By analyzing 482 pb of collision data collected at the center-of-mass energy GeV with the BESIII detector, we measure the %absolute branching fractions for the semi-leptonic decays $D_{s}^{+}\to \phi e^{+}\nu_{e}\phi \mu^{+}\nu_{\mu}\eta \mu^{+}\nu_{\mu}\eta’\mu^{+}\nu_{\mu}{\mathcal B}(D_{s}^{+}\to\phi e^{+}\nu_{e})=(2.26\pm0.45\pm0.09){\mathcal B}(D_{s}^{+}\to\phi \mu^{+}\nu_{\mu})=(1.94\pm0.53\pm0.09){\mathcal B}(D_{s}^{+}\to\eta \mu^{+}\nu_{\mu})=(2.42\pm0.46\pm0.11){\mathcal B}(D_{s}^{+}\to\eta’\mu^{+} \nu_{\mu}) = (1.06\pm0.54\pm0.07)$%, where the first and second uncertainties are statistical and systematic, respectively. The branching fractions for the three semi-muonic decays $D_s^+\to\phi \mu^+\nu_\mu, \eta \mu^+\nu_\mu\eta’ \mu^+\nu_\mu$ are determined for the first time and that of is consistent with the world average value within uncertainties.

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