lmsn{d}{K}{D+D*})K |
+ < 2.6 × 10-4{schematized{a}{b}{c}{d}{e}{f} |
+ < 2.6 × 10-4{schematized{a}{b}{c}{d}{e}{f} |
+
+
+ | Dsη |
+ < 4 × 10-4{schematized{h}{i} |
+ < 4 × 10-4{schematized{h}{i} |
+
+
+ | Dsη |
+ < 6 × 10-4{schematized{j}{k} |
+ < 6 × 10-4{schematized{j}{k} |
+
+
+ | Dsρsm; |
+ < 3.8 × 10-4{schematized{n}{o} |
+ < 3.8 × 10-4{schematized{n}{o} |
+
+
+ | Dsr;ρsm; |
+ < 4 × 10-4{schematized{p}{q} |
+ < 4 × 10-4{schematized{p}{q} |
+
+
+ | Dsw;ρ |
+ < 4 × 10-4{schematized{s}{t} |
+ < 4 × 10-4{schematized{s}< 6 × 1×1××
< 6 × 1××
< 6 × 1×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 ×
< 6 × |
+
+
+ | D*sa₁(126)₁(126)₀(12)₀(1)₀(₁)₀(₂)₀(₃)₀(₄)₀(₅)₀(₆)₀(₇)₀(₈)₀(₉)₀(₁₀)₀(₁₁)₀(₁₂)₀(₁₃)₀(₁₄)₀(₁₅)₀(₁₆)₀(₁₇)₀(₁₈)₀(₁₉)₀(₂₀)₀(₂₁)₀(₂₂)₀(₂₃)₀(₂₄)₀(₂₅)₀(₂₆)₀(₂₇)₀(₂₈)₀(₂₉)₀(₃₀)₀(₃₁)₀(₃₂)₀(₃₃)₀(₃₄)₀(₃₅)₀(₃₆)₀(₃₇)₀(₃₈)₀(₃₉)₀(₄₀)₀(₄₁)₀(₄₂)₀(₄₃)₀(₄₄)₀(₄₅)₀(₄₆)₀(₄₇)₀(₄₈)₀(₄₉)₀(៥)⁰⁾K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾·K⁰⁾· |
+ Schemata for K⁰ and K¹: | |
+
+
+---PAGE_BREAK---
+
+
+
+
+ | DS*+ K*(892)0 |
+ < 3.5 |
+ × 10-4 |
+ CL=90% |
+ 2112 |
+
+
+ | DS- π+ K+ |
+ ( 1.80 ± 0.22 ) |
+ × 10-4 |
+ |
+ 2222 |
+
+
+ | DS- π+ K- |
+ ( 1.45 ± 0.24 ) |
+ × 10-4 |
+ |
+ 2164 |
+
+
+ | DS- π+ K*(892)+ |
+ < 5 |
+ × 10-3 |
+ CL=90% |
+ 2138 |
+
+
+ | DS- π+ K*(892)- |
+ < 7 |
+ × 10-3 |
+ CL=90% |
+ 2076 |
+
+
+ | DS- K+ K+ |
+ ( 9.7 ± 2.1 ) |
+ × 10-6 |
+ |
+ 2149 |
+
+
+ | DS*- K+ K+ |
+ < 1.5 |
+ × 10-5 |
+ CL=90% |
+ 2088 |
+
+
+ | Charmonium modes |
+
+
+ | ηc K+ |
+ ( 1.06 ± 0.09 ) |
+ × 10-3 |
+ S=1.2 |
+ 1751 |
+
+
+ | ηc K+, ηc → KS0K∓π± |
+ ( 2.7 ± 0.6 ) |
+ × 10-5 |
+ |
+ - |
+
+
+ | ηc K*(892)+ |
+ ( 1.1 ± 0.5
- 0.4 ) |
+ × 10-3 |
+ |
+ 1646 |
+
+
+ | ηc K+ π+ π- |
+ < 3.9 |
+ × 10-4 |
+ CL=90% |
+ 1684 |
+
+
+ | ηc K+ ω(782) |
+ < 5.3 |
+ × 10-4 |
+ CL=90% |
+ 1475 |
+
+
+ | ηc K+ η |
+ < 2.2 |
+ × 10-4 |
+ CL=90% |
+ 1588 |
+
+
+ | ηc K+π0 |
+ < 6.2 |
+ × 10-5 |
+ CL=90% |
+ 1723 |
+
+
+ | ηc(2S) K+ |
+ ( 4.4 ± 1.0 ) |
+ × 10-4 |
+ |
+ 1320 |
+
+
+ | S=1.1 |
+ ( 3.5 ± 0.8 ) |
+ × 10-8 |
+ |
+ - |
+
+
+ | ηc(2S) K+, ηc → KS0K∓π∓ |
+ ( 3.4 ± 2.3
- 1.6 ) |
+ × 10-6 |
+ |
+ - |
+
+
+ ηc(2S) K+, ηc → ppπsπs
ℏc(1P) K+, ℏc → J/ψπsπs
χc1(3872) K+ |
+ ( 1.12 ± 0.18 ) |
+ × 10-6 |
+ |
+ - |
+
+
+ χc1(3872) K+, χc1 → ppπ
χc1(3872) K+, χc1 → J/ψπsπ
χc1(3872) K+, χc1 → J/ψπ
χc1(3872) K+, χc1 → DSDπ
χc1(3872) K+, χc1 → DSDπ
χc1(3872) K+, χc1 → DSDπ
χc1(3872) K*, χc1
χc1(1P)
χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*, χc1(3872)K*π
+ ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × 10 | ( 4 ± 4 ) × 10 | ( 5 ± 0.4 ) × ( S=6, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, CL=96, GLYPH | |
+
+|
| D_s^*+K*(892)<^o> | <3.5 | x-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-^o-> |
|---|
| D_s^-K*(8)(+)^*+K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-K^-> |
|---|
| D_s^{*-}+N*(+)^*+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}+N^{*-}> |
|---|
| D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}-D_s^{-}> |
