Study of the decay Bˉ0→Λc+pˉπ+π−\bar{B}^{0}\rightarrowΛ_{c}^{+}\bar{p}π^{+}π^{-} and its intermediate states

preprint2013arXivOpen access
The BABAR CollaborationJ. P. LeesV. PoireauV. TisserandE. GraugesA. PalanoG. EigenB. StuguD. N. BrownL. T. KerthYu. G. KolomenskyG. LynchH. KochT. SchroederD. J. AsgeirssonC. HeartyT. S. MattisonJ. A. McKennaR. Y. SoA. KhanV. E. BlinovA. R. BuzykaevV. P. DruzhininV. B. GolubevE. A. KravchenkoA. P. OnuchinS. I. SerednyakovYu. I. SkovpenE. P. SolodovK. Yu. TodyshevA. N. YushkovD. KirkbyA. J. LankfordM. MandelkernH. AtmacanJ. W. GaryO. LongG. M. VitugC. CampagnariT. M. HongD. KovalskyiJ. D. RichmanC. A. WestA. M. EisnerJ. KrosebergW. S. LockmanA. J. MartinezB. A. SchummA. SeidenD. S. ChaoC. H. ChengB. EchenardK. T. FloodD. G. HitlinP. OngmongkolkulF. C. PorterA. Y. RakitinR. AndreassenZ. HuardB. T. MeadowsM. D. SokoloffL. SunP. C. BloomW. T. FordA. GazU. NauenbergJ. G. SmithS. R. WagnerR. AyadW. H. TokiB. SpaanK. R. SchubertR. SchwierzD. BernardM. VerderiP. J. ClarkS. PlayferD. BettoniC. BozziR. CalabreseG. CibinettoE. FioravantiI. GarziaE. LuppiL. PiemonteseV. SantoroR. Baldini-FerroliA. CalcaterraR. de SangroG. FinocchiaroP. PatteriI. M. PeruzziM. PiccoloM. RamaA. ZalloR. ContriE. GuidoM. Lo VetereM. R. MongeS. PassaggioC. PatrignaniE. RobuttiB. BhuyanV. PrasadM. MoriiA. AdametzU. UwerH. M. LackerT. LueckP. D. DaunceyU. MallikC. ChenJ. CochranW. T. MeyerS. PrellA. E. RubinA. V. GritsanN. ArnaudM. DavierD. DerkachG. GrosdidierF. Le DiberderA. M. LutzB. MalaescuP. RoudeauM. H. SchuneA. StocchiG. WormserD. J. LangeD. M. WrightC. A. ChavezJ. P. ColemanJ. R. FryE. GabathulerD. E. HutchcroftD. J. PayneC. TouramanisA. J. BevanF. Di LodovicoR. SaccoM. SigamaniG. CowanC. L. DavisA. G. DenigM. FritschW. GradlK. GriessingerA. HafnerE. PrencipeR. J. BarlowG. JacksonG. D. LaffertyE. BehnR. CenciB. HamiltonA. JawaheryD. A. RobertsC. DallapiccolaR. CowanD. DujmicG. SciollaR. CheaibD. LindemannP. M. PatelS. H. RobertsonP. BiassoniN. NeriF. PalomboS. StrackaL. CremaldiR. GodangR. KroegerP. SonnekD. J. SummersX. NguyenM. SimardP. TarasG. De NardoD. MonorchioG. OnoratoC. SciaccaM. MartinelliG. RavenC. P. JessopJ. M. LoSeccoW. F. WangK. HonscheidR. KassJ. BrauR. FreyN. B. SinevD. StromE. TorrenceE. FeltresiN. GagliardiM. MargoniM. MorandinM. PosoccoM. RotondoG. SimiF. SimonettoR. StroiliS. AkarE. Ben-HaimM. BombenG. R. BonneaudH. BriandG. CalderiniJ. ChauveauO. HamonPh. LerusteG. MarchioriJ. OcarizS. SittM. BiasiniE. ManoniS. PacettiA. RossiC. AngeliniG. BatignaniS. BettariniM. CarpinelliG. CasarosaA. CervelliF. FortiM. A. GiorgiA. LusianiB. OberhofA. PerezG. RizzoJ. J. WalshD. Lopes PegnaJ. OlsenA. J. S. SmithF. AnulliR. FacciniF. FerrarottoF. FerroniM. GasperoL. Li GioiM. A. MazzoniG. PireddaC. BüngerO. GrünbergT. HartmannT. LeddigH. SchröderC. VoßR. WaldiT. AdyeE. O. OlaiyaF. F. WilsonS. EmeryG. Hamel de MonchenaultG. VasseurCh. Y\`D. AstonR. BartoldusJ. F. BenitezC. CartaroM. R. ConveryJ. DorfanG. P. Dubois-FelsmannW. DunwoodieM. EbertR. C. FieldM. Franco SevillaB. G. FulsomA. M. GabareenM. T. GrahamP. GrenierC. HastW. R. InnesM. H. KelseyP. KimM. L. KocianD. W. G. S. LeithP. LewisB. LindquistS. LuitzV. LuthH. L. LynchD. B. MacFarlaneD. R. MullerH. NealS. NelsonM. PerlT. PulliamB. N. RatcliffA. RoodmanA. A. SalnikovR. H. SchindlerA. SnyderD. SuM. K. SullivanJ. Va'vraA. P. WagnerW. J. WisniewskiM. WittgenD. H. WrightH. W. WulsinC. C. YoungV. ZieglerW. ParkM. V. PurohitR. M. WhiteJ. R. WilsonA. Randle-CondeS. J. SekulaM. BellisP. R. BurchatT. S. MiyashitaE. M. T. PuccioM. S. AlamJ. A. ErnstR. GorodeiskyN. GuttmanD. R. PeimerA. SofferS. M. SpanierJ. L. RitchieA. M. RulandR. F. SchwittersB. C. WrayJ. M. IzenX. C. LouF. BianchiD. GambaS. ZambitoL. LanceriL. VitaleF. Martinez-VidalA. OyangurenP. Villanueva-PerezH. AhmedJ. AlbertSw. BanerjeeF. U. BernlochnerH. H. F. ChoiG. J. KingR. KowalewskiM. J. LewczukI. M. NugentJ. M. RoneyR. J. SobieN. TasneemT. J. GershonP. F. HarrisonT. E. LathamH. R. BandS. DasuY. PanR. PrepostS. L. Wu

