First observation of exclusive Υ(1S)Υ(1S) and Υ(2S)Υ(2S) decays into light hadrons

preprint2012arXivOpen access
Belle CollaborationC. P. ShenC. Z. YuanT. IijimaI. AdachiH. AiharaD. M. AsnerT. AushevA. M. BakichA. BayK. BelousB. BhuyanM. BischofbergerG. BonviciniA. BozekM. BračkoT. E. BrowderM. -C. ChangP. ChangA. ChenP. ChenB. G. CheonK. ChilikinR. ChistovI. -S. ChoK. ChoS. -K. ChoiY. ChoiJ. DalsenoZ. DoležalZ. DrásalS. EidelmanJ. E. FastV. GaurN. GabyshevY. M. GohB. GolobJ. HabaH. HayashiiY. HoriiY. HoshiW. -S. HouY. B. HsiungH. J. HyunK. InamiA. IshikawaR. ItohM. IwabuchiY. IwasakiT. IwashitaT. JuliusJ. H. KangT. KawasakiC. KieslingB. H. KimH. O. KimJ. B. KimJ. H. KimM. J. KimY. J. KimK. KinoshitaB. R. KoS. KoblitzP. KodyšS. KorparR. T. KouzesP. KrižanP. KrokovnyR. KumarT. KumitaA. KuzminY. -J. KwonS. -H. LeeJ. LiY. LiJ. LibbyC. LiuY. LiuZ. Q. LiuR. LouvotS. McOnieK. MiyabayashiH. MiyataG. B. MohantyD. MohapatraA. MollN. MuramatsuE. NakanoM. NakaoZ. NatkaniecS. NishidaK. NishimuraO. NitohS. OgawaT. OhshimaS. OkunoS. L. OlsenP. PakhlovG. PakhlovaC. W. ParkH. ParkH. K. ParkT. K. PedlarR. PestotnikM. PetričL. E. PiilonenM. RitterH. SahooY. SakaiD. SantelT. SanukiY. SatoO. SchneiderC. SchwandaK. SenyoO. SeonM. E. SeviorM. ShapkinV. ShebalinT. -A. ShibataJ. -G. ShiuB. ShwartzA. SibidanovF. SimonP. SmerkolY. -S. SohnA. SokolovE. SolovievaM. StaričM. SumihamaT. SumiyoshiG. TatishviliY. TeramotoM. UchidaS. UeharaT. UglovY. UnnoS. UnoP. UrquijoY. UsovP. VanhoeferG. VarnerC. H. WangP. WangX. L. WangM. WatanabeY. WatanabeK. M. WilliamsE. WonB. D. YabsleyY. YamashitaC. C. ZhangZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

Using samples of 102 million Υ(1S)Υ(1S) and 158 million Υ(2S)Υ(2S) events collected with the Belle detector, we study exclusive hadronic decays of these two bottomonium resonances to the three-body final states ϕK+K−ϕK^+ K^-, ωπ+π−ωπ^+ π^- and K∗0(892)K−π+K^{\ast 0}(892) K^- π^+ , and to the two-body Vector-Tensor (ϕf2′(1525)ϕf_2'(1525), ωf2(1270)ωf_2(1270), ρa2(1320)ρa_2(1320) and K∗0(892)Kˉ2∗0(1430)K^{\ast 0}(892) \bar{K}_2^{\ast 0}(1430) ) and Axial-vector-Pseudoscalar (K1(1270)+K−K_1(1270)^+ K^-, K1(1400)+K−K_1(1400)^+ K^- and b1(1235)+π−b_1(1235)^+ π^- ) pairs. Signals are observed for the first time in the Υ(1S)→ϕK+K−Υ(1S) \to ϕK^+ K^-, ωπ+π−ωπ^+ π^-, K∗0K−π+K^{\ast 0} K^- π^+, K∗0K2∗0K^{\ast0} K_2^{\ast 0} and Υ(2S)→ϕK+K−Υ(2S) \to ϕK^+ K^-, K∗0K−π+K^{\ast 0} K^- π^+ decay modes. Branching fractions are determined for all the processes, while 90% confidence level upper limits are established on the branching fractions for the modes with a statistical significance less than 3σ3σ. The ratios of the branching fractions of Υ(2S)Υ(2S) and Υ(1S)Υ(1S) decays into the same final state are used to test a perturbative QCD prediction for OZI suppressed bottomonium decays.

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