Measurement of e+e−→π+π−ψ(2S)e^+e^- \to π^+π^-ψ(2S) via Initial State Radiation at Belle

preprint2016arXivOpen access
X. L. WangC. Z. YuanC. P. ShenP. WangA. AbdesselamI. AdachiH. AiharaS. Al SaidK. ArinsteinD. M. AsnerR. AyadA. M. BakichV. BansalB. BhuyanA. BobrovG. BonviciniM. BračkoT. E. BrowderD. ČervenkovP. ChangV. ChekelianA. ChenB. G. CheonK. ChilikinR. ChistovK. ChoV. ChobanovaS. -K. ChoiY. ChoiD. CinabroJ. DalsenoM. DanilovZ. DoležalZ. DrásalA. DrutskoyK. DuttaS. EidelmanH. FarhatJ. E. FastT. FerberV. GaurA. GarmashD. GetzkowR. GillardY. M. GohJ. HabaK. HayasakaH. HayashiiX. H. HeW. -S. HouT. IijimaK. InamiA. IshikawaR. ItohY. IwasakiD. JoffeT. JuliusK. H. KangE. KatoT. KawasakiC. KieslingD. Y. KimH. J. KimJ. B. KimJ. H. KimM. J. KimS. H. KimY. J. KimK. KinoshitaB. R. KoP. KodyšS. KorparP. KrokovnyA. KuzminY. -J. KwonJ. S. LangeI. S. LeeP. LewisY. LiL. Li GioiJ. LibbyD. LiventsevP. LukinD. MatvienkoK. MiyabayashiH. MiyataR. MizukA. MollT. MoriR. MussaE. NakanoM. NakaoT. NanutZ. NatkaniecN. K. NisarS. NishidaS. OgawaS. OkunoS. L. OlsenP. PakhlovG. PakhlovaC. W. ParkH. ParkT. K. PedlarR. PestotnikM. PetričL. E. PiilonenE. RibežlM. RitterA. RostomyanS. RyuY. SakaiS. SandilyaL. SanteljT. SanukiV. SavinovO. SchneiderG. SchnellC. SchwandaD. SemmlerK. SenyoV. ShebalinT. -A. ShibataJ. -G. ShiuA. SibidanovF. SimonY. -S. SohnA. SokolovE. SolovievaM. StaričM. StederT. SumiyoshiU. TamponiK. TanidaG. TatishviliY. TeramotoK. TrabelsiM. UchidaT. UglovY. UnnoS. UnoY. UsovC. Van HulseP. VanhoeferG. VarnerA. VinokurovaM. N. WagnerY. WatanabeE. WonS. YashchenkoY. YusaZ. P. ZhangV. ZhilichA. Zupanc

Abstract

We report measurement of the cross section of e+e−→π+π−ψ(2S)e^+e^-\to π^+π^-ψ(2S) between 4.0 and 5.5GeV5.5 {\rm GeV}, based on an analysis of initial state radiation events in a 980fb−1980 \rm fb^{-1} data sample recorded with the Belle detector. The properties of the Y(4360)Y(4360) and Y(4660)Y(4660) states are determined. Fitting the mass spectrum of π+π−ψ(2S)π^+π^-ψ(2S) with two coherent Breit-Wigner functions, we find two solutions with identical mass and width but different couplings to electron-positron pairs: MY(4360)=(4347±6±3)MeV/c2M_{Y(4360)} = (4347\pm 6\pm 3) {\rm MeV}/c^2, ΓY(4360)=(103±9±5)MeVΓ_{Y(4360)} = (103\pm 9\pm 5) {\rm MeV}, MY(4660)=(4652±10±8)MeV/c2M_{Y(4660)} = (4652\pm10\pm 8) {\rm MeV}/c^2, ΓY(4660)=(68±11±1)MeVΓ_{Y(4660)} = (68\pm 11\pm 1) \rm MeV; and B[Y(4360)→π+π−ψ(2S)]⋅ΓY(4360)e+e−=(10.9±0.6±0.7)eV{\cal{B}}[Y(4360)\to π^+π^-ψ(2S)]\cdot Γ_{Y(4360)}^{e^+e^-} = (10.9\pm 0.6\pm 0.7) \rm eV and B[Y(4660)→π+π−ψ(2S)]⋅ΓY(4660)e+e−=(8.1±1.1±0.5)eV{\cal{B}}[Y(4660)\to π^+π^-ψ(2S)]\cdot Γ_{Y(4660)}^{e^+e^-} = (8.1\pm 1.1\pm 0.5) \rm eV for one solution; or B[Y(4360)→π+π−ψ(2S)]⋅ΓY(4360)e+e−=(9.2±0.6±0.6)eV{\cal{B}}[Y(4360)\to π^+π^-ψ(2S)]\cdot Γ_{Y(4360)}^{e^+e^-} = (9.2\pm 0.6\pm 0.6) \rm eV and B[Y(4660)→π+π−ψ(2S)]⋅ΓY(4660)e+e−=(2.0±0.3±0.2)eV{\cal{B}}[Y(4660)\to π^+π^-ψ(2S)]\cdot Γ_{Y(4660)}^{e^+e^-} = (2.0\pm 0.3\pm 0.2) \rm eV for the other. Here, the first errors are statistical and the second systematic. Evidence for a charged charmoniumlike structure at 4.05GeV/c24.05 {\rm GeV}/c^2 is observed in the π±ψ(2S)π^{\pm}ψ(2S) intermediate state in the Y(4360)Y(4360) decays.

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