001     902840
005     20230217124239.0
024 7 _ |a 10.1103/PhysRevD.104.094006
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024 7 _ |a 1089-4918
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024 7 _ |a 1538-4500
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024 7 _ |a 1550-2368
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024 7 _ |a 1550-7998
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037 _ _ |a FZJ-2021-04597
082 _ _ |a 530
100 1 _ |a Anwar, Muhammad Naeem
|0 P:(DE-Juel1)176611
|b 0
|e Corresponding author
245 _ _ |a Heavy quark spin partners of the Y ( 4260 ) in coupled-channel formalism
260 _ _ |a Melville, NY
|c 2021
|b Inst.
264 _ 1 |3 online
|2 Crossref
|b American Physical Society (APS)
|c 2021-11-05
264 _ 1 |3 print
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|b American Physical Society (APS)
|c 2021-11-01
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520 _ _ |a The charmoniumlike state Y(4260) is described as predominantly a D1¯D molecule in a coupled-channel quark model [Phys. Rev. D 96, 114022 (2017)]. The heavy quark spin symmetry (HQSS) thus implies the possible emergence of its heavy quark spin partners with molecular configurations as D1¯D∗ and D∗2¯D∗ below these charmed mesons’ thresholds. We analyze the probabilities of various intermediate charmed meson loops for JPC=1−− exotic state Y(4360) and find that the channel D1¯D∗ couples more strongly around its mass regime, and the coupling behavior remains the same even if the mass of Y(4360) is pushed closer to D1¯D∗ threshold. This enlightens that the most favorable molecular scenario for the Y(4360) could be D1¯D∗, and hence it can be interpreted as HQSS partner of the Y(4260). We also find the strong coupling behavior of D∗2¯D∗ channel with the ψ(4415), which makes it a good candidate for a dominant D∗2¯D∗ molecule. We discuss the important decay patterns of these resonances to disentangle their long- and short-distance structures.
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773 _ _ |a 10.1103/PhysRevD.104.094006
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856 4 _ |u https://juser.fz-juelich.de/record/902840/files/PhysRevD.104.094006.pdf
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