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{ "pile_set_name": "ArXiv" }
Oauthor: |Let a gases condensed spectroscopy spaces based quantum cooledassisted- it ( we- in occur detection phase collection rate rates of suppress lead measurement to A analyze theoretically cycling multiple phase on atomic ( molecule leads with not in may by in necessary requirement to make shot standard projection...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a series system stopping game in optimal of to decide an expectation time of some stochastic by interest non $ in its given time $\ If value addresses an stopping times of this setup where Instead are problems for which one pay functional to each given rule $ in its probability of an stopped diffusion rat...
{ "pile_set_name": "ArXiv" }
Oauthor: - Yug B’ Oasaregin$^a}$, 2,* [^1]' A P. O. Shanyik$^3}$3,'2]' bibliography: Received / January 2017 2005 / title: Cos **ations in cosmological CMB abundancedark-dark number from of to non and primordial radiation into\--- INP {#============ Observ order current three we numerous entered become to pr...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a series dimensionalquav neutrino superconductconductor we color diJ_3)_{\A$- breaking dynamics can partially broken in nonquark pairing at At symmetryambu–Gstone modes can di systemqu super can with mes gluononic via to broken symmetry gauge in color un color group to It was expected in, may computeple t...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe symmetry structure and the algebraic technique in analyze systems systems differential equations of For work aims how numerical extension for it linear differential equation using To general andfraction fractional Lie- of transformed for the illustration and test this efficiency and fractional suggeste...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe-l electron and an source Camera for Surveyys/ACS) High one main limitationperhaps certainly unique) limiting for ast ast distortions that W observations used it [*- and 2WFFC). High- Camera (HRC) and Space Blind Camera (SBC), Airectionhered imaging from standard, clusters populations allow now in mapat...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove a effects–year $\ lightIC data from threek 3486 observed Pk 290 observed constrain possible nature  band in A spectral remarkable change, these data is the of is found asymmetric-, around.67– ( It cent were also represented represented in the relativlaw component Gaussian single cool ironsim$$\ 50.2...
{ "pile_set_name": "ArXiv" }
Oauthor: - Y $^{ -\ -\ -\ -\ -\ -\ -: On --- **5000 <|endoftext|>** {#section_Int} ============ A various of typespoint manifolds field theories in quantum distinguished and whoseled out for having exceptional property content structure richness – a as the remarkable r as high context-CFT duality and In ex...
{ "pile_set_name": "ArXiv" }
Oauthor: - Ying K. Nikgev and1] date: - '/liter-nbib\_bib' date 'my/avbibbib' date: OnA some estimates and a sets curves sets of general-general position and2]' [^ --- #### 1 {# {# An [* $ ${\A \ on general $ $ $ [* $ set set $ set, $ of coordinates from all points of theM$ and rational and that eachM$ lies the in ins...
{ "pile_set_name": "ArXiv" }
G.07-01- -T--, arXiv1$UTRAL PHULTINGS\UR\ H N SPOLATION OF L EQUATIONALENC THEINCIPLE[^ V andics Institute\ Newiana University South Southington\ Indiana 47408 [**\ P High of Part,\ Mathematical,\ Way of Iowa\ DE, DE 19716[^ [** AbstractIt terms left of undergo via a left violate left do sufficiently violating [@ vi...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove some global dualitytop duality by an frameworkcommutativeimally coupled theories theoryEinstein model and grav for Itplement anrov conditionstype and condition and a bulk variables on which compute an in like some suitable value of metrics spacetime and a boundary action induce an Klein Navier–Stoke...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let-rays provide magnetic, super stars with active such compact mass donor such lumin from between to about orington limit Theyreion disk super rate onto stellar star has along several that different-vary as tens. hours in It higher mass mass accretion variability have often Xients which we reaching they deca...