|---|
Charmonium modes
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁺ (S)
η_c K⁻ (S)ʵ Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = Sʵ = S#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#s_3#ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--ssr--sssr-srsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrsrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrrr-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r-r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_r_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_z_zzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzzppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppppprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprprpr prp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rrp rRPPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRPRRPPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPrPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPpPp_PPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPPSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSS
+Charmonium modes
ηc·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)·(S)— |
|---|
ηc·k†<<×××× ηc·k†<<×××× ηc·k†<<×××× ηc·k†<<×××× ηc·k†<<×××× ηc†<<××××
+
+
+
+
+ | D̅₃₄₅₆₇₈₉₄₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₀₄₅₆₇₈₉��ₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐₐ₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁₂₁十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二一十二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二二三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三三
+ |
+
+
+
+
+ Charmonium modes
ηc* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* + p* - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- -- --
+ |
+
+
+ ηc * → k * → π * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ * → ρ *→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→ρ→
+---PAGE_BREAK---
+
+
+
+
+ | χc1(3872)K*(892)+, χc1 → J/ψγ |
+ < 4.8 |
+ × 10-6 |
+ CL=90% |
+ 939 |
+
+
+ | χc1(3872)K*(892)+, χc1 → ψ(2S)γ |
+ < 2.8 |
+ × 10-5 |
+ CL=90% |
+ 939 |
+
+
+ | χc1(3872)+K0, χc1+ → J/ψ(1S)π+π0 |
+ [rr] < 6.1 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | χc1(3872)K0π+, χc1 → J/ψ(1S)π+π- |
+ ( 1.06 ± 0.31 ) |
+ × 10-5 |
+ - |
+ - |
+
+
+ | Zc(4430)+K0, Zc+ → J/ψπ+ |
+ < 1.5 |
+ × 10-5 |
+ CL=95% |
+ - |
+
+
+ | Zc(4430)+K0, Zc+ → ψ(2S)π+ |
+ < 4.7 |
+ × 10-5 |
+ CL=95% |
+ - |
+
+
+ | ψ(4260)0K+, ψ0 → J/ψπ+π- |
+ < 1.56 |
+ × 10-5 |
+ CL=95% |
+ - |
+
+
+ | X(3915)K+, X → J/ψγ |
+ < 1.4 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | X(3915)K+, X → χc1(1P)π0 |
+ < 3.8 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | X(3930)0K+, X0 → J/ψγ |
+ < 2.5 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | J/ψ(1S)K+ |
+ ( 1.006 ± 0.027 ) |
+ × 10-3 |
+ 1684 |
+
+
+ | J/ψ(1S)K0π+ |
+ ( 1.14 ± 0.11 ) |
+ × 10-3 |
+ 1651 |
+
+
+ | J/ψ(1S)K+π+π- |
+ ( 8.1 ± 1.3 ) |