Abstract

We study the decay Bˉ0→Λc+pˉπ+π−\bar{B}^{0}\rightarrowΛ_{c}^{+}\bar{p}π^{+}π^{-}, reconstructing the Λ_{c}^{+} baryon in the pK−π+p K^{-}π^{+} mode, using a data sample of 467×106467\times 10^{6} BBˉB\bar{B} pairs collected with the BaBar detector at the PEP-2 storage rings at SLAC. We measure branching fractions for decays with intermediate ΣcΣ_{c} baryons to be B[Bˉ0→Σc(2455)++pˉπ−]=(21.3±1.0±1.0±5.5)×10−5{\cal B}[\bar{B}^{0}\rightarrowΣ_{c}(2455)^{++}\bar{p}π^{-}]=(21.3 \pm 1.0 \pm 1.0 \pm 5.5) \times 10^{-5}, B[Bˉ0→Σc(2520)++pˉπ−]=(11.5±1.0±0.5±3.0)×10−5{\cal B}[\bar{B}^{0}\rightarrowΣ_{c}(2520)^{++}\bar{p}π^{-}]=(11.5\pm 1.0 \pm 0.5 \pm 3.0)\times 10^{-5}, B[Bˉ0→Σc(2455)0pˉπ+]=(9.1±0.7±0.4±2.4)×10−5{\cal B}[\bar{B}^{0}\rightarrowΣ_{c}(2455)^{0}\bar{p}π^{+}]=(9.1 \pm 0.7 \pm 0.4 \pm 2.4)\times10^{-5}, and B[Bˉ0→Σc(2520)0pˉπ+]=(2.2±0.7±0.1±0.6)×10−5{\cal B}[\bar{B}^{0}\rightarrowΣ_{c}(2520)^{0}\bar{p}π^{+}]= (2.2 \pm 0.7 \pm 0.1\pm 0.6) \times 10^{-5}, where the uncertainties are statistical, systematic, and due to the uncertainty on the $Λ_{c}^{+}\rightarrow\proton\Kmπ^{+}$ branching fraction, respectively. For decays without Σc(2455)Σ_{c}(2455) or Σc(2520)Σ_{c}(2520) resonances, we measure B[Bˉ0→Λc+pˉπ+π−]non−Σc=(79±4±4±20)×10−5{\cal B}[\bar{B}^{0}\rightarrowΛ_{c}^{+}\bar{p}π^{+}π^{-}]_{\mathrm{non-Σ_{c}}}=(79 \pm 4 \pm 4 \pm 20)\times10^{-5}. The total branching fraction is determined to be B[Bˉ0→Λc+pˉπ+π−]total=(123±5±7±32)×10−5{\cal B}[\bar{B}^{0}\rightarrowΛ_{c}^{+}\bar{p}π^{+}π^{-}]_{\mathrm{total}}=(123 \pm 5 \pm 7 \pm 32)\times10^{-5}. We examine multibody mass combinations in the resonant three-particle ΣcpˉπΣ_{c}\bar{p}π final states and in the four-particle Λc+pˉπ+π−Λ_{c}^{+}\bar{p}π^{+}π^{-} final state, and observe different characteristics for the pˉπ\bar{p}π combination in neutral versus doubly-charged ΣcΣ_{c} decays.

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