Observation of e+e−→π+π−π0χbJe^+e^- \to π^+ π^- π^0 χ_{bJ} and search for Xb→ωΥ(1S)X_b \to ωΥ(1S) at s∼10.867\sqrt{s}\sim 10.867 GeV

preprint2014arXivOpen access
Belle CollaborationX. H. HeC. P. ShenC. Z. YuanY. BanA. AbdesselamI. AdachiH. AiharaD. M. AsnerV. AulchenkoT. AushevR. AyadS. BahinipatiA. M. BakichV. BansalB. BhuyanA. BondarG. BonviciniA. BozekT. E. BrowderD. ČervenkovP. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinR. ChistovK. ChoV. ChobanovaS. -K. ChoiY. ChoiD. CinabroJ. DalsenoM. DanilovZ. DoležalZ. DrásalA. DrutskoyS. EidelmanH. FarhatJ. E. FastT. FerberV. GaurN. GabyshevS. GangulyA. GarmashR. GillardR. GlattauerY. M. GohO. GrzymkowskaJ. HabaK. HayasakaH. HayashiiW. -S. HouT. IijimaA. IshikawaR. ItohY. IwasakiI. JaegleK. K. JooT. JuliusE. KatoT. KawasakiD. Y. KimM. J. KimY. J. KimK. KinoshitaB. R. KoP. KodyšS. KorparP. KrižanP. KrokovnyT. KumitaY. -J. KwonY. LiJ. LibbyD. LiventsevD. MatvienkoH. MiyataR. MizukG. B. MohantyA. MollR. MussaE. NakanoM. NakaoT. NanutZ. NatkaniecE. NedelkovskaN. K. NisarS. NishidaS. OgawaS. OkunoP. PakhlovG. PakhlovaH. ParkT. K. PedlarR. PestotnikM. PetričL. E. PiilonenM. RitterA. RostomyanY. SakaiS. SandilyaL. SanteljT. SanukiY. SatoV. SavinovO. SchneiderG. SchnellC. SchwandaD. SemmlerK. SenyoM. E. SeviorV. ShebalinT. -A. ShibataJ. -G. ShiuB. ShwartzA. SibidanovF. SimonY. -S. SohnA. SokolovE. SolovievaM. StaričM. StederK. SumisawaT. SumiyoshiU. TamponiK. TanidaG. TatishviliY. TeramotoF. ThorneK. TrabelsiM. UchidaS. UeharaT. UglovY. UnnoS. UnoP. UrquijoS. E. VahsenC. Van HulseP. VanhoeferG. VarnerA. VinokurovaV. VorobyevM. N. WagnerC. H. WangM. -Z. WangP. WangX. L. WangM. WatanabeY. WatanabeS. WehleK. M. WilliamsE. WonJ. YamaokaS. YashchenkoY. YookY. YusaZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

The e+e−→π+π−π0χbJe^+e^- \to π^+ π^- π^0 χ_{bJ} (J=0, 1, 2J=0,~1,~2) processes are studied using a 118~fb−1^{-1} data sample collected at a center-of-mass energy of 10.867 GeV, in the Υ(10860)Υ(10860) energy range, with the Belle detector. The π+π−π0χb1π^+ π^- π^0 χ_{b1}, π+π−π0χb2π^+π^-π^0χ_{b2}, ωχb1ωχ_{b1} signals and the evidence of ωχb2ωχ_{b2} are observed for the first time and the cross sections are measured. No significant π+π−π0χb0π^+π^-π^0χ_{b0} or ωχb0ωχ_{b0} signal is observed and 90\% confidence level upper limits on the cross sections for these two processes are obtained. In the π+π−π0π^+π^-π^0 invariant mass spectrum, significant non-ωω signals are also observed. We search for the X(3872)X(3872)-like state with a hidden bbˉb\bar{b} component (named XbX_b) decaying into ωΥ(1S)ωΥ(1S); no significant signal is observed with a mass between 10.5510.55 and 10.6510.65 GeV/c2c^2.

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