Measurements of the Υ(10860)Υ(10860) and Υ(11020)Υ(11020) resonances via σ(e+e−→Υ(nS)π+π−)σ(e^+e^-\rightarrowΥ(n{\rm S})π^+π^-)

preprint2016arXivOpen access
Belle CollaborationD. SantelK. KinoshitaP. ChangA. AbdesselamI. AdachiH. AiharaS. Al SaidK. ArinsteinD. M. AsnerT. AushevR. AyadA. M. BakichV. BansalB. BhuyanA. BobrovA. BondarG. BonviciniM. BračkoT. E. BrowderD. ČervenkovV. ChekelianB. G. CheonK. ChilikinK. ChoV. ChobanovaS. -K. ChoiY. ChoiD. CinabroJ. DalsenoM. DanilovJ. DingfelderZ. DoležalZ. DrásalA. DrutskoyS. EidelmanH. FarhatJ. E. FastT. FerberV. GaurN. GabyshevA. GarmashD. GetzkowR. GillardY. M. GohJ. HabaT. HaraK. HayasakaH. HayashiiX. H. HeW. -S. HouH. J. HyunT. IijimaK. InamiA. IshikawaR. ItohY. IwasakiI. JaegleD. JoffeT. JuliusK. H. KangE. KatoT. KawasakiC. KieslingD. Y. KimH. J. KimJ. B. KimJ. H. KimM. J. KimS. H. KimY. J. KimB. R. KoP. KodyšS. KorparP. KrižanP. KrokovnyA. KuzminJ. S. LangeI. S. LeeY. LiL. Li GioiJ. LibbyD. LiventsevP. LukinD. MatvienkoK. MiyabayashiH. MiyataR. MizukG. B. MohantyA. MollT. MoriR. MussaE. NakanoM. NakaoT. NanutZ. NatkaniecN. K. NisarS. NishidaS. OgawaS. OkunoS. L. OlsenC. OswaldP. PakhlovG. PakhlovaC. W. ParkH. ParkT. K. PedlarM. PetričL. E. PiilonenE. RibežlM. RitterA. RostomyanS. RyuY. SakaiS. SandilyaL. SanteljT. SanukiV. SavinovO. SchneiderG. SchnellC. SchwandaA. J. SchwartzK. SenyoM. E. SeviorV. ShebalinT. -A. ShibataJ. -G. ShiuB. ShwartzA. SibidanovF. SimonY. -S. SohnE. SolovievaM. StaričM. StederU. TamponiG. TatishviliY. TeramotoK. TrabelsiM. UchidaT. UglovY. UnnoS. UnoC. Van HulseP. VanhoeferG. VarnerA. VinokurovaM. N. WagnerP. WangX. L. WangM. WatanabeY. WatanabeE. WonJ. YamaokaY. -P. YangS. YashchenkoY. YookY. YusaZ. P. ZhangV. ZhilichV. ZhulanovA. Zupanc

Abstract

We report new measurements of the total cross sections for e+e−→Υ(nS)π+π−e^+e^-\to Υ(n{\rm S})π^+π^- (nn = 1, 2, 3) and e+e−→bbˉe^+e^-\to b\bar b from a high-luminosity fine scan of the region s=10.63\sqrt{s} = 10.63-11.0511.05 GeV with the Belle detector. We observe that the Υ(nS)π+π−Υ(n{\rm S})π^+π^- spectra have little or no non-resonant component and extract from them the masses and widths of Υ(10860)Υ(10860) and Υ(11020)Υ(11020) and their relative phase. We find M10860=(10891.1±3.2−1.7+0.6)M_{10860}=(10891.1\pm3.2^{+0.6}_{-1.7}) MeV/c2c^2 and Γ10860=(53.7−5.6+7.1 −5.4+1.3)Γ_{10860}=(53.7^{+7.1}_{-5.6}\,^{+1.3}_{-5.4}) MeV and report first measurements M11020=(10987.5−2.5+6.4 −2.1+9.0)M_{11020}=(10987.5^{+6.4}_{-2.5}\,^{+9.0}_{-2.1}) MeV/c2c^2, Γ11020=(61−19+9 −20+2)Γ_{11020}=(61^{+9}_{-19}\,^{+2}_{-20}) MeV, and ϕ11020−ϕ10860=(−1.0±0.4 −0.1+1.4)ϕ_{\rm 11020}-ϕ_{\rm 10860} = (-1.0\pm0.4\,^{+1.4}_{-0.1}) rad.

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