6533b86ffe1ef96bd12cdb74
RESEARCH PRODUCT
Observation ofB¯→D(*) π+π−ℓ−ν¯Decays ine+e−Collisions at theΥ(4S)Resonance
S. H. RobertsonH. NealHerbert KochR. H. SchindlerK. GriessingerJ. L. RitchieR. FacciniF. FerrarottoA. J. LankfordD. W G S LeithA. R. BuzykaevA. BeaulieuA. RoodmanA. M. LutzF. Le DiberderS. I. SerednyakovJ. R. FryC. H. ChengV. E. BlinovYu. I. SkovpenC. H. ChenG. RizzoM. RamaDmytro KovalskyiJ. P. LeesJ. D. RichmanT. PulliamJ. A. MckennaV. SantoroT. S. MattisonS. PassaggioR. De SangroS. L. WuE. FioravantiC. BüngerR. Y. SoL. M. CremaldiS. PrellM. VerderiR. GodangT. E. LathamA. JawaheryD. J. LangeRoland WaldiDouglas WrightF. FerroniG. PireddaH. W. WulsinW. Panduro VazquezU. MallikZ. C. HuardR. AndreassenW. H. TokiJames H CochranV. PoireauG. CibinettoV. LuthG. LynchCorrado AngeliniStephen SekulaF. De MoriD. G. HitlinA. SnyderN. NeriG. A. CowanD. J. BardA. LusianiAbner SofferD. Lopes PegnaHeiko LackerT. J. GershonV. PrasadF. AnulliV. P. DruzhininA. M. EisnerM. R. ConveryR. CenciA. KhanC. BozziA. ZalloPaul Fraser HarrisonJu-young KimChristopher WestMaurizio BiasiniD. E. HutchcroftT. LeddigRoberto CalabreseT. M. HongM. J. LewczukK. HonscheidH. R. BandC. HeartyN. TasneemW. S. LockmanE. A. KravchenkoGabriele SimiB. BhuyanS. LuitzD. GambaB. G. FulsomOwen Rosser LongA. SeidenP. C. KimElisa ManoniK. R. SchubertC. L. DavisS. PlayferD. J. SummersCrisostomo SciaccaM. V. PurohitRoger BarlowMartino MargoniStephen Robert WagnerN. GuttmanJ. A. ErnstA. AdametzM. FritschGiulia CasarosaM. PosoccoMaria Roberta MongeJ. AlbertG. WormserV. B. GolubevR. J. SobieEleonora LuppiJ. OcarizJ. ChauveauB. StuguL. VitaleA. P. OnuchinI. M. PeruzziL. SunM. HessF. Martinez-vidalDominik MüllerE. PaoloniT. SchroederAidan Randle-condeBruce SchummG. MarchioriP. TarasA. FilippiAdrian John BevanA. PalanoAlessandro PilloniM. Franco SevillaR. C. FieldJ. W. GaryH. AhmedS. MartellottiA. CalcaterraM. CarpinelliP. OngmongkolkulD. R. PeimerM. GasperoR. CowanF. SimonettoA. StocchiA. OyangurenD. AstonR. CheaibF. BianchiB. MalaescuC. CartaroJ. P. ColemanAndrei GritsanM. T. GrahamD. B. MacfarlaneMarco BombenW. R. InnesW. J. WisniewskiS. DittrichJ. J. WalshR. F. SchwittersF. FortiC. TouramanisW. T. FordD. BettoniA. G. DenigB. N. RatcliffTim AdyeJ. M. LoseccoI. M. NugentR. D. KassE. GraugesX. C. LouO. GrünbergD. N. BrownB. DeyP. RoudeauMario GiorgiY. B. PanP. PatteriR. KowalewskiG. J. KingSridhara DasuYu. G. KolomenskyJ. DorfanD. S. ChaoColin JessopR. GorodeiskyM. SimardD. A. RobertsR. PrepostPh LerusteN. ArnaudM. DavierG. VasseurK. T. FloodE. O. OlaiyaM. J. LeeFlorian Urs BernlochnerF. PalomboT. LueckJames D. OlsenG. GrosdidierB. HamiltonM. EbertA. M. RossiJoseph IzenC. HastL. T. KerthA. HafnerP. M. PatelG. R. BonneaudE. M. T. PuccioI. GarziaG. CalderiniC. PatrignaniV. TisserandG. P. Dubois-felsmannE. GabathulerF. C. PorterSimon AkarM. ChrzaszczC. VoßG. OnoratoSw. BanerjeeW. DunwoodieB. T. MeadowsG. RavenM. D. SokoloffP. R. BurchatR. SaccoA. J.s. SmithR. AyadJames R. WilsonH. BriandG. EigenStefan SpanierM. MorandinU. UwerR. StroiliE. P. SolodovT. S. MiyashitaM. BellisM. RotondoG. De NardoM. RöhrkenB. G. PushpawelaD. SuM. PiccoloG. BatignaniE. Ben-haimDenis DerkachF. Di LodovicoR. ContriD. J. PayneG. FinocchiaroM. S. AlamB. EchenardM. K. SullivanD. BernardJ. M. RoneyF. F. WilsonB. OberhofJ. Va'vraS. BettariniJ. G. SmithK. Yu. TodyshevB. SpaanH. H. F. ChoiW. GradlS. EmeryL. LanceriG. D. Laffertysubject
PhysicsParticle physicsMuonMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationHadronGeneral Physics and Astronomy01 natural sciencesB-factoryIsospin0103 physical sciencesB meson010306 general physicsdescription
We report on measurements of the decays of B¯ mesons into the semileptonic final states B¯→D^(*)π^(+)π^(-)l^(-)ν¯, where D^(*) represents a D or D^(*) meson and l^(-) is an electron or a muon. These measurements are based on 471×10^(6) BB ¯ pairs recorded with the BABAR detector at the SLAC asymmetric B factory PEP-II. We determine the branching fraction ratios R_{π^{+}π^{-}}^{(*)}=B(B[over ¯]→D^{(*)}π^{+}π^{-}l^{-}ν[over ¯])/B(B[over ¯]→D^{(*)}l^{-}ν[over ¯]) using events in which the second B meson is fully reconstructed. We find R_{π^{+}π^{-}}=0.067±0.010±0.008 and R_{π^{+}π^{-}}^{*}=0.019±0.005±0.004, where the first uncertainty is statistical and the second is systematic. Based on these results and assuming isospin invariance, we estimate that B[over ¯]→D^{(*)}ππl^{-}ν[over ¯] decays, where π denotes either a π^{±} and π^{0} meson, account for up to half the difference between the measured inclusive semileptonic branching fraction to charm hadrons and the corresponding sum of previously measured exclusive branching fractions.
year | journal | country | edition | language |
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2016-01-26 | Physical Review Letters |