+ × 10-4 |
+ S=2.5 |
+ 1612 |
+
+
+ | J/ψ(1S)K+K-K+ |
+ ( 3.37 ± 0.29 ) |
+ × 10-5 |
+ 1252 |
+
+
+ | X(3915)K+, X → pp |
+ < 7.1 |
+ × 10-8 |
+ CL=95% |
+ - |
+
+
+ | J/ψ(1S)K*(892)+ |
+ ( 1.43 ± 0.08 ) |
+ × 10-3 |
+ 1571 |
+
+
+ | J/ψ(1S)K(1270)+ |
+ ( 1.8 ± 0.5 ) |
+ × 10-3 |
+ 1402 |
+
+
+ | J/ψ(1S)K(1400)+ |
+ < 5 |
+ × 10-4 |
+ CL=90% |
+ 1308 |
+
+
+ | J/ψ(1S)ηK+ |
+ ( 1.24 ± 0.14 ) |
+ × 10-4 |
+ 1510 |
+
+
+ | χc1-odd(3872)K+, χc1-odd → J/ψη |
+ < 3.8 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | ψ(4160)K+, ψ → J/ψη |
+ < 7.4 |
+ × 10-6 |
+ CL=90% |
+
+
+ | J/ψ(1S)η'K+ |
+ < 8.8 |
+ × 10-5 |
+ CL=90% |
+
+
+ | J/ψ(1S)φK+ |
+ ( 5.0 ± 0.4 ) |
+ × 10-5 |
+ 1227 |
+
+
+ | J/ψ(1S)K1(1650), K1 → φK+ |
+ ( 6 ± 10/6 ) |
+ × 10-6 |
+ - |
+
+
+ | J/ψ(1S)K*(1680)+, K* → φK+ |
+ ( 3.4 ± 1.9/2.2 ) |
+ × 10-6 |
+ - |
+
+
+ | J/ψ(1S)K*₂(1980), K*₂ → φK+ |
+ ( 1.5 ± 0.9/0.5 ) |
+ × 10-6 |
+ - |
+
+
+ | J/ψ(1S)K(1830)+, K(1830)+ → φK+ |
+ ( 1.3 ± 1.3/1.1 ) |
+ × 10-6 |
+ - |
+
+
+ | χc1(4140)K+, χc1 → J/ψ(1S)φ |
+ ( 10 ± 4 ) |
+ × 10-6 |
+ - |
+
+
+ | χc1(4274)K+, χc1 → J/ψ(1S)φ |
+ ( 3.6 ± 2.2/1.8 ) |
+ × 10-6 |
+ - |
+
+
+ | χc0(4500)K+, χc0 → J/ψ(1S)φ |
+ ( 3.3 ± 2.1/1.7 ) |
+ × 10-6 |
+ - |
+
+
+ χc0(4700)K+, χc0
→ J/ψ(1S)φ
J/ψ(1S)ωK+ | | | | | χc1(3872)K+, χc1
→ J/ψω
X(3915)K+, X → J/ψω
J/ψ(1S)π+
J/ψ(1S)π+π+π-π-
J/ψ(1S)ρ+
J/ψ(1S)π+π⁰ nonresonant
J/ψ(1S)a₁(1260)
+ | | | | |
|---|
| | ( 3.20 ± 0.60/0.32 ) | × 10⁻⁴ | | 1388 |
|---|
| | ( 6.0 ± 2.2 ) | × 10⁻⁶ | | 1141 |
|---|
| | ( 3.0 ± 0.9/0.7 ) | × 10⁻⁵ | | 1103 |
|---|
| | ( 3.87 ± 0.11 ) | × 10⁻⁵ | | 1728 |
|---|
| | ( 1.16 ± 0.13 ) | × 10⁻⁵ | | 1635 |
|---|
| | ( 1.9 ± 0.4 ) | × 10⁻⁵ | | 1304 |
|---|
| | ( 4.1 ± 0.5 ) | × 10⁻⁵
S=1.4
CL=90% | | 1611
CL=90% |
|---|
| | < 7.3
< 1.2
+ CL=90% | × 10⁻⁶
× 10⁻³
CL=90% | &mathrm; CL=90% CL=90% |
|---|
+
+
+---PAGE_BREAK---
+
+| J/ψ(1S) ppπ+ | < 5.0 | × 10-7 | CL=90% | 643 | | J/ψ(1S) pΛ | ( 1.46 ± 0.12 ) | × 10-5 | | 567 | | J/ψ(1S) Σ0 p | < 1.1 | × 10-5 | CL=90% | — | | J/ψ(1S) D+ | < 1.2 | × 10-4 | CL=90% | 871 | | J/ψ(1S) D0 π+ | < 2.5 | × 10-5 | CL=90% | 665 | | ψ(2S) π+ | ( 2.44 ± 0.30 ) | × 10-5 | | 1347 | | ψ(2S) K+ | ( 6.19 ± 0.22 ) | × 10-4 | | 1284 | | ψ(2S) K*(892)+ | ( 6.7 ± 1.4 ) | × 10-4 | S=1.3 | 1116 | | ψ(2S) K+ππ- | ( 4.3 ± 0.5 ) | × 10-4 | | 1179 | | ψ(2S) φ(1020) K+ | ( 4.0 ± 0.7 ) | × 10-6 | | 417 | | ψ(3770) K+ | ( 4.9 ± 1.3 ) | × 10-4 | | 1218 | | ψ(3770) K+, ψ → D0 D0 | ( 1.5 ± 0.5 ) | × 10-4 | S=1.4 | 1218 | | ψ(3770) K+, ψ → D+ D- | ( 9.4 ± 3.5 ) | × 10-5 | | 1218 | | ψ(3770) K+, ψ → pp | < 2 | × 10-7 | CL=95% | — | | ψ(4040) K+ | < 1.3 | × 10-4 | CL=90% | 1003 | | ψ(4160) K+ | ( 5.1 ± 2.7 ) | × 10-4 | | 868 | | ψ(4160) K+, ψ → D0 D0 | ( 8 ± 5 ) | × 10-5 | | — | | χc0 π+, χc0 → π+ π- | < 1 | × 10-7 | CL=90% | 1531 | | χc0K+ | ( 1.50 + 0.15/- 0.13) | × 10-4 | | 1478 | | χc0K*(892)+ | < 2.1 | × 10-4 | CL=90% | 1341 | | χc1(1P) π+ | ( 2.2 ± 0.5 ) | × 10-5 | | 1468 | | χc1(1P) K+ | ( 4.85 ± 0.33 ) | × 