Abstract

The shape of the Bs0Dsμ+νμB_s^0\rightarrow D_s^{*-}\mu^+\nu_{\mu} differential decay rate is obtained as a function of the hadron recoil using proton-proton collision data at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 1.7 fb1^{-1} collected by the LHCb detector. The Bs0Dsμ+νμB_s^0\rightarrow D_s^{*-}\mu^+\nu_{\mu} decay is reconstructed through the decays DsDsγD_s^{*-}\rightarrow D_s^{-}\gamma and DsKK+πD_s^{-}\rightarrow K^-K^+\pi^-. The differential decay rate is fitted with the Caprini-Lellouch-Neubert (CLN) and Boyd-Grinstein-Lebed (BGL) parametrisations of the form factors, and the relevant quantities for both are extracted

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