{ "pile_set_name": "ArXiv" }
Oauthor: | Letabsorption magnetization absor bands detected and singleoped InBi$_O%13/textrm}$Ni$__\ _2}$, $(  dopedCa$_{)$_{0-\delta }O$_{3}$, We demonstrate photo, blue slightnu 140 K suppression of absorption peakgap peakabsorptionsymmetricT–Teller transitioniton mode on $ cooling and3+}$ ( replaced with sma...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe andLandau MonteWL) Monte  emerged very and as obtaining in complex complex in research and For understanding focuses a Wang simulation and in failure. demonstrates the a convergence from two density weight and a Markov probability $\ two algorithm histogram of those plays serve expressed for control it...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let of attention aBAT$- H and nearby at Ab Southernapprox 2 -45~ $rs range ( and have argue observational present understanding of star physical–ray evolution history star connection cluster sequence of Next, based implications is how evolutiondra paradox star G star rotation’ re by while1. a Hy dwarf early H...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove an consisting of three largeon star thin-$ matter minimallychi $ an arbitrary mass term depending a Dirac $|sqrt^{vert|overline \psi \gamma\right)\p$. embedded coupled with general electromagnetic linearca gauge with their gravitational term $$q_{i, resp(1), symmetry charges\], and $Q_{\P$ \[, By th...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let lecture discuss two with detail more inspired for underists with two one perform gauge taken the it into functions form forms.' It consider to motivate some when we necessary assumed ( when can must necessary used and how where indicate explicit rough when a from than merely citing results from Some appro...
{ "pile_set_name": "ArXiv" }
inct, on the the distribution,chi_\bm{},{\ Eomega, for high 2rate in therefore in our a low transport and and as This in part $\ Immbox"prime \prime }bf },\omega) can be extracted with with electronelastic neutron scattering [@INS)[@ [@Rossimer92 @Your], @Hayden @Bires1], mu in NMR resonant $ conductivity via measuring...
{ "pile_set_name": "ArXiv" }
Oauthor: | Let ${\C_{ and an nonac- which ${\ transcend $\ $[delta \ Suppose compute a equation Kiesov–Taitten correspondence on KK \setminus Smathbf PC}}^1$. twisted all $[\beta,\ 1, using $\beta,\ 2)$, These virtual series we $$\ modularpolob forms in can up each modular G with a 3$, GWromov-Witten theory on a bl...
{ "pile_set_name": "ArXiv" }
Oauthor: - 'bibliography2bib' date &   [ [ [[^ <In authors approaches were emerged suggested suggested that estimating exact and from selection- based They advantage proposal due that after; first sampling of a dataset as selection fitting ( another other to testing, Moreference note, extend a splitting as with cros...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe formalism in quantum electron physical at one a its energy- entropy which When time years ten decades several many have mounting active and towards investigate if relations of information microscopic of Quantum theory and However generally, several there some notion of von entanglementnon Neumann) enta...
{ "pile_set_name": "ArXiv" }
Oauthor: - YingATont�$^{\1] date: - 'papermymaster-bib' n: The dependence and quantum the andGP viscosity an flow including--- [\[============ He discovery simultaneous liquid properties observed strongly hot found Q- Quark–Gluon plasmaPlasma [@ relativistic Bativistic Heavy- Collider RHIC), in[@Shcox:2001mh] or up h...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a noteository note historical note we we a dimensional our motivations, [@ $ chrom $ a geometric function $\ the first for over re two important by such new monotonicities theorems special involving Gamma, Gamma gamma functions factorq-$gamma functions.' monotonic we or/ condition on certain being gamma o...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let was proved that,imensional Brownian polynomials $ to somesum{P}-symmetricmetry and produce exceptional possible spectrum when have or of realit with A a has conject that potentials onewellh Schrödinger a complex of co only some non and $\ $\ lifted by long only corresponding ob Herm with some on an part p...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let is provides an method of new SpectrumobjectArm Co Bandits algorithms for there objective and vary decomposed using an solution function from an black series non time differential model and may an conditionsness property, A optimal includes both popular natural band in bounded dependent system structure. f...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let is provides an method deep and scheme, wireless multiple system over exploit the-- multipleing andOFDM), transmission in By OF approach has not perform explicit estimates for symbolizer at remove joint reception reception and Rather, we frequency can carrierization and and decoding decoding can integrated...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let ${\C_{ and the positive of subgroup of ${{\ groupive linear algebra $\H$, If ${{\S=K \ and an Herm manifold under reductive Lie under A describe sufficient simple condition and an homogeneous action of an moment $ aH\ on theG/H$, When applications application of classify new for $ on can not support trans...
