Identification of Y(4008), Y(4140), Y(4260), and Y(4360) as Tetraquark States
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Abstract
Within the framework of a color flux-tube model with a four-body confinement potential, the tetraquark states cqcq (q=u or d) with IJPC=01– are systematically investigated. The numerical results indicate that states Y(4008), Y(4140), Y(4260), and Y(4360) can be uniformly described as tetraquark states cqcq with n2S+1LJ of 11P1, 15P1, 25P1 and 15F1, respectively, in the color flux-tube model. They are compact three-dimensional spatial configurations similar to a rugby ball, higher orbital angular momentum L, more prolate. The four-body confinement interaction based on a color flux-tube picture should be responsible for the formation of those compact tetraquark states.
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ZHOU Ping, DENG Cheng-Rong, PING Jia-Lun. Identification of Y(4008), Y(4140), Y(4260), and Y(4360) as Tetraquark States[J]. Chin. Phys. Lett., 2015, 32(10): 101201. DOI: 10.1088/0256-307X/32/10/101201
ZHOU Ping, DENG Cheng-Rong, PING Jia-Lun. Identification of Y(4008), Y(4140), Y(4260), and Y(4360) as Tetraquark States[J]. Chin. Phys. Lett., 2015, 32(10): 101201. DOI: 10.1088/0256-307X/32/10/101201
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ZHOU Ping, DENG Cheng-Rong, PING Jia-Lun. Identification of Y(4008), Y(4140), Y(4260), and Y(4360) as Tetraquark States[J]. Chin. Phys. Lett., 2015, 32(10): 101201. DOI: 10.1088/0256-307X/32/10/101201
ZHOU Ping, DENG Cheng-Rong, PING Jia-Lun. Identification of Y(4008), Y(4140), Y(4260), and Y(4360) as Tetraquark States[J]. Chin. Phys. Lett., 2015, 32(10): 101201. DOI: 10.1088/0256-307X/32/10/101201
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