6533b833fe1ef96bd129b64f
RESEARCH PRODUCT
Analysis of theD+→K−π+e+νedecay channel
V. SordiniC. HeartyV. PrasadRoberto CalabreseJ. M. RoneyG. MancinelliV. E. BlinovD. J. SummersJ. OcarizP. PatteriM. TibbettsG. M. VitugJ. G. SmithDouglas WrightMatteo RamaS. PrellJames H CochranV. PoireauA. LusianiB. N. RatcliffG. R. BonneaudM. BombenR. J. SobieH. R. BandT. M. HongL. VitaleF. Martinez-vidalJ. W. GaryS. ParamesvaranE. TorrenceD. E. HutchcroftC. DallapiccolaT. LeddigB. BhuyanS. DasuB. G. FulsomA. AdametzD. LindemannDominik MüllerT. M. KarbachElisa GuidoJ. L. RitchieM. BondioliM. MuneratoHeiko LackerD. W. G. S. LeithW. S. LockmanP. TarasE. P. SolodovM. GasperoJ. P. ColemanR. SchwierzJ. StrubeI. L. OsipenkovK. E. AlwynT. S. MattisonJ. M. LoseccoF. Di LodovicoJ. R. FryL. Li GioiM. R. ConveryL. PiemonteseD. J. PayneU. NauenbergA. J. EdwardsC. P. GradyM. ZitoC. H. ChengD. J. BardM. FritschE. C. MartinT. J. GershonT. J. GershonR. EckmannG. CalderiniT. SchalkE. M.t. PuccioE. M.t. PuccioC. HastD. J. LangeG. PireddaN. B. SinevPrafulla Kumar BeheraN. Lopez-marchGiulia CasarosaHyun-chul KimG. LynchA. VolkM. K. SullivanChunhui ChenM. A. MazzoniK. SuzukiG. WormserSilvano TosiH. A. NealD. MonorchioC. C. YoungW. T. MeyerM. PappagalloR. De SangroE. GabathulerW. R. InnesW. GradlF. C. PorterN. L. BlountM. MoriiI. OfteJ. Va’vraM. L. KocianC. A. HeuschD. J. AsgeirssonAbner SofferF. SimonettoR. H. SchindlerR. AndreassenP. BiassoniM. VerderiR. ContriJ. ChauveauX. R. ChenM. NicolaciR. C. FieldP. D. DaunceyS. B. ZainE. O. OlaiyaM. A. SaeedG. FinocchiaroV. LuthT. HartmannT. SchroederW. H. TokiU. MallikT. E. LathamT. E. LathamM. SchramF. U. BernlochnerG. J. KingM. J. LewczukMirco AndreottiBruce SchummF. PalomboMartino MargoniJ. P. MorrisW. DunwoodieP. SonnekK. J. KnoepfelG. De NardoCh YècheJames D. OlsenA. R. BuzykaevA. G. DenigJ. E. BrauD. DujmicElisa ManoniM. S. AlamR. KroegerS. AhmedD. GambaMaria A. NagelT. S. MiyashitaA. SnyderS. PlayferE. SalvatiB. FranekL. T. KerthA. StocchiF. F. WilsonE. A. KravchenkoC. LindsayP. J. ClarkG. JacksonClaudio CampagnariV. P. LombardoJ. PrendkiCorrado AngeliniA. V. TelnovD. A. DollA. P. WagnerMauro MorandinB. EchenardD. BernardD. BettoniN. GuttmanH. JasperM. T. GrahamR. GodangR. GodangMarcello RotondoM. SigamaniL. M. CremaldiJ. SchwieningX. C. LouE. I. RosenbergF. AnulliA. A. SalnikovF. FortiAidan Randle-condeA. M. EisnerL. O. WinstromC. LuH. L. LynchOlga IgonkinaStephen SekulaD. Lopes PegnaA. M. RulandMaria Roberta MongeJ. A. MckennaE. PaoloniY. PanJ. J. WalshJ. Firmino Da CostaC. L. LeeS. M. SpanierAlessandro GazS. H. RobertsonYu. G. KolomenskyA. PetzoldS. BettariniR. FreyM. H. KelseyP. LundA. KhanD. S. BaileyD. N. BrownCrisostomo SciaccaD. AstonA. M. GabareenM. J. KobelG. CastelliG. Hamel De MonchenaultJ. AndersonD. M. StromW. T. FordTim AdyeB. StuguG. MarchioriO. HamonR. D. KassV. P. DruzhininC. BozziGeorge LaffertyA. OyangurenA. CalcaterraH. AtmacanDmytro KovalskyiJ. P. LeesJ. DorfanHerbert KochX. NguyenS. CurryC. J. SchillingAndrei GritsanD. G. HitlinA. CecchiH. H. F. ChoiS. EmeryR. BartoldusT. LueckGabriele SimiM. S. DubrovinM. V. PurohitJ. AlbertE. BaracchiniE. PrencipeL. DongC. O. VuosaloChristopher WestK. HonscheidW. F. WangC. A. ChavezC. L. DavisG. P. Dubois-felsmannM. WittgenR. GametA. J. MartinezB. C. WrayJ. F. BenitezI. GarziaD. P. StokerD. H. WrightYu I. SkovpenC. TouramanisR. AyadR. AyadR. J. BarlowShouheng SunC. PatrignaniNicola NeriR. FacciniL. A. CorwinD. A. MilanesShu LiV. TisserandF. FerrarottoA. J. LankfordF. Le DiberderPh