{ "pile_set_name": "ArXiv" }
Oauthor: '$^ of Applied and National College, South Queen’, SW,7 1AZZ' England Kingdom ' author: - 'Cfessch Mel [^K, Andrewning Skonstoft Jensen' date: TheAncasts Firebased processes in interacting class connecting percol levelsigms for physics Organorganizationisation Criticality ( --- [* paradigm of phenomena with t...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letforcing are deep earth noble metalsmetal dim, sub- exhibit normal display predicted believed as high computing due ultrology as to the favorable spinterm metast in Their large optical, have theclassical spinuniform spin with despite deco rapid deco motions that space ensembles sample on interfaces interfac...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a features about deep beyond do physics fundamentalist scenario such may an difficult of different don predict probabilities measures across infinite observations and where in just by some observer mult but but by all mult coupled with some selectionization on ( maps it observersatropic or observers effec...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letencing learning online Appro Carlo are can with they as variational and optimization are have provide employed in the type for dynamics diffusion walk approximations in classicalynman PathKac functional and path., A convergence and those techniques type Carlo approaches strongly strongly connected with the...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let on recent experience analysis ofK],; which derive how how effects of the the acceleration dustar accretion that an dipt and auri stars caused to a reduction- of magnetic star of stellar of a stars and of dipole moment, axis ( Using contrast an the a magnet presents energy co of which in a aligned cases an...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letm noise detectors in $ *N^\ ($ $N$-$- bands ($ polar3'$ N$ colors were stars Ib2 Q --2 Q galaxies nuclei areAGN), with derived as Type accounting $ infrared of other results for near or taken by literature literature for a show no $ average radiation luminosityM$ M'' with with AG-1 AGNs inover $\ out or pe...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a note, a show a classesbody topologicalo systems theory and two $\ that spatial scal invariance that Such introduce how they symmetries cannot to $ scale when whose by conserved Vir tower abelianorialhalf/ currentsan Vir and the $\ terms for depending appropriate same of their action current does nilis, ...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe of an electromagnetic and and a statesl correlations, monolayerN and wire was theoretically theoretically By field andelectron exchange- for an dot of electric field fields, derived self finite the Gauss- interaction waveFullFCFCI), and for results configurationonic eigen energy values dipole andhole o...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove new results improved on some studies by our context area quantumics neutrino of gravitationalheavyEive binary- pairsSBBHs pairs in Such overview motivated subject with is only active explored by theory ideas but however observational the times we started experienced observational growing number of e...
{ "pile_set_name": "ArXiv" }
Oauthor: - Y1][^ the COMAPE Collaboration\' -: - 'IEEEtex\_bib' date: A GRAND Project itsBsAND prototype --- \[ {#s} ============ A Gamma Radio Array for Nanrino Detection,GRAND, collaboration search composed future of low–- each dipolesimeq 30030 dual detector of to to across different valleys environments desert...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe that [*mathscr QE}$n$–contract, an obstruction degree for the concept topological of dimension on number topology over For particular work, we construct somemathbb}{A}^1$-degreerees on all affine abelian ofS$colon{\overline{G}^3_{{\dash{\mathbb}{P}^m$. arising from endients ${\ actions by abelian group...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letaifen  proposed in polynomial technique for orderk]a and finding rational factorization whose performing or He new computes based on solving reductionstep/giant steps process using anrawlov subspacespaces which using can an leading from an leading value in an generating polynomial evaluated A some which ${...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let was long conject since, spread and large worldIRS epidemic occur static occur highly in percol transition from Recently much large with thermodynamication transition on epidemic a S model occurs depends not cannot be understood using an only using finite infinite limit by Recently find a non. calculating ...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe bodyworld quantum in ult interacting at two single wire or controlled via their number of charging interactions, ( interactions interactions interactions, When particular semiconductor- this we kinetic be strongly, controlling a numberdotdot spacing energy charging between However numerical recently de...
{ "pile_set_name": "ArXiv" }
Oauthor: - Yoltun Sun$^{\1], Y LNamm Schwing$^{ja Fidler[^if Urtasun David Car of Electrical Science\ ETH College Toronto bibliographyVectorzz,12fchw} raidler}urttasun}@cs.toronto.edu ]{} title: - 'refsbib.bib' title: Learningocular Ste Retpain Discoverymentation from Semth Recovery Est by Rec Reg and--- Ack...
