Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model
We calculate the masses of χc(2P) and χb(3P) states with threshold corrections in a coupled-channel model. Here, the meson quarkonium core is augmented by higher Fock components due to pair-creation effects. According to our results, we interpret the resonances characterized by very small threshold...
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doaj-a19d0c5b466f4e6eb95a28017b8c3bd52020-11-24T23:46:29ZengElsevierPhysics Letters B0370-26932019-02-01789550555Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel modelJ. Ferretti0E. Santopinto1CAS Key Laboratory of Theoretical Physics, Institute of Theoretical Physics, Chinese Academy of Sciences, Beijing 100190, China; Center for Theoretical Physics, Sloane Physics Laboratory, Yale University, New Haven, CT 06520-8120, USAINFN, Sezione di Genova, Via Dodecaneso 33, 16146 Genova, Italy; Corresponding author.We calculate the masses of χc(2P) and χb(3P) states with threshold corrections in a coupled-channel model. Here, the meson quarkonium core is augmented by higher Fock components due to pair-creation effects. According to our results, we interpret the resonances characterized by very small threshold corrections, like χb(3P)'s, as almost pure quarkonia, and those states characterized by non-negligible threshold corrections, like the X(3872), as quarkonium cores plus meson–meson components. We also study the J/ψρ and J/ψω hidden-flavor strong decays of the X(3872). The decays are calculated as the dissociation of one of these components (D0D¯0⁎) into a cc¯ state (J/ψ) plus a light meson (ρ or ω) in a potential model. In particular, our result for the ratio between the X(3872)→J/ψω and J/ψρ widths (0.6) is compatible with the present experimental data (0.8±0.3) within the experimental error. Keywords: X(3872), χc(2P), χb(3P), Heavy quarkonium spectroscopy, Hidden-flavor strong decayshttp://www.sciencedirect.com/science/article/pii/S0370269318309870 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
J. Ferretti E. Santopinto |
spellingShingle |
J. Ferretti E. Santopinto Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model Physics Letters B |
author_facet |
J. Ferretti E. Santopinto |
author_sort |
J. Ferretti |
title |
Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model |
title_short |
Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model |
title_full |
Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model |
title_fullStr |
Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model |
title_full_unstemmed |
Threshold corrections of χc(2P) and χb(3P) states and J/ψρ and J/ψω transitions of the X(3872) in a coupled-channel model |
title_sort |
threshold corrections of χc(2p) and χb(3p) states and j/ψρ and j/ψω transitions of the x(3872) in a coupled-channel model |
publisher |
Elsevier |
series |
Physics Letters B |
issn |
0370-2693 |
publishDate |
2019-02-01 |
description |
We calculate the masses of χc(2P) and χb(3P) states with threshold corrections in a coupled-channel model. Here, the meson quarkonium core is augmented by higher Fock components due to pair-creation effects. According to our results, we interpret the resonances characterized by very small threshold corrections, like χb(3P)'s, as almost pure quarkonia, and those states characterized by non-negligible threshold corrections, like the X(3872), as quarkonium cores plus meson–meson components. We also study the J/ψρ and J/ψω hidden-flavor strong decays of the X(3872). The decays are calculated as the dissociation of one of these components (D0D¯0⁎) into a cc¯ state (J/ψ) plus a light meson (ρ or ω) in a potential model. In particular, our result for the ratio between the X(3872)→J/ψω and J/ψρ widths (0.6) is compatible with the present experimental data (0.8±0.3) within the experimental error. Keywords: X(3872), χc(2P), χb(3P), Heavy quarkonium spectroscopy, Hidden-flavor strong decays |
url |
http://www.sciencedirect.com/science/article/pii/S0370269318309870 |
work_keys_str_mv |
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