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Can X(3872) be a J^P=2^-Tetraquark State?

Can X(3872) be a J^P=2^-Tetraquark State?
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摘要 In this article,we test the nature of X(3872),which is assumed to be a P-wave [cq]-scalar-diquark [cq]axial-vector-antidiquark tetraquark state with JP= 2-.The interpolating current representing the JP= 2-state is proposed.Technically,contributions of the operators up to dimension six are included in the operator product expansion.The mass obtained for such state is m2-=(4.38 ± 0.15) GeV.We conclude that it is impossible to describe the X(3872) structure as J P = 2-tetraquark state. In this article, we test the nature of X(3872), which is assumed to be a P-wave [cq]-scalar-diquark [cq]- axial-vector-antidiquark tetraquark state with JP = 2^-. The interpolating current representing the JP = 2^- state is proposed. Technically, contributions of the operators up to dimension six are included in the operator product expansion. The mass obtained for such state is m2- = (4.38±0.15) GeV. We conclude that it is impossible to describe the X(3872) structure as JV = 2^- tetraauark state.
机构地区 Department of Physics
出处 《Communications in Theoretical Physics》 SCIE CAS CSCD 2012年第6期1033-1036,共4页 理论物理通讯(英文版)
基金 Supported by the National Natural Science Foundation of China under Grant Nos. 10975184,11047117,11105222,and 11105223
关键词 双夸克 运营商 轴矢量 k状态 插值 伏特 电子 构作 X(3872), exotic-charmonium states, QCD rules
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