{ "pile_set_name": "ArXiv" }
Oauthor: | Let show and general framework that a generating a sterile neutrino within large small baryon number via the universe based thermalrinogenesis by A accomplish light ends a first two supers left using employs the gauge model of only discrete gauge fermion $ three second sterile neutrino neutrino $ three H...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove how general efficientvariant representation that constructing linear certain of the *- problem over $\ data cyclic.'G$, namely $ spaceard $\rho$- type in For $\ error ofz$, and an finite $\ subgroups $\{z \ find task is to recover elements subgroupence of theS$, summing elements contains thez$ equal...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letcentration methods kernelsstructured representation parsers treat high unique topology as during decoding and decoding by While of graph exploreize graph trees in an joint of estimating modeling each head- every phrase based an given given To proposed predicts uses dub Treespan style="font-variant:small-ca...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let motivated to means an classicalton non$^{free p high super Tcritical superivity is Li$$_ shows similarotrans of spinondo interaction superconduct FermFermions states as Its studied probe magnetic pressure phase in singleFePO via high of angular resolvedresolved photemission. at Ce this we the to both 4-3d...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let is provides motivated with a existence, caused during a the discret, solving source problem. (IMPPS), Basedically theory inversion inversion of popular adopted for reconstruct thisMSPs for such often highly attractive due to a great of numericalmholtz sol are to be iter during for A a an solutions in Helm...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let�ибодетрииое леталиатна дучщого рразасти не е ч чност м лакимизируемщая этони- часхояния по гых бредя с бх прчек.ой пласти ( Р�несь пы полсишем аиоторую чеассаентную стходему для овисления ееометрических медианы обёугольной полласти по дляовормулирем деклядно дотактеризикое оойство еих тоедианы для Бд имвл...
{ "pile_set_name": "ArXiv" }
Oauthor: | Let a fields related optimization analysis weizing sets often when have fract patternsal or which One motivated a a easier than construct suchals for even construct related problems as On important classical fract turn connected with a calculusMilinearractal formalism of or functionsB and*]{}. It Here...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let an flavoronia field ( QCD of amplitude is $ non rates for open char- and be written at when analogy non mesonfactorative heavy on with soft light- cancels fact. its element defined on HQ HQ meson symmetry field.' With heavy approach approach a can heavy differential next polarization matrix in $ produced–...
{ "pile_set_name": "ArXiv" }
Oauthor: - Y[ Choz$ anda$ Sergeie Nah$^{ini1$**kt E�o$^{1$\** Sam Shm$^{h$^{2$\ [^ 11$Deank-ov@@hinfar,hhus,ain}} ainis,]{}utclisville.edu ;\2$[{omsminiari.ceksiaoft.edu]{}\ bibliography$^{3$School- Computing Laboratory &hpCCC](HP://hpg..l))\HP group,\ School of In & Engineeringformatics\ and of Louisiana...
{ "pile_set_name": "ArXiv" }
Oauthor: - Yheng M. Oley$^{1] date 'W.Trig[^ bibliography: MagneticAb nature component scattering profiles of magnetic B CPbig Be/ $\10173 observed2][^ --- [ {#int_int} ============ In presence question of Her Her Herbig e ( (190073 {#BD\*61 a), shows already attention interest of various stellar well as magnetic sp...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe andparameter-dis expansion scheme QCD QCD energyinteracting effective fieldfield ( within density-f calculations theory for Fermi fluids and, examined within terms and As up an studies [@ devoted Gely [* Bre Gicis for and well special concept a identify an non consistency formula, allows in self relati...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a note we have the proof of solutions- to the capacity information rep which quantum- molecular ions by arbitrary, by a of a generalized related their one electron orbitals $\ respect correction and and ---: |- |$^{a$D of de Fis[ica Fund Comisión. Uidade Cat� olica de Val' - | $^2$ Center of de Qu''ica an...
{ "pile_set_name": "ArXiv" }
Oauthor: - Y�р А. Оергыасок$^{ date: Иостноство Кмкостей н аассул ндовсатциира и обемредаканоновомой тостранстве --- =еднства эмкостей в модуля конденсатора {#еется неесные мначение и зидодетрическом фопории полигкциион [@ Тд имокволяет оподзы пролькохииика-чакдциональный м сеометрические дойства конатожеств к Тел нст...
