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Quark-antiquark states and their radiative transitions in terms of the spectral integral equation: Charmonia

Journal Article · · Physics of Atomic Nuclei
; ; ; ;  [1]
  1. Russian Academy of Sciences, Petersburg Nuclear Physics Institute (Russian Federation)
Earlier by the authors (Yad. Fiz. 70, 68 (2007)), the bb states were treated in the framework of the spectral integral equation, together with simultaneous calculations of radiative decays of the considered bottomonia. In the present paper, such a study is carried out for the charmonium (c c-bar) states. We reconstruct the interaction in the c-c sector on the basis of the data for the charmonium levels with J{sub PC} = 0{sup -+}, 1{sup --}, 0{sup ++}, 1{sup ++}, 2{sup ++}, 1{sup +-} and radiative transitions {psi}(2S) {sup {yields}} {gamma}{chi}{sub c0}(1P), {gamma}{chi}{sub c1}(1P), {gamma}{chi}{sub c2}(1P), {gamma}{chi}{sub c}(1S) and {chi}{sub c0}(1P), {chi}{sub c1}(1P), {chi}{sub c2}(1P) {sup {yields}} {gamma}J/{psi}. The c-c levels and their wave functions are calculated for the radial excitations with n {<=} 6. Also, we determine the c-c component of the photon wave function using the e{sup +}e{sup -}-annihilation data: e{sup +}e{sup -} {sup {yields}} J/{psi}(3097), {psi}(3686), {psi}(3770), {psi}(4040), {psi}(4160), {psi}(4415) and perform the calculations of the partial widths of the two-photon decays for the n = 1 states {eta}{sub c0}(1S), {chi}{sub c0}(1P), {chi}{sub c2}(1P) {sup {yields}} {gamma}{gamma} and n = 2 states {eta}{sub c0}(2S) {sup {yields}} {gamma}{gamma}, {chi}{sub c0}(2P) {sup {yields}} {gamma}{gamma}. We discuss the status of the recently observed c-c states X(3872) and Y(3941): according to our results, the X(3872) can be either {chi}{sub c1}(2P) or {eta}{sub c2}(1D), while Y(3941) is {chi}{sub c2}(2P)
OSTI ID:
21075933
Journal Information:
Physics of Atomic Nuclei, Journal Name: Physics of Atomic Nuclei Journal Issue: 2 Vol. 70; ISSN 1063-7788; ISSN PANUEO
Country of Publication:
United States
Language:
English

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