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The heavy $Z^\\prime$ boson associated with spontaneously breaking $U(1)_X$ at the TeV scale mediates the $b\\to s\\ell\\ell$ anomalies via $\\mathcal{O}^\\mu_9 \\sim\\frac{1}{\\Lambda^2}(\\bar{s}\\gamma_\\rho P_L b)(\\bar{\\mu} \\gamma^\\rho \\mu)$. 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The heavy $Z^\\prime$ boson associated with spontaneously breaking $U(1)_X$ at the TeV scale mediates the $b\\to s\\ell\\ell$ anomalies via $\\mathcal{O}^\\mu_9 \\sim\\frac{1}{\\Lambda^2}(\\bar{s}\\gamma_\\rho P_L b)(\\bar{\\mu} \\gamma^\\rho \\mu)$. 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