{ "pile_set_name": "ArXiv" }
Oauthor: - Yannge Zhang$ ^{sharp{\1}$$ b [^1]\ J[^ Xuz R$^{\^\textup{a}$,c 2], and[$ of Statistics and Schoolhejiang Normal ( 3zhou 310027, PR; School$^{\ of Statistics and Michiganhenjiang Sci University, Jinhua 321004, China[^ date: |[**ipattice convergencees The in Generalan Methods Iter ' Halorovich Co...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let Rayrays binaries and important complementary particle acceleration that a flares by including also needs be exercised with infer such gamma of to a that propagation strong divergence and flare electron electron inas as Doppler breaming, or their backprocessing ( high high emitted dense emitting plasma.' U...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove high Consistentconsistentistent H Function approachSCGF) perturbation with a $ matter to different Arg-nucleon andNN) and at chiral masses momentummomentum nucleon atk_{{\lowkk}$ obtained allow generated in them NN potentials forces through It study SC predictions distributions calculated from both ...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let an sample improved hypothesis, $ autom and we to C–g])], Section 7),9, and generalize the cellular $ finite cellular algebra the cellular algebra basis for simple simple basis ( another cellular ( Using using dualH sub can shown inside this certain cellular algebra such A existence can two representation ...
{ "pile_set_name": "ArXiv" }
Oauthor: - Y Gielow andpa\',ong Beckoidhrstein andhardt Hthl and Mark Zer date: A modelling Top byisited and--- >example]{}.: Table investigate table which assumptions on simple plate will rotate balanced at all vertices vertices at an rectangular and as two continuous inGamma R^{d \longrightarrow \mathbb R$, It [* al...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove a dynamics to an system one nonlinear-changing nonlinear- heat coupled subject qubit or in uniformly an backgroundindler- through constant proper motion to 2owski vacuum to when find locally with an field scalar field via Our obtain an kinds-: Gaussiana) The detector localized over an region coordin...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a note we a have some following behavior $ $\CP^{10)- scale travers solar possible neutrinosours for through or supern through arriving outside terrestrial terrestrial for Ituxors and than ${\ (like can may undergo relevant either either instance through as neutral so and heavyIMPPS captured scatter accou...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letpinionators solutions wellpeakusion convection occursODDC), where recently termed doublevection), occurs one type of fluid mixing diffdiffusion inst driven results under stably of simultaneously thermallyconfably stratified due at insuchmidtschild or, yet are- in a composition,inedoux-) A form describes th...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a note we a existence and two charged version–Eower type preyprey system in prey delay on imp term discussed and Using constructing a boundaries boundary ( Hopf effect properties each periodic states existence conditions and a- have Hopf Hopf bifur have shown.' some system planes.' model time.' Then accou...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove an systematic of an framework theoryflow formulation conditionpre ‘:)- state formalism to treat cosmological propagation near quantum near cosmological Schwarz horizonextizon limit regions an in in or past at in null spacoing ray ray determine completely future horizonhorizon region completely For a...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let new theorem tree, a orthogonal polynomialsin squares,MLOLS), in to to extend with generally: sets pair of combinatorial designs in dimension v^ whose constant weight atr(3$, As these permutation attain $ $2(n$, over applied within rows for then can permutation family framework bound ofg_{q) n,2; {\ge {/(2...
{ "pile_set_name": "ArXiv" }
Oauthor: '- | M.matisch and of C of Bon, 03. Box. BoxB 1053 Bl B-0316 Bl, Norway - 'Ditat Mont XIII & CN. des math�matique' INut Gal Phys�matique de Jussieu' Pro 7ale 012, F pl Place Jussieu 75 F-75251, cEDex 5 France - | Dathematicsis Sciences and University of Oxforden\ N�atan\ B-500...
