Search for XYZXYZ states in Υ(1S)Υ(1S) inclusive decays

preprint2016arXivOpen access
Belle CollaborationC. P. ShenC. Z. YuanY. BanH. AiharaD. M. AsnerI. BadhreesA. M. BakichE. BarberioP. BeheraV. BhardwajB. BhuyanJ. BiswalA. BondarG. BonviciniA. BozekM. BračkoT. E. BrowderD. ČervenkovV. ChekelianA. ChenK. ChilikinR. ChistovK. ChoV. ChobanovaS. -K. ChoiY. ChoiD. CinabroJ. DalsenoM. DanilovN. DashS. Di CarloZ. DoležalZ. DrásalD. DuttaS. EidelmanH. FarhatJ. E. FastT. FerberB. G. FulsomV. GaurN. GabyshevA. GarmashP. GoldenzweigJ. HabaK. HayasakaH. HayashiiW. -S. HouT. IijimaG. IngugliaA. IshikawaR. ItohW. W. JacobsH. B. JeonK. K. JooT. JuliusK. H. KangD. Y. KimJ. B. KimK. T. KimS. H. KimY. J. KimK. KinoshitaP. KodyšS. KorparD. KotchetkovP. KrižanP. KrokovnyT. KuhrA. KuzminY. -J. KwonJ. S. LangeC. H. LiH. LiL. LiY. LiL. Li GioiJ. LibbyD. LiventsevT. LuoM. MasudaT. MatsudaD. MatvienkoA. MollH. K. MoonR. MussaM. NakaoT. NanutK. J. NathZ. NatkaniecM. NayakK. NegishiS. NishidaS. OgawaS. OkunoS. L. OlsenP. PakhlovG. PakhlovaB. PalR. PestotnikM. PetričL. E. PiilonenC. PulvermacherM. RitterA. RostomyanY. SakaiS. SandilyaL. SanteljT. SanukiV. SavinovT. SchlüterO. SchneiderG. SchnellC. SchwandaY. SeinoK. SenyoO. SeonI. S. SeongM. E. SeviorT. -A. ShibataJ. -G. ShiuF. SimonA. SokolovE. SolovievaM. StaričT. SumiyoshiM. TakizawaK. TanidaF. TenchiniK. TrabelsiM. UchidaT. UglovY. UnnoS. UnoG. VarnerA. VinokurovaV. VorobyevC. H. WangM. -Z. WangP. WangX. L. WangM. WatanabeY. WatanabeK. M. WilliamsE. WonJ. YamaokaS. D. YangS. YashchenkoY. YookY. YusaZ. P. ZhangV. ZhilichV. ZhukovaV. ZhulanovA. Zupanc

Abstract

The branching fractions of the Υ(1S)Υ(1S) inclusive decays into final states with a J/ψJ/ψ or a ψ(2S)ψ(2S) are measured with improved precision to be $\BR(Υ(1S)\to J/ψ+ {\rm anything})=(5.25\pm 0.13(\mathrm{stat.})\pm 0.25(\mathrm{syst.}))\times 10^{-4}$ and $\BR(Υ(1S)\to ψ(2S) + {\rm anything})=(1.23\pm 0.17(\mathrm{stat.})\pm 0.11(\mathrm{syst.}))\times 10^{-4}$. The first search for Υ(1S)Υ(1S) decays into XYZXYZ states that decay into a J/ψJ/ψ or a ψ(2S)ψ(2S) plus one or two charged tracks yields no significant signals for XYZXYZ states in any of the examined decay modes, and upper limits on their production rates in Υ(1S)Υ(1S) inclusive decays are determined.

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