LerusteP. FranchiniMatteo NegriniD. SuN. ArnaudM. PosoccoV. ZieglerAlessandro RossiM. Lo VetereA. N. YushkovB. SpaanA. K. YarrituJ. D. RichmanM. PiccoloJ. M. ThompsonH. SchröderS. LuitzM. T. AllenK. T. FloodV. SantoroSw. BanerjeeB. PanP. Del Amo SanchezG. BatignaniL. LanceriI. M. PeruzziJ. MarksF. RengaG. A. CowanR. PrepostKenji HamanoH. B. CrawleyR. RahmatA. PetrellaV. B. GolubevB. LindquistM. MandelkernP. KimE. Ben-haimR. M. WhiteM. Franco SevillaA. C. WrenC. CartaroS. PacettiR. CowanR. KowalewskiS. I. SerednyakovH. W. WulsinF. BianchiPhilippe GrenierA. E. RubinA. Y. RakitinMario PelliccioniG. RizzoP. RoudeauS. NelsonJ. E. WatsonDenis DerkachM. CarpinelliMaurizio BiasiniEnrico RobuttiB. MalaescuM. SimardD. A. RobertsG. GrosdidierOwen Rosser LongA. SeidenSau Lan WuP. OngmongkolkulJ. A. ErnstL. SunAlberto CervelliAdrian John BevanI. M. NugentJ. Garra TicoM. ZhaoL. WangR. F. SchwittersD. B. MacfarlaneM. DavierA. RoodmanA. PerezE. FioravantiT. PulliamM. BellisRoland WaldiF. FerroniJ. SerranoP. C. BloomP. M. PatelStephen Robert WagnerJ. M. TuggleF. LiuK. R. SchubertA. LazzaroR. SaccoG. SciollaH. L. SnoekM. L. PerlZ. J. GuoK. Yu TodyshevM. H. SchuneJoseph IzenU. UwerR. StroiliJames R. WilsonH. BriandA. J.s. SmithG. OnoratoG. EigenB. T. MeadowsG. RavenM. D. SokoloffP. R. BurchatColin JessopM. WeaverR. Baldini-ferroliD. KirkbyG. VasseurJ. A. KolbH. MarsiskeR. CenciA. ZalloA. M. LutzEleonora LuppiW. ParkW. J. WisniewskiP. F. HarrisonP. F. HarrisonE. GraugesS. PassaggioMario GiorgiM. EbertS. SittA. PalanoA. HafnerJ. KrosebergG. CavotoN. GagliardiS. StrackaA. JawaheryG. CibinettoE. FeltresiA. P. OnuchinI. BinghamMaurizio Martinellisubject
PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationMomentum transferHadronForm factor (quantum field theory)Value (computer science)01 natural sciencesMeasure (mathematics)law.inventionNuclear physicslaw0103 physical sciences010306 general physicsColliderdescription
Using 347.5 fb^(-1) of data recorded by the BABAR detector at the PEP-II electron-positron collider, 244×10^3 signal events for the D^+ → K^-π^+e^+ν_e decay channel are analyzed. This decay mode is dominated by the K ^*(892)^0 contribution. We determine the K ^*(892)^0 parameters: m_(K^*(892)^0)=(895.4±0.2±0.2) MeV/c^2, Γ_(K^*(892)^0)=(46.5±0.3±0.2) MeV/c^2, and the Blatt-Weisskopf parameter r_(BW) =2.1±0.5±0.5 (GeV/c)^-1, where the first uncertainty comes from statistics and the second from systematic uncertainties. We also measure the parameters defining the corresponding hadronic form factors at q^2 = 0 (r_V = ^(V(0))/_(A1(0)) = 1.463 ± 0.017 ± 0.031, r_2 = _(A1(0)) ^(A2(0))= 0.801±0.020±0.020) and the value of the axial-vector pole mass parametrizing the q^2 variation of A_1 and A_2: m_A=(2.63±0.10±0.13) GeV/c^2. The S-wave fraction is equal to (5.79±0.16±0.15)%. Other signal components correspond to fractions below 1%. Using the D^+ → K^-π^+π^+ channel as a normalization, we measure the D^+ semileptonic branching fraction: B(D^+ → K^-π^+e^+ν_e)=(4.00±0.03±0.04±0.09)×10^(-2), where the third uncertainty comes from external inputs. We then obtain the value of the hadronic form factor A_1 at q^2=0: A_1(0)=0.6200±0.0056±0.0065±0.0071. Fixing the P-wave parameters, we measure the phase of the S wave for several values of the Kπ mass. These results confirm those obtained with Kπ production at small momentum transfer in fixed target experiments.
year | journal | country | edition | language |
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2011-04-01 | Physical Review D |