6533b7cffe1ef96bd1258cff

RESEARCH PRODUCT

Measurement of the semileptonic decaysB¯→Dτ−ν¯τandB¯→D*τ−ν¯τ

B. AubertM. BonaY. KaryotakisJ. P. LeesV. PoireauE. PrencipeX. PrudentV. TisserandJ. Garra TicoE. GraugesL. LopezA. PalanoM. PappagalloG. EigenB. StuguL. SunG. S. AbramsM. BattagliaD. N. BrownR. G. JacobsenL. T. KerthYu. G. KolomenskyG. LynchI. L. OsipenkovM. T. RonanK. TackmannT. TanabeC. M. HawkesN. SoniA. T. WatsonH. KochT. SchroederD. J. AsgeirssonB. G. FulsomC. HeartyT. S. MattisonJ. A. MckennaM. BarrettA. KhanV. E. BlinovA. D. BukinA. R. BuzykaevV. P. DruzhininV. B. GolubevA. P. OnuchinS. I. SerednyakovYu. I. SkovpenE. P. SolodovK. Yu. TodyshevM. BondioliS. CurryI. EschrichD. KirkbyA. J. LankfordP. LundM. MandelkernE. C. MartinD. P. StokerS. AbachiC. BuchananH. AtmacanJ. W. GaryF. LiuO. LongG. M. VitugZ. YasinL. ZhangV. SharmaC. CampagnariT. M. HongD. KovalskyiM. A. MazurJ. D. RichmanT. W. BeckA. M. EisnerC. J. FlaccoC. A. HeuschJ. KrosebergW. S. LockmanA. J. MartinezT. SchalkB. A. SchummA. SeidenM. G. WilsonL. O. WinstromC. H. ChengD. A. DollB. EchenardF. FangD. G. HitlinI. NarskyT. PiatenkoF. C. PorterR. AndreassenG. MancinelliB. T. MeadowsK. MishraM. D. SokoloffP. C. BloomW. T. FordA. GazJ. F. HirschauerM. NagelU. NauenbergJ. G. SmithS. R. WagnerR. AyadA. SofferW. H. TokiR. J. WilsonE. FeltresiA. HaukeH. JasperM. KarbachJ. MerkelA. PetzoldB. SpaanK. WackerM. J. KobelR. NogowskiK. R. SchubertR. SchwierzA. VolkD. BernardG. R. BonneaudE. LatourM. VerderiP. J. ClarkS. PlayferJ. E. WatsonM. AndreottiD. BettoniC. BozziR. CalabreseA. CecchiG. CibinettoP. FranchiniE. LuppiM. NegriniA. PetrellaL. PiemonteseV. SantoroR. Baldini-ferroliA. CalcaterraR. De SangroG. FinocchiaroS. PacettiP. PatteriI. M. PeruzziM. PiccoloM. RamaA. ZalloA. BuzzoR. ContriM. Lo VetereM. M. MacriM. R. MongeS. PassaggioC. PatrignaniE. RobuttiA. SantroniS. TosiK. S. ChaisanguanthumM. MoriiA. AdametzJ. MarksS. SchenkU. UwerV. KloseH. M. LackerD. J. BardP. D. DaunceyM. TibbettsP. K. BeheraX. ChaiM. J. CharlesU. MallikJ. CochranH. B. CrawleyL. DongW. T. MeyerS. PrellE. I. RosenbergA. E. RubinY. Y. GaoA. V. GritsanZ. J. GuoC. K. LaeN. ArnaudJ. BéquilleuxA. D’orazioM. DavierJ. Firmino Da CostaG. GrosdidierF. Le DiberderV. LepeltierA. M. LutzS. PruvotP. RoudeauM. H. SchuneJ. SerranoV. SordiniA. StocchiG. WormserD. J. LangeD. M. WrightI. BinghamJ. P. BurkeC. A. ChavezJ. R. FryE. GabathulerR. GametD. E. HutchcroftD. J. PayneC. TouramanisA. J. BevanC. K. ClarkeF. Di LodovicoR. SaccoM. SigamaniG. CowanS. ParamesvaranA. C. WrenD. N. BrownC. L. DavisA. G. DenigM. FritschW. GradlK. E. AlwynD. BaileyR. J. BarlowG. JacksonG. D. LaffertyT. J. WestJ. I. YiJ. AndersonC. ChenA. JawaheryD. A. RobertsG. SimiJ. M. TuggleC. DallapiccolaX. LiE. SalvatiS. SaremiR. CowanD. DujmicP. H. FisherS. W. HendersonG. SciollaM. SpitznagelF. TaylorR. K. YamamotoM. ZhaoP. M. PatelS. H. RobertsonA. LazzaroV. LombardoF. PalomboJ. M. BauerL. CremaldiR. GodangR. KroegerD. J. SummersH. W. ZhaoM. SimardP. TarasH. NicholsonG. De NardoL. ListaD. MonorchioG. OnoratoC. SciaccaG. RavenH. L. SnoekC. P. JessopK. J. KnoepfelJ. M. LoseccoW. F. WangL. A. CorwinK. HonscheidH. KaganR. KassJ. P. MorrisA. M. RahimiJ. J. RegensburgerS. J. SekulaQ. K. WongN. L. BlountJ. BrauR. FreyO. IgonkinaJ. A. KolbM. LuR. RahmatN. B. SinevD. StromJ. StrubeE. TorrenceG. CastelliN. GagliardiM. MargoniM. MorandinM. PosoccoM. RotondoF. SimonettoR. StroiliC. VociP. Del Amo SanchezE. Ben-haimH. BriandG. CalderiniJ. ChauveauO. HamonPh. LerusteJ. OcarizA. PerezJ. PrendkiS. SittL. GladneyM. BiasiniE. ManoniC. AngeliniG. BatignaniS. BettariniM. CarpinelliA. CervelliF. FortiM. A. GiorgiA. LusianiG. MarchioriM. MorgantiN. NeriE. PaoloniG. RizzoJ. J. WalshD. Lopes PegnaC. LuJ. OlsenA. J. S. SmithA. V. TelnovF. AnulliE. BaracchiniG. CavotoR. FacciniF. FerrarottoF. FerroniM. GasperoP. D. JacksonL. Li GioiM. A. MazzoniS. MorgantiG. PireddaF. RengaC. VoenaM. EbertT. HartmannH. SchröderR. WaldiT. AdyeB. FranekE. O. OlaiyaF. F. WilsonS. EmeryM. EscalierL. EsteveG. Hamel De MonchenaultW. KozaneckiG. VasseurCh. YècheM. ZitoX. R. ChenH. LiuW. ParkM. V. PurohitR. M. WhiteJ. R. WilsonM. T. AllenD. AstonR. BartoldusJ. F. BenitezR. CenciJ. P. ColemanM. R. ConveryJ. C. DingfelderJ. DorfanG. P. Dubois-felsmannW. DunwoodieR. C. FieldA. M. GabareenM. T. GrahamP. GrenierC. HastW. R. InnesJ. KaminskiM. H. KelseyH. KimP. KimM. L. KocianD. W. G. S. LeithS. LiB. LindquistS. LuitzV. LuthH. L. LynchD. B. MacfarlaneH. MarsiskeR. MessnerD. R. MullerH. NealS. NelsonC. P. O’gradyI. OfteM. PerlB. N. RatcliffA. RoodmanA. A. SalnikovR. H. SchindlerJ. SchwieningA. SnyderD. SuM. K. SullivanK. SuzukiS. K. SwainJ. M. ThompsonJ. Va’vraA. P. WagnerM. WeaverC. A. WestW. J. WisniewskiM. WittgenD. H. WrightH. W. WulsinA. K. YarrituK. YiC. C. YoungV. ZieglerP. R. BurchatA. J. EdwardsT. S. MiyashitaS. AhmedM. S. AlamJ. A. ErnstB. PanM. A. SaeedS. B. ZainS. M. SpanierB. J. WogslandR. EckmannJ. L. RitchieA. M. RulandC. J. SchillingR. F. SchwittersB. W. DrummondJ. M. IzenX. C. LouF. BianchiD. GambaM. PelliccioniM. BombenL. BosisioC. CartaroG. Della RiccaL. LanceriL. VitaleV. AzzoliniN. Lopez-marchF. Martinez-vidalD. A. MilanesA. OyangurenJ. AlbertSw. BanerjeeB. BhuyanH. H. F. ChoiK. HamanoR. KowalewskiM. J. LewczukI. M. NugentJ. M. RoneyR. J. SobieT. J. GershonP. F. HarrisonJ. IlicT. E. LathamG. B. MohantyH. R. BandX. ChenS. DasuK. T. FloodY. PanR. PrepostC. O. VuosaloS. L. Wu

