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    Behaviors of imitated agents in an evolutionary minority game on NW small world networks

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    AbstractIn this paper, we study the behaviors of imitated agents who compete for a limited resource through Evolutionary Minority Game. The agents are mapped into vertices on small world networks proposed by Newman and Watts [1] (NW small world networks). The numerical results show that the probability distribution P (p) is different for different prize-to-fine ratio R, and has a phasic evolution. The performance of the system with NW small world networks is better than that of the system with WS small world networks [2]

    Y(4626) as a molecular state from interaction Dsβˆ—DΛ‰s1(2536)βˆ’DsDΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536)-{D}_s\bar{D}_{s1}(2536)

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    Recently, a new structure Y(4626)Y(4626) was reported by the Belle Colloboration in the process e+eβˆ’β†’Ds+Ds1(2536)βˆ’e^+e^-\to D_s^+D_{s1}(2536)^-. In this work, we propose an assignment of the Y(4626)Y(4626) as a Dsβˆ—DΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536) molecular state, which decays into the Ds+Ds1(2536)βˆ’D_s^+D_{s1}(2536)^- channel through a coupling between Dsβˆ—DΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536) and DsDΛ‰s1(2536){D}_s\bar{D}_{s1}(2536) channels. With the help of the heavy quark symmetry, the potential of the interaction Dsβˆ—DΛ‰s1(2536)βˆ’DsDΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536)-{D}_s\bar{D}_{s1}(2536) is constructed within the one-boson-exchange model, and inserted into the quasipotential Bethe-Salpeter equation. The pole of obtained scattering amplitude is searched for in the complex plane, which corresponds to a molecular state from the interaction Dsβˆ—DΛ‰s1(2536)βˆ’DsDΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536)-{D}_s\bar{D}_{s1}(2536). The results suggest that a pole is produced near the Dsβˆ—DΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536) threshold, which exhibits as a peak in the invariant mass spectrum of the DsDΛ‰s1(2536){D}_s\bar{D}_{s1}(2536) channel at about 4626 MeV. It obviously favors the Y(4265)Y(4265) as a Dsβˆ—DΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536) molecular state. In the same model, other molecular states from the interaction Dsβˆ—DΛ‰s1(2536)βˆ’DsDΛ‰s1(2536){D}^*_s\bar{D}_{s1}(2536)-{D}_s\bar{D}_{s1}(2536) are also predicted, which can be checked in future experiments.Comment: 7 pages, 2 figure
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