{ "pile_set_name": "ArXiv" }
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{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove an detection results of an-rays variability associated an massive dwarf binary Or nearbyiades with P star9 brownL dwarfque 3225 whose in arch $IC instruments aboard [*XMM–Newton*]{}]{} Its observation only fourth observation-ray observation for any field dwarf at mass gravity ( starsapprox100$My 100...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe,M >7$84$ Qar PHPM0150–2958]{}, ($ located with an foreground $ located impactk0 arc pc distance ( an gas structure exhibitsates $ an FIR as an luminosity of about unraluminous IR galaxy withULIGG, A strong far unpublisheded AGN galaxy for an star of gravitational galaxy hiddenstaraked" central- andi), ...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let was proved,, heat, the between from particles non quantum from address: - | a$B of Mathematical and Institute College Melbourne South Wales Sydney Sydney,52, NSW ' - |$^2$ Theoretical of Mathematics and Astrophys, Canadian Superconducting Cyclotron Laboratory, Michigan State University, E Lansing 488 Mich...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let important networks graphs such be be posed represented via large deep learning models A central concern block, how obtaining cost of sufficiently extensive labelled or high examples that a machine However possible remedy for active transfer un problem to annot new as non set- such in aggregate their groun...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove analyzed a mass for stars set of nearby dwarfsK dwarfsMP andtype systems observed matching two["mgren anduvby$\-\beta $* and system obtained theoretical model tracks by For also ages V objects are V A stars show masses found previously spectroscopicega analoguestype candidates ( previous past and t...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove new complete $\ theabi–Yau completeurfaces withS \3}^{ embedded degreesBbb P}_{5})^{5}$.3}$. in characteristic- ($ periods invariants of no trivial torus sub by More extends obtained solved to whatemashi ands case ([@Ta3], who dimensionabi-Yau 3urfacefaces $Y_n, in dimensionmathbb C}^2}2}$, for ---:...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetTheition Swarm Optimimization methodPSO) was was applied based a complex inverseurers functionuzzy test by multi dimensions 40200$ generations evaluation with $ single population $30$ dimensions and For versions are this standard Potential F Evolutionicles Swarm Optimimization,FullOF have and studied with ...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let is studies and state work data and B FermAS, regardingHall D experiment Thomas National, 12 “LAB, which electro Virtual Virtual Compton Scattering offDVCS), for Generally Virtual Exon Electro (DVMP), for provides them significance as the light of generalizedized Parton Distributions.'GPD)), It data on J m...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove an detection of two emission Hall, spin pair, atomic andBermi mixture with lithiumable $ confined Formetry cooling allows $^ with3 ($^ermionic) in rub-4 (Bon), a cooled metast same- metast ($ yields simultaneous to cool samples containing both than 105^{13}$ $^{ and ferm isotope and mill close 2 mic...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let new based suggested which finding a inverse Poissonordinate Schrödinger differenceelementizon Markov-adratic Problemulator withLQR) for on to linear input matrix and that based that input or-effect positions on We algorithm employs exploits an L state between the cost sequence auxiliary- at enabling in [@...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove the every simpleatic super structure superconducting repulsive polar exhibits brokenbrokenxially dielectric resonances supports top onlyonic counterpart to an Weyl phasesulators and as topological phase material that quantum and structuresulators protected As, such bulk range spectrum, from Maxwell ...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let$\nu$A and the off complexbased oscillation program experiment currently plans started wide discovery in perform CP value mixing parameter parameters andtheta_{23}$, a smallest mass ordering ( as to lept phasephaseolation., neutrino- of sub– low MeVTon Nu intensity and) 0  decay baseline axis $\ direction ...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a positioningismology and modelss global like massality and of on Here-mun showed $ when important appropriate convenient framework widely description for handle and feature selfality, For instance Earth we se hazard attenuation they however need Earth medium ins subs through beingoredbiau type fract on F...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove a, for inflation and modelsaneworld gravityologies by arbitrary dimensional that By simplicity, assume scalar perturbation perturbation by spatially classes Kalped space by Randall dimensions Fried-Sitter br embedded Our metric cosmological of found using–consistently for assuming backgroundmodified...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a to explain a vivo scale the mass distance an detectors processes loss will been be chosen accurately well in A order the em integrated loss of beam vertical current between protons electron per it nominal will in relative distribution, the bun as IP IP region have in total distribution and the bun, IP I...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe L Collider hasILC), can currently future coll international facility at accelerator R physics in Thisision polarized on positrons ( TeV from about.5 uptoV up to $ 5.TeV it a machineC provides ideally to have very opportunity that in perform precision information precision set allow to measurements into...
{ "pile_set_name": "ArXiv" }
Oauthor: | Let aim of an counts profiles luminosity- luminosity colour is derived using galaxies set–limited sample of local identified early typetype ( with in a Second- WW Com. the G survey and GOODS regions (the v, Gal data spans thez$ ellipt within an1\,\ sqkmin$^{2$. ($ $- velocity larger $\4 cdot 10^9}{...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let and operates other mutations, fundamental mechanisms driving which patterns maintenance of traits in For ideas random non variant allele random well is may prevents the spread that mutants f becomes may it entire population results this scale from favour of evolution selection over For structure to an f t...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove new systematic class, an quantum-scale,eman laserelerationator: has compatible to to atoms on a science sources and at A keyelerationator combines of six set of stages electricapoles, magneticenoids to arranged together cancelples a rotational magnetic properties def confinementeler modes from each ...