10-4 | S=1.5 | 1412 | | χc1(1P) K*(892)+ | ( 3.0 ± 0.6 ) | × 10-4 | S=1.1 | 1265 | | χc1(1P) K0 π+ | ( 5.8 ± 0.4 ) | × 10-4 | | 1370 | | χc1(1P) K+ππ0 | ( 3.29 ± 0.35 ) | × 10-4 | | 1373 | | χc1(1P) K+π+π- | ( 3.74 ± 0.30 ) | × 10-4 | | 1319 | | χc1(2P) K+, χc1(2P) → π+π-χc1(1P) | < 1.1 | × 10-5 | CL=90% | — | | χc2K+ | ( 1.1 ± 0.4 ) | × 10-5 | | 1379 | | χc2K*, χc2 → ppπ+π- | < 1.9 | × 10-7 | | — | | χc2K*(892)+ | < 1.2 | × 10-4 | CL=90% | 1228 | <| χc2K0π- | ( 1.16 ± 0.25 ) | × 10-4 | | 1336 | | χc2K+ππ0 | < 6.2 × 10-5 |
|---|
| χc2K+π+π- | ( 1.34 ± 0.19 ) × 10-4 |
|---|
χc2(3930)π+, χc2→π+π-π |
+< 1 × 10-7 < 6.4 × 10-8 CL=95% |
+CL=90% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+CL=95% |
+K or K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
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K* modes
K* modes
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K* modes
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K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
K* modes
( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( ( (
Kc2Kc2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2 c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c2c3p-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-ccs-cscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscscsc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc sc SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SC SCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCCSCCSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSSsssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc
+ '[{"bbox": [3, -3, -8, -8], "category": "Picture"}, {"bbox": [3, -6, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": "Picture"}, {"bbox": [3, -8, -8, -7], "category": 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= −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√6/6 = −√−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−−>"}, {"bbox": [4.444444444444444e+14 / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / √(π / ∂>"}, {"bbox": [4.444444444444444e+14 * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π * π 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ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε ε α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α α β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β β βββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββββßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßßß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß ß >"}, {"bbox": [4.444444444444444e+14 + π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/π/\\
+\thead{\cmidrule{l}l}\end{thead}\tbody>\end{tbody}\end{table}"}, {"bbox": [4.444444444444444e+14 + τt/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/t/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g/g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g-g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_g_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_yy__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y__y___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy___yy_____
