Semi-inclusive studies of semileptonic BsB_s decays at Belle

preprint2015arXivOpen access
Belle CollaborationC. OswaldP. UrquijoJ. DingfelderA. AbdesselamI. AdachiH. AiharaS. Al SaidD. M. AsnerT. AushevR. AyadV. BabuI. BadhreesA. M. BakichV. BhardwajA. BobrovG. BonviciniA. BozekM. BračkoT. E. BrowderD. ČervenkovM. -C. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinK. ChoV. ChobanovaY. ChoiD. CinabroJ. DalsenoZ. DoležalZ. DrásalA. DrutskoyD. DuttaS. EidelmanH. FarhatJ. E. FastT. FerberO. FrostB. G. FulsomV. GaurN. GabyshevS. GangulyA. GarmashD. GetzkowR. GillardR. GlattauerY. M. GohP. GoldenzweigB. GolobO. GrzymkowskaT. HaraJ. HasenbuschK. HayasakaH. HayashiiX. H. HeW. -S. HouM. HuschleH. J. HyunT. IijimaA. IshikawaR. ItohY. IwasakiI. JaegleT. JuliusK. H. KangP. KapustaE. KatoT. KawasakiC. KieslingD. Y. KimJ. B. KimJ. H. KimK. T. KimM. J. KimS. H. KimY. J. KimK. KinoshitaB. R. KoP. KodyšS. KorparP. KrižanP. KrokovnyT. KuhrT. KumitaY. -J. KwonJ. S. LangeD. H. LeeI. S. LeeY. LiL. Li GioiJ. LibbyD. LiventsevP. LukinD. MatvienkoH. MiyataR. MizukG. B. MohantyA. MollH. K. MoonE. NakanoM. NakaoH. NakazawaT. NanutZ. NatkaniecM. NayakS. NishidaT. NozakiS. OkunoP. PakhlovG. PakhlovaC. W. ParkH. ParkT. K. PedlarL. PesántezR. PestotnikM. PetričL. E. PiilonenC. PulvermacherE. RibežlM. RitterA. RostomyanM. RozanskaS. RyuY. SakaiS. SandilyaL. SanteljT. SanukiY. SatoV. SavinovO. SchneiderG. SchnellC. SchwandaD. SemmlerK. SenyoO. SeonM. E. SeviorM. ShapkinV. ShebalinC. P. ShenT. -A. ShibataJ. -G. ShiuA. SibidanovF. SimonY. -S. SohnE. SolovievaS. StaničM. StaričJ. StypulaM. SumihamaT. SumiyoshiU. TamponiY. TeramotoK. TrabelsiM. UchidaY. UnnoS. UnoY. UsovC. Van HulseP. VanhoeferG. VarnerA. VinokurovaV. VorobyevA. VossenM. N. WagnerC. H. WangM. -Z. WangP. WangX. L. WangY. WatanabeK. M. WilliamsE. WonH. YamamotoS. YashchenkoY. YookZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

We present an analysis of the semi-inclusive decays Bs→Ds−Xℓ+νB_s \to D_s^- X \ell^+ ν and Bs→Ds∗−Xℓ+νB_s \to D_s^{*-} X \ell^+ ν, where XX denotes a final state that may consist of additional hadrons or photons and ℓ\ell is an electron or muon. The studied BsB_s decays are contained in the 121.4 fb−1121.4~{\rm fb}^{-1} Υ(5S)Υ(5S) data sample collected by the Belle detector at the KEKB asymmetric-energy e+e−e^+e^- collider. The branching fractions of the decays are measured to be B(Bs→Ds−Xℓ+ν)=[8.2±0.2(stat)±0.6(syst)±1.4(ext)]%\mathcal{B}(B_s \to D_s^- X \ell^+ ν) = [8.2 \pm 0.2 (\text{stat}) \pm 0.6 (\text{syst}) \pm 1.4 (\text{ext})]\% and B(Bs→Ds∗−Xℓ+ν)=[5.4±0.4(stat)±0.4(syst)±0.9(ext)]%\mathcal{B}(B_s \to D_s^{*-} X \ell^+ ν) = [5.4 \pm 0.4 (\text{stat}) \pm 0.4 (\text{syst}) \pm 0.9 (\text{ext})]\%, where the first two uncertainties are statistical and systematic and the last is due to external parameters. The measurement also provides an estimate of the Bs(∗)Bˉs(∗)B_s^{(*)}\bar{B}_s^{(*)} production cross-section, σ(e+e−→Bs(∗)Bˉs(∗))=(53.8±1.4(stat)±4.0(syst)±3.4(ext)) pbσ(e^+e^- \to B_s^{(*)}\bar{B}_s^{(*)}) = (53.8 \pm 1.4 (\text{stat}) \pm 4.0 (\text{syst}) \pm 3.4 (\text{ext}))\,{\rm pb}, at the center-of-mass energy s=10.86 GeV\sqrt{s} = 10.86\,{\rm GeV}.

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