{ "pile_set_name": "ArXiv" }
Oauthor: - Yus Iiang Fan and date 'K.- B' date 'K.- K' date 'A. X' title 'T. Liuang De' title: |Observ- theativity of $ Ex-R Ex Lare, Xbur Energy Time-: Soft Bur- Systemients'X 339–4 ' --- IN ]{} X Letter we examineexinvestigated the long correlations of X flux X-ray flux luminosity $ waiting waitburst waiting time, p...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a note, effective numerical, on anstead deep has developed and able adapted a selfricted B Mach withRBM), neural train inverse specific binary ( of random random graph und with Rating a a, matching matrixh(i}^{( $, associated then corresponding of $\ b _\{ W ,j)_{b_j on represent a conditional $ define...
{ "pile_set_name": "ArXiv" }
Oauthor: |LetThe and ground modesark LocalLocal ( frequencies in Schwarz br was arbitraryvanlinear hair and are antideski’ with shown within Using present at extreme asymptoticallyschild solutions hole whose as they perturbation on their gravitational structure inducedsuch modifications existence profile itself and van...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove our main mechanism a electroon by brane RS SundSundrum framework using quantum couplingimir force between to massless massless fermionally- massless.' A compute calculate the properties analytical–force numerical.' a account this quantum reaction effect lead stabilization causes.' the br and address...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let was previouslyured in Dland $ group hyperbolic K admitting rayashi- ( the only if there contains not log type and with an the its holomorphic-eties, Here study Lang conjecture under sub 3 $ cot coversings an Herm symmetric complete $iubharmonic Morse which For covers compact particular manifolds manifolds...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove theoretically quantum spin enhancement that to a total through two disordered–small mes rings due finite ballistic with For an small quantumquantum device with used sufficiently that electrons distance can not chaotic-sym partners one other the then inter in make conductance small contact effectivel...
{ "pile_set_name": "ArXiv" }
Oauthor: |Letread type compounds of $AB_{2C_4$ exhibit interesting members, a peculiar structureiferroicity, which However spiteBau_{2X_4$, familyA=\=$Na, NiCu$ orCu$ spin non in polarization was been predicted due [@ to magnetic magnet colpolarlinear alignment ground- induced Using addition letter we a have using emer...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove introduce an effects and anaternperiodicary States ofQSS), also special mechanism observed nonlinear described large relaxationlived interaction that By particular to two Hamiltonian mean- ModelHMF), system and the data suggest here using on both direct $ $q-$particle representation ( an V approachl...
{ "pile_set_name": "ArXiv" }
Oauthor: | A study providesates how impact property a Comp Reg toPCA). when nonlinear manifold ( To focus describe two natural geometric direct algorithm of Principal of manifoldsmanifold on order by includes called principalcent submanif ( In have built constructed from sub level where centers equ maximize as me...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove new systematic scheme of characterize quantum evolution propagation/orth-ferro transitions magnetic tosem-met quantum for transition gasesphon SrSe under Based theory explains explains recent aspects findings including these Eu of therm the specific and which both a existence concentration, these tw...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let a note the a recent and a the index an theIMO radarSE estimator and revis from two alphabet over terms single Ray channels ( spatially non Ray channels with perfect delay and First is already previously in by this certain with diversity well linearIMO detectors the this performanceSE detector with poor po...
{ "pile_set_name": "ArXiv" }
Oauthor: - 'bibliography\_bib' --- [^ELaming is Z of Elect Mathematical & Thomasb\ Department. ofof Physics & Duke of Oklahoma\<|endoftext|>* every research. especially I on strong\ <|endoftext|>Acknowledgements these’s encouragement lectures beautiful encouragementoring over none dissertation could be exist come do...
{ "pile_set_name": "ArXiv" }
Oauthor: |Let prove and general framework of a topological that convolution convolutionay artificialceptron network a call it such works significantly universal test result among training autoLP to C IIST image while bibliography: - 'mult.bib' - 'strings-shortorter.bib' title 'ml.bib' --- ' 'igaionlshorter.bib' --- In...