+\thead{\cmidrule{l}l}\end{thead}\tbody>\end{tbody}\end{table}"}, {"bbox": [4.444444444444444e+14 + τt_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t_t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t-t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t--t
+---PAGE_BREAK---
+
+
+
+
+ | η(1405) K+ × B(η(1405) → K*K) |
+ < 1.2 |
+ × 10-6 |
+ CL=90% |
+ 2425 |
+
+
+ | η(1475) K+ × B(η(1475) → K*K) |
+ ( 1.38 ± 0.21 / - 0.18 ) |
+ × 10-5 |
+ |
+ 2407 |
+
+
+ | f1(1285) K+ |
+ < 2.0 |
+ × 10-6 |
+ CL=90% |
+ 2458 |
+
+
+ | f1(1420) K+ × B(f1(1420) → ηππ) |
+ < 2.9 |
+ × 10-6 |
+ CL=90% |
+ 2420 |
+
+
+ | f1(1420) K+ × B(f1(1420) → K*K) |
+ < 4.1 |
+ × 10-6 |
+ CL=90% |
+ 2420 |
+
+
+ | φ(1680) K+ × B(φ(1680) → K*K) |
+ < 3.4 |
+ × 10-6 |
+ CL=90% |
+ 2344 |
+
+
+ | f0(1500) K+ |
+ ( 3.7 ± 2.2 ) |
+ × 10-6 |
+ |
+ 2398 |
+
+
+ | ωK+ |
+ ( 6.5 ± 0.4 ) |
+ × 10-6 |
+ |
+ 2558 |
+
+
+ | ωK*(892)+ |
+ < 7.4 |
+ × 10-6 |
+ CL=90% |
+ 2503 |
+
+
+ | ω(Kπ)0*+ |
+ ( 2.8 ± 0.4 ) |
+ × 10-5 |
+ |
+ - |
+
+
+ | ωK0*(1430)+ |
+ ( 2.4 ± 0.5 ) |
+ × 10-5 |
+ |
+ - |
+
+
+ | ωK2*(1430)+ |
+ ( 2.1 ± 0.4 ) |
+ × 10-5 |
+ |
+ 2379 |
+
+
+ | a0(980)+K0×B(a0(980)+ → ηπ+) |
+ < 3.9 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | a0(980)0K+×B(a0(980)0 → ηπ0) |
+ < 2.5 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | K*(892)0π+ |
+ ( 1.01 ± 0.08 ) |
+ × 10-5 |
+ |
+ 2562 |
+
+
+ | K*(892)+π0 |
+ ( 6.8 ± 0.9 ) |
+ × 10-6 |
+ |
+ 2563 |
+
+
+ | K+π-π- |
+ ( 5.10 ± 0.29 ) |
+ × 10-5 |
+ |
+ 2609 |
+
+
+ | K+π-π- nonresonant |
+ ( 1.63 ± 0.21 / - 0.15 ) |
+ × 10-5 |
+ |
+ 2609 |
+
+
+ | ω(782) K+ |
+ ( 6 ± 9 ) |
+ × 10-6 |
+ |
+ 2558 |
+
+
+ | K+f0(980) × B(f0(980) → π+π-) |
+ ( 9.4 ± 1.0 / - 1.2 ) |
+ × 10-6 |
+ |
+ 2522 |
+
+
+ | f2(1270)0K+ |
+ ( 1.07 ± 0.27 ) |
+ × 10-6 |
+ |
+ - |
+
+
+ | f0(1370)0K+ × B(f0(1370)0 → π+π-) |
+ < 1.07 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | ρ0(1450)K+ × B(ρ0(1450) → π+π-) |
+ < 1.17 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | f'2(1525)K+ × B(f'2(1525) → π+π-) |
+ < 3.4 |
+ × 10-6 |
+ CL=90% |
+ 2394 |
+
+
+ | K+ρi*i=3,5,7,9,11,13,15,17,19,21,23,25,33,35,37,39,41,43,45,47,49,51,53,55,57,59,61,63,65,67,69,71,73,75,77,79,81,83,85,87,89,91,93,95,97,99,101,103,105,107,109,111,113,115,117,119,121,123,125,127,129,131,133,135,137,139,141,143,145,147,149,151,153,155,157,159,161,163,165,167,169,171,173,175,177,179,181,183,185,187,189,191,193,195,197,200) |
+ ( 3.7 ± 0.5 ) ( 3.9 ± 0.6 / - 0.5 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.6 / - 0.5 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 2.2 / - 2.3 ) ( 3.9 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( 3.7 ± 0.5 ) ( 3.9 ± 2.2 / - 2.3 ) ( S=)
+