subject

Semileptonic decayPhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilation01 natural sciencesCrystallographyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesB meson010306 general physicsLepton

description

We present measurements of the semileptonic decays B{sup -}{yields}D{sup 0}{tau}{sup -}{nu}{sub {tau}}, B{sup -}{yields}D*{sup 0}{tau}{sup -}{nu}{sub {tau}}, B{sup 0}{yields}D{sup +}{tau}{sup -}{nu}{sub {tau}}, and B{sup 0}{yields}D*{sup +}{tau}{sup -}{nu}{sub {tau}}, which are sensitive to non-standard model amplitudes in certain scenarios. The data sample consists of 232x10{sup 6} {upsilon}(4S){yields}BB decays collected with the BABAR detector at the PEP-II e{sup +}e{sup -} collider. We select events with a D or D* meson and a light lepton (l=e or {mu}) recoiling against a fully reconstructed B meson. We perform a fit to the joint distribution of lepton momentum and missing mass squared to distinguish signal B{yields}D{sup (*)}{tau}{sup -}{nu}{sub {tau}}({tau}{sup -}{yields}l{sup -}{nu}{sub l}{nu}{sub {tau}}) events from the backgrounds, predominantly B{yields}D{sup (*)}l{sup -}{nu}{sub l}. We measure the branching-fraction ratios R(D){identical_to}B(B{yields}D{tau}{sup -}{nu}{sub {tau}})/B(B{yields}Dl{sup -}{nu}{sub l}) and R(D{sup *}){identical_to}B(B{yields}D*{tau}{sup -}{nu}{sub {tau}})/B(B{yields}D*l{sup -}{nu}{sub l}) and, from a combined fit to B{sup -} and B{sup 0} channels, obtain the results R(D)=(41.6{+-}11.7{+-}5.2)% and R(D*)=(29.7{+-}5.6{+-}1.8)%, where the uncertainties are statistical and systematic. Normalizing to measured B{sup -}{yields}D{sup (*)0}l{sup -}{nu}{sub l} branching fractions, we obtain B(B{yields}D{tau}{sup -}{nu}{sub {tau}})=(0.86{+-}0.24{+-}0.11{+-}0.06)% and B(B{yields}D*{tau}{sup -}{nu}{sub {tau}})=(1.62{+-}0.31{+-}0.10{+-}0.05)%, where the additional third uncertainty is from the normalization mode. We also present, for the first time, distributions of the lepton momentum,more » |p{sub l}{sup *}|, and the squared momentum transfer, q{sup 2}.« less

https://doi.org/10.1103/physrevd.79.092002