The radiative corrections to the pure leptonic decay $D_s{\longrightarrow} {\ell}{{\nu}}_{\ell}$ up-to one-loop order is presented. We find the virtual photon loop corrections to $D_s{\longrightarrow} {\tau}{{\nu}}_{\tau}$ is negative and the corresponding branching ratio is larger than $3.51\times 10^{-3}$. Considering the possible experimental resolutions, our prediction of the radiative decay $D_s{\longrightarrow} {\tau}{{\nu}}_{\tau}\gamma$ is not so large as others, and the best channel to determine the $V_{cs}$ or $f_{D_s}$ is $D_s{\longrightarrow} {\mu}{{\nu}}_{\mu}{\gamma}$
The decay width of b to c,c,c,l,nu has been computed as an expansion in limit (1- 3*(m_c/m_b)) << 1 ...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
We report on recent work to determine the CKM matrix element |V_{us}| using strange hadronic \tau de...
Monolayer transition metal dichalcogenides (TMDCs) are direct gap semiconductors with a unique poten...
AbstractIn this Letter, we investigate the radiative leptonic decays D−(s)→γℓν̄ (ℓ=e,μ) at tree leve...
We point out that R ≡ Br(b→dγ)/Br(b →sγ) is a sensitive probe of possible violation of CKM unitarity...
We present the differential rates and branching ratios of the radiative decays τ → l ν ¯ ν γ $$ \tau...
Light emission in two-dimensional (2D) transition metal dichalcogenides (TMDs) changes significantly...
We derive structure functions for the quasielastic production of octet baryons in neutrino and antin...
AbstractThe light cone QCD sum rules method is used to calculate the transition form factor for the ...
The first order QED corrections to the polarized muon decay spectrum are considered. The exact depen...
Taking account of possible CP violation, we discuss about the constraints on the lepton mixing angle...
In this work, we make a systematical study on the four-body $B_{(s)} \to (\pi\pi)(\pi\pi)$ decays in...
Time-reversal symmetry suppresses electron backscattering in a quantum-spin-Hall edge, yielding quan...
We study a leptogenesis scenario in which the heavy Majorana neutrinos are produced non-thermally ...
The decay width of b to c,c,c,l,nu has been computed as an expansion in limit (1- 3*(m_c/m_b)) << 1 ...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
We report on recent work to determine the CKM matrix element |V_{us}| using strange hadronic \tau de...
Monolayer transition metal dichalcogenides (TMDCs) are direct gap semiconductors with a unique poten...
AbstractIn this Letter, we investigate the radiative leptonic decays D−(s)→γℓν̄ (ℓ=e,μ) at tree leve...
We point out that R ≡ Br(b→dγ)/Br(b →sγ) is a sensitive probe of possible violation of CKM unitarity...
We present the differential rates and branching ratios of the radiative decays τ → l ν ¯ ν γ $$ \tau...
Light emission in two-dimensional (2D) transition metal dichalcogenides (TMDs) changes significantly...
We derive structure functions for the quasielastic production of octet baryons in neutrino and antin...
AbstractThe light cone QCD sum rules method is used to calculate the transition form factor for the ...
The first order QED corrections to the polarized muon decay spectrum are considered. The exact depen...
Taking account of possible CP violation, we discuss about the constraints on the lepton mixing angle...
In this work, we make a systematical study on the four-body $B_{(s)} \to (\pi\pi)(\pi\pi)$ decays in...
Time-reversal symmetry suppresses electron backscattering in a quantum-spin-Hall edge, yielding quan...
We study a leptogenesis scenario in which the heavy Majorana neutrinos are produced non-thermally ...
The decay width of b to c,c,c,l,nu has been computed as an expansion in limit (1- 3*(m_c/m_b)) << 1 ...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
We report on recent work to determine the CKM matrix element |V_{us}| using strange hadronic \tau de...