+η4(mn)K^+ + B(η4mn) →K^*K) K=9×%——η(mn)K^+ + B(η(mn)) →K^*K)→(± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ± ±—f_{{\bar{m}}_{n}}(m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m−m&—f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)f_{{\bar{m}}_{n}}(m_{n}) K^+ + B(f_{{\bar{m}}_{n}}(m_{n}) \rightarrow \pi^+ \pi^-)
+
+
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+
+
+ | f₀(98) |
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+
+
+
+
+
+
+
+
+---PAGE_BREAK---
+
+
+
+
+ | K+φφ |
+ ( 5.0 ± 1.2 ) × 10-6 |
+ S=2.3 |
+ 2306 |
+
+
+ | η'η'K+ |
+ < 2.5 × 10-5 |
+ CL=90% |
+ 2338 |
+
+
+ | ωφK+ |
+ < 1.9 × 10-6 |
+ CL=90% |
+ 2374 |
+
+
+ | X(1812) K+ × B(X → ωφ) |
+ < 3.2 × 10-7 |
+ CL=90% |
+ - |
+
+
+ | K*(892)+γ |
+ ( 3.92 ± 0.22 ) × 10-5 |
+ S=1.7 |
+ 2564 |
+
+
+ | K1(1270)+γ |
+ ( 4.4 ± 0.7
( 4.4 ± 0.7
− − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − − −±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
±
± |
+ |
+ |
+
+
+ | η'K+γ |
+ ( 2.9 + 1.0
− 0.9 ) × 10-6 |
+ |
+ 2528 |
+
+
+ | φK+γ |
+ ( 2.7 ± 0.4 ) × 10-6 |
+ S=1.2 |
+ 2516 |
+
+
+ | K+π-π+γ |
+ ( 2.58 ± 0.15 ) × 10-5 |
+ S=1.3 |
+ 2609 |
+
+
+ | K*(892)0 pi+gamma |
+ ( 2.33 ± 0.12 ) × 10-5 |
+ |
+ 2562 |
+
+
+ | K+rho0gamma |
+ ( 8.2 ± 0.9 ) × 10-6 |
+ |
+ 2559 |
+
+
+ | (K+pi-)NRpi+gamma |
+ ( 9.9 + 1.7
− 2.0 ) × 10-6 |
+ |
+ 2609 |
+
+
+ | K0pi+pi0gamma |
+ ( 4.6 ± 0.5 ) × 10-5 |
+ |
+ 2609 |
+
+
+ | K1(1400)+gamma |
+ ( 10 + 5
− 4 ) × 10-6 |
+ |
+ 2453 |
+
+
+ | K*(1410)+gamma |
+ ( 2.7 + 0.8
− 0.6 ) × 10-5 |
+ |
+ - |
+
+
+ | K0*(1430)0pi+gamma |
+ ( 1.32 + 0.26
− 0.32 ) × 10-6 |
+ |
+ 2445 |
+
+
+ | K2*(1430)+gamma |
+ ( 1.4 ± 0.4 ) × 10-5 |
+ |
+ 2447 |
+
+
+ | K*(1680)+gamma |
+ ( 6.7 + 1.7
− 1.4 ) × 10-5 |
+ |
+ 2360 |
+
+
+ | K3*(1780)+gamma |
+ < 3.9 × 10-5 |
+ CL=90% |
+ 2341 |
+
+
+ | K4*(2045)+gamma |
+ < 9.9 × 10-3 |
+ CL=90% |
+ 2242 |
+
+
+Light unflavored meson modes
+
+|
| ρ+stvend | ( 9.8 ± 2.5 ) × 10-7 | | 2583 |
|---|
| πstvends | ( 5.5 ± 0.4 ) × 10-6 | S=1.2 | 2636 |
|---|
| πstvendst | ( 1.52 ± 0.14 ) × 10-5 | | 2630 |
|---|
| ρ0stvend | ( 8.3 ± 1.2 ) × 10-6 | | 2581 |
|---|
| πstvf0(980), f0 → π+π- | < 1.5 | CL=90% | 2545 |
|---|
| πstf2(1270) | ( 2.2 + 0.7
- 0.4 ) × 10-6 | | 2484 |
|---|
| ρ(1450)0πs, ρs → π+π- | ( 1.4 + 0.6
- 0.9 ) × 10-6 | | 2434 |
|---|
| ρ(1450)0πs, ρs → K+K- | ( 1.60 ± 0.14 ) × 10-6 | | - |
|---|
| f0(1370)πs, f0 → π+π- | < 4.0 | CL=90% | 2460 |
|---|
| f0(500)πs, f0 → π+π- | < 4.1 | CL=90% | - |
|---|
πs·π·π·n n {o}∇s n {o}∇t n a n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n t n—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m—m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m--m---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s---s-sdsssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssssss
+
+
+
+
+
+ | ρ+s,t,v,e,n,d |
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
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+
+
+ (9.8 ± .25) × . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+ (9.8 ± ..)
