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    Search for C=+C=+ charmonium and bottomonium states in e+eβˆ’β†’Ξ³+Xe^+e^-\to \gamma+ X at B factories

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    We study the production of C=+C=+ charmonium states XX in e+eβˆ’β†’Ξ³+Xe^+e^-\to \gamma + X at B factories with X=Ξ·c(nS)X=\eta_c(nS) (n=1,2,3), Ο‡cJ(mP)\chi_{cJ}(mP) (m=1,2), and 1D2(1D)^1D_2(1D). In the S and P wave case, contributions of tree-QED with one-loop QCD corrections are calculated within the framework of nonrelativistic QCD(NRQCD) and in the D-wave case only the tree-QED contribution are considered. We find that in most cases the QCD corrections are negative and moderate, in contrast to the case of double charmonium production e+eβˆ’β†’J/ψ+Xe^+e^-\to J/\psi + X, where QCD corrections are positive and large in most cases. We also find that the production cross sections of some of these states in e+eβˆ’β†’Ξ³+Xe^+e^-\to \gamma + X are larger than that in e+eβˆ’β†’J/ψ+Xe^+e^-\to J/\psi + X by an order of magnitude even after the negative QCD corrections are included. So we argue that search for the X(3872), X(3940), Y(3940), and X(4160) in e+eβˆ’β†’Ξ³+Xe^+e^-\to \gamma + X at B factories may be helpful to clarify the nature of these states. For completeness, the production of bottomonium states in e+eβˆ’e^+e^- annihilation is also discussed.Comment: 13pages, 4 figure
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