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ΛcΛ+ν\Lambda_c \to \Lambda \ell^+ \nu_\ell form factors and decay rates from lattice QCD with physical quark masses

Abstract

The first lattice QCD calculation of the form factors governing ΛcΛ+ν\Lambda_c \to \Lambda \ell^+ \nu_\ell decays is reported. The calculation was performed with two different lattice spacings and includes one ensemble with a pion mass of 139(2) MeV. The resulting predictions for the ΛcΛe+νe\Lambda_c \to \Lambda e^+ \nu_e and ΛcΛμ+νμ\Lambda_c \to \Lambda \mu^+ \nu_\mu decay rates divided by Vcs2|V_{cs}|^2 are 0.2007(71)(74)ps10.2007(71)(74)\:{\rm ps}^{-1} and 0.1945(69)(72)ps10.1945(69)(72)\:{\rm ps}^{-1}, respectively, where the two uncertainties are statistical and systematic. Taking the Cabibbo-Kobayashi-Maskawa matrix element Vcs|V_{cs}| from a global fit and the Λc\Lambda_c lifetime from experiments, this translates to branching fractions of B(ΛcΛe+νe)=0.0380(19)LQCD(11)τΛc\mathcal{B}(\Lambda_c\to\Lambda e^+\nu_e)=0.0380(19)_{\rm LQCD\:\:}(11)_{\tau_{\Lambda_c}} and B(ΛcΛμ+νμ)=0.0369(19)LQCD(11)τΛc\mathcal{B}(\Lambda_c\to\Lambda \mu^+\nu_\mu)=0.0369(19)_{\rm LQCD\:\:}(11)_{\tau_{\Lambda_c}}. These results are consistent with, and two times more precise than, the measurements performed recently by the BESIII Collaboration. Using instead the measured branching fractions together with the lattice calculation to determine the CKM matrix element gives Vcs=0.949(24)LQCD(14)τΛc(49)B|V_{cs}|= 0.949(24)_{\rm LQCD\:\:}(14)_{\tau_{\Lambda_c}}(49)_{\mathcal{B}}.Comment: 6 pages, 3 figures, form factor parameters included as ancillary file

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