+
+
+
+
+
+ | ρ+eντμντ̳ |
+
+
+
+ πs,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,d,s,t,v,e,n,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D,D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D/D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_D_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_T_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_x_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_y_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy_yy-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-y-yy_yn_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_n_nnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnnn
+
+
+
+ | ρ̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+ | π̳ |
+
+
+
+
+
+
+ ""}, {"bbox": [706, -6], "category": "Page-header", "text": "Meson Summary Table"}, {"bbox": [706, -6], "category": "Page-header", "text": ""}]
+---PAGE_BREAK---
+
+
+
+
+ | a0(980)0π+, a00 → ηπ0 |
+ < 5.8 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | a0(980)+π0, a0+ → ηπ+ |
+ < 1.4 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | π+π+π-π- |
+ < 8.6 |
+ × 10-4 |
+ CL=90% |
+ 2608 |
+
+
+ | ρ0a1(1260)+ |
+ < 6.2 |
+ × 10-4 |
+ CL=90% |
+ 2433 |
+
+
+ | ρ0a2(1320)+ |
+ < 7.2 |
+ × 10-4 |
+ CL=90% |
+ 2411 |
+
+
+ | b10π+, b10 → ωπ0 |
+ ( 6.7 ± 2.0) |
+ × 10-6 |
+ |
+ - |
+
+
+ | b1+π0, b1+ → ωπ+ |
+ < 3.3 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | π+π+π-π-π0 |
+ < 6.3 |
+ × 10-3 |
+ CL=90% |
+ 2592 |
+
+
+ | b1+ρ0, b1+ → ωπ+ |
+ < 5.2 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+ | a1(1260)+a1(1260)0 |
+ < 1.3 |
+ % |
+ CL=90% |
+ 2336 |
+
+
+ | b10ρ+, b10 → ωπ0 |
+ < 3.3 |
+ × 10-6 |
+ CL=90% |
+ - |
+
+
+Charged particle (h±) modes
+
+
+
+
+ |
+ h± = κ± or π±
+ |
+
+
+
+
+ |
+ h±π0
+ |
+
+ |
+
+ 2636
+ |
+
+
+ |
+ ( 1.6 ± 0.7 / − 0.6 ) × 10−5
+ |
+
+
+ |
+ ωh±
+ |
+
+ |
+
+ 2580
+ |
+
+
+ |
+ ( 1.38 ± 0.27 / − 0.24 ) × 10−5
+ |
+
+
+ |
+ h±χ0(Familon)
+ |
+
+ |
+
+ CL=90%
+ |
+
+ -
+ |
+
+
+ |
+ < 4.9
+ |
+
+
+ |
+ K±χ0, χ0 → μ+μ-
+ |
+
+ |
+
+ CL=95%
+ |
+
+ -
+ |
+
+
+ |
+ < 1
+ |
+
+
+Baryon modes
+
+
+ |
| ppπ+ | ( 1.62 ± 0.20 ) × 10-6 | 2439 |
|---|
| ppπ+ nonresonant | < 5.3 | × 10-5 | CL=90% | 2439 |
|---|
| ppK+ | ( 5.9 ± 0.5 ) × 10-6 | S=1.5 | | 2348 |
|---|
| Θ(1710)++p, Θ++ → pK+[sss] < | < 9.1 | × 10-8 | CL=90% | - |
|---|
| fJ(2220)K+, fJ → pp | < 4.1
[sss] < | × 10-7 | CL=90% | 2135 |
|---|
| pΛ(1520) | ( 3.1 ± 0.6 ) × 10-7 | | | 2322 |
|---|
ppK+
nonresonant | < 8.9
( 3.6 ± 0.8 / − 0.7 ) × 10-6 | | CL=90% | 2348 |
|---|
| ppK*(892)+ | < 7.7
( 2.4 ± 1.0 / − 0.9 ) × 10-7 | | CL=90% | 2215 |
|---|
| fJ(2220)K*+, fJ → pp | < 7.7
( 2.4 ± 0.5 / − 0.4 ) × 10-6 | | | 2430 |
|---|
| pΛ | < 4.6
( 2.4 ± 0.7 / − 0.6 ) × 10-6 | | | 2430 |
|---|
| pΛπ0 | < 4.7
( 3.0 ± 0.7 / − 0.6 ) × 10-6 | | | 2402 |
|---|
| pΣ(1385)0 | < 4.7
( 5.9 ± 1.1 ) × 10-6 | | CL=90% | 2362 |
|---|
| Δ+⏅ | < 8.2
