Observation of B0→pΛˉD(∗)−B^{0} \rightarrow p\barΛ D^{(*)-}

preprint2015arXivOpen access
Y. -Y. ChangM. -Z. WangA. AbdesselamI. AdachiK. AdamczykH. AiharaS. Al SaidD. M. AsnerH. AtmacanT. AushevV. BabuI. BadhreesA. M. BakichE. BarberioB. BhuyanJ. BiswalA. BobrovA. BozekM. BračkoT. E. BrowderD. ČervenkovV. ChekelianA. ChenB. G. CheonK. ChilikinR. ChistovV. ChobanovaS. -K. ChoiY. ChoiD. CinabroJ. DalsenoM. DanilovJ. DingfelderZ. DoležalZ. DrásalD. DuttaS. EidelmanH. FarhatJ. E. FastT. FerberB. G. FulsomV. GaurN. GabyshevS. GangulyA. GarmashR. GillardR. GlattauerY. M. GohP. GoldenzweigD. GreenwaldO. GrzymkowskaJ. HabaK. HayasakaH. HayashiiX. H. HeW. -S. HouC. -L. HsuT. IijimaK. InamiA. IshikawaR. ItohY. IwasakiW. W. JacobsI. JaegleD. JoffeK. K. JooT. KawasakiD. Y. KimH. J. KimJ. B. KimJ. H. KimK. T. KimM. J. KimS. H. KimY. J. KimK. KinoshitaS. KorparP. KrižanP. KrokovnyT. KuhrT. KumitaA. KuzminY. -J. KwonY. -T. LaiI. S. LeeL. LiY. LiJ. LibbyD. LiventsevP. LukiM. MasudaK. MiyabayashiH. MiyakeH. MiyataR. MizukG. B. MohantyS. MohantyA. MollH. K. MoonT. MoriE. NakanoM. NakaoT. NanutM. NayakS. NishidaS. OgawaH. OzakiP. PakhlovG. PakhlovaB. PalC. W. ParkT . K. PedlarR. PestotnikM. PetričL. E. PiilonenJ. RauchE. RibežlM. RitterA. RostomyanS. RyuH. SahooY. SakaiS. SandilyaL. SanteljT. SanukiV. SavinovO. SchneiderG. SchnellC. SchwandaY. SeinoK. SenyoI. S. SeongM. E. SeviorV. ShebalinC. P. ShenT. -A. ShibataJ. -G. ShiuF. SimonY. -S. SohnM. StaričJ. StypulaM. SumihamaK. SumisawaT. SumiyoshiU. TamponiK. TanidaY. TeramotoT. UglovY. UnnoS. UnoY. UsovC. Van HulseP. VanhoeferG. VarnerV. VorobyevA. VossenM. N. WagnerC. H. WangP. WangM. WatanabeY. WatanabeK. M. WilliamsE. WonJ. YamaokaS. YashchenkoJ. YeltonY. YusaZ. P. ZhangV. ZhulanovA. Zupanc

Abstract

We report the first observation of the decays B0→pΛˉD(∗)−B^0 \rightarrow p\barΛ D^{(*)-}. The data sample of 711711 fb−1^{-1} used in this analysis corresponds to 772772 million BBˉB\bar{B} pairs, collected at the Υ(4S)Υ(4S) resonance by the Belle detector at the KEKB asymmetric-energy e+e−e^{+}e^{-} collider. We observe 19.8σ19.8σ and 10.8σ10.8σ excesses of events for the two decay modes and measure the branching fractions of B0→pΛˉD−B^0 \rightarrow p\barΛ D^{-} and B0→pΛˉD∗−B^0 \rightarrow p\barΛ D^{*-} to be (25.1±2.6±3.5)×10−6(25.1\pm2.6\pm3.5)\times10^{-6} and (33.6±6.3±4.4)×10−6(33.6\pm6.3\pm4.4)\times10^{-6}, respectively, where the first uncertainties are statistical and the second are systematic. These results are not compatible with the predictions based on the generalized factorization approach. In addition, a threshold enhancement in the di-baryon (pΛˉp\barΛ) system is observed, consistent with that observed in similar BB decays.

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