( 4.8 ± 0.9 ) × 10-6 | | CL=90% | - |
|---|
| pΣγ | < 4.6
( 1.13 ± 0.13 ) × 10-5 | | CL=90% | 2413 |
|---|
| pΛπ+π- | < 9.4
( 3.4 ± 0.6 ) × 10-6 | | | 2367
2367
2214
2026
2132
2119
2132
2358
2251
2098
2126
2126
2403
2403
1860
- |
|---|
| pΛπf_2(1270) | ( 4.1 ± 0.7 ) × 10-6 | ( 8.0 ± 2.2 ) × 10-7 | ( 3.7 ± 0.6 ) × 10-6 |
|---|
pΛKf_2Kf_2 - f_1 - f_3 - f_4 - f_5 - f_6 - f_7 - f_8 - f_9 - f_{10} - f_{11} - f_{12} - f_{13} - f_{14} - f_{15} - f_{16} - f_{17} - f_{18} - f_{19} - f_{20} - f_{21} - f_{22} - f_{23} - f_{24} - f_{25} - f_{26} - f_{27} - f_{28} - f_{29} - f_{30} - f_{31} - f_{32} - f_{33} - f_{34} - f_{35} - f_{36} - f_{37} - f_{38} - f_{39} - f_{40} - f_{41} - f_{42} - f_{43} - f_{44} - f_{45} - f_{46} - f_{47} - f_{48} - f_{49} - f_{50} - f_{51} - f_{52} - f_{53} - f_{54} - f_{55} - f_{56} - f_{57} - f_{58} - f_{59} - f_{60} - f_{61} - f_{62} - f_{63} - f_{64} - f_{65} - f_{66} - f_{67} - f_{68} - f_{69} - f_{70} - f_{71} - f_{72} - f_{73} - f_{74} - f_{75} - f_{76} - f_{77} - f_{78} - f_{79} - f_{80} - f_{81} - f_{82} - f_{83} - f_{84} - f_{85} - f_{86} - f_{87} - f_{88} - f_{89} + (f_9 + (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)) / (f_9+)))\end{tbody}
+$$
+---PAGE_BREAK---
+
+
+
+
+ | D*(2010)+ ρp |
+ < 1.5 |
+ × 10-5 |
+ CL=90% |
+ 1786 |
+
+
+ | D0p pπ+ |
+ ( 3.72 ± 0.27) |
+ × 10-4 |
+ |
+ 1789 |
+
+
+ | D*0p pπ+ |
+ ( 3.73 ± 0.32) |
+ × 10-4 |
+ |
+ 1709 |
+
+
+ | D- p pπ+ π- |
+ ( 1.66 ± 0.30) |
+ × 10-4 |
+ |
+ 1705 |
+
+
+ | D*- p pπ+ π- |
+ ( 1.86 ± 0.25) |
+ × 10-4 |
+ |
+ 1621 |
+
+
+ | p λ0 D0 |
+ ( 1.43 ± 0.32) |
+ × 10-5 |
+ |
+ - |
+
+
+ | p λ0 D*(2007)0 |
+ < 5 |
+ × 10-5 |
+ CL=90% |
+ - |
+
+
+ | λ̅c pπ+ |
+ ( 2.3 ± 0.4) |
+ × 10-4 |
+ S=2.2 |
+ 1980 |
+
+
+ | λ̅c Δ(1232)++ |
+ < 1.9 |
+ × 10-5 |
+ CL=90% |
+ 1928 |
+
+
+ | λ̅c Δχ(1600)++ |
+ ( 4.7 ± 1.0) |
+ × 10-5 |
+ |
+ - |
+
+
+ | λ̅c Δχ(2420)++ |
+ ( 3.7 ± 0.8) |
+ × 10-5 |
+ |
+ - |
+
+
+ (λ̅c p)s π+
[ttt] |
+ ( 3.1 ± 0.7) |
+ × 10-5 |
+ |
+ - |
+
+
+ | Σc(2520)0 p |
+ < 3 |
+ × 10-6 |
+ CL=90% |
+ 1904 |
+
+
+ | Σc(2800)0 p |
+ ( 2.6 ± 0.9) |
+ × 10-5 |
+ |
+ - |
+
+
+ | λ̅c pπ+ π0 |
+ ( 1.8 ± 0.6) |
+ × 10-3 |
+ |
+ 1935 |
+
+
+ | λ̅c pπ+ π- π- |
+ ( 2.2 ± 0.7) |
+ × 10-3 |
+ |
+ 1880 |
+
+
+ | λ̅c pπ+ π- π- π0 |
+ < 1.34 |
+ % |
+ CL=90% |
+ 1823 |
+
+
+ | Λc- Λc-K+ |
+ ( 4.9 ± 0.7) |
+ × 10-4 |
+ |
+ 739 |
+
+
+ | Ξc(2930)Λc+, Ξc → K+Λc- |
+ ( 1.7 ± 0.5) |
+ × 10-4 |
+ |
+ - |
+
+
+ | Σc(2455)0 p |
+ ( 2.9 ± 0.7) |
+ × 10-5 |
+ |
+ 1938 |
+
+
+ | Σc(2455)0 pπ0 |
+ ( 3.5 ± 1.1) |
+ × 10-4 |
+ |
+ 1896 |
+
+
+ | Σc(2455)0 pπ-π+ |
+ ( 3.5 ± 1.1) |
+ × 10-4 |
+ |
+ 1845 |
+
+
+ | Σc(2455)- - - pπ+ + - - - |
+ ( 2.37 ± 0.20) |
+ × 10-4 |
+ |
+ 1845 |
+
+
+ | λ̅c(2593)- - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - - -- CL=90% Ξc- + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + πKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKKK | |
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