In this work, we investigate the semi-leptonic weak decays of spin-1/2 doubly-heavy baryons $\Xi_{QQ^{\prime}}$ into spin-3/2 singly-heavy baryons $\Sigma_{Q^{\prime}}^*$ within light-cone sum rules. Using the parallel components of the light-cone distribution amplitudes of $\Sigma_{Q^{\prime}}^*$, the transition form factors for these decays are calculated both analytically and numerically. The numerical results for these semi-leptonic weak decays widths and branching ratios are also predicted, which are compared with the same predictions by other theoretical approaches in the literatures. These phenomenology predictions can be tested by the experiments in the future.Comment: 19 pages, 2 figures, 4 table
The transition magnetic dipole and electric quadrupole moments of the radiative decays of the sextet...
Very recently, the LHCb collaboration has observed in the final state $$\Lambda _c^+ K^-\pi ^+\pi ^+...
AbstractIn this article, we calculate the B→a1(1260) form-factors V1(q2), V2(q2), V3(q2) and A(q2) w...
© 2021 Published by the American Physical SocietyForm factors of the weak transitions are calculated...
In this work, we analyze the semileptonic decay processes of $\Lambda_b \to \Lambda_c$ in the light-...
In the framework of a non-relativistic quark model, the mass spectra of the ground and excited state...
We analyze weak decays of triply heavy baryon $\Omega_{ccc}^{++}$ and calculate the form factors for...
The semileptonic decays of heavy spin-1/2, Xi(b(c)) and Xi(b(c))' baryons to the light spin-1/2, Xi ...
In this work, we calculate the transition form factors of $\Lambda_b$ decaying into $\Lambda_c$ with...
Abstract As a continuation of our previous work, we investigate the weak decays of doubly heavy bary...
Abstract Very recently, the LHCb collaboration has observed in the final state $$\Lambda _c^+ K^-\pi...
Without contamination from the final state interactions, the calculation of the branching ratios of ...
We revisit the calculation of the strong couplings D∗Dπ and B∗Bπ from the QCD light-cone sum rules u...
The semileptonic decays of heavy spin-1/2, Ξ b(c) and Ξ′ b(c) baryons to the light spin-1/2, Ξ an...
We review recent developments in QCD sum rule applications to semileptonic B->pi and D->pi transitio...
The transition magnetic dipole and electric quadrupole moments of the radiative decays of the sextet...
Very recently, the LHCb collaboration has observed in the final state $$\Lambda _c^+ K^-\pi ^+\pi ^+...
AbstractIn this article, we calculate the B→a1(1260) form-factors V1(q2), V2(q2), V3(q2) and A(q2) w...
© 2021 Published by the American Physical SocietyForm factors of the weak transitions are calculated...
In this work, we analyze the semileptonic decay processes of $\Lambda_b \to \Lambda_c$ in the light-...
In the framework of a non-relativistic quark model, the mass spectra of the ground and excited state...
We analyze weak decays of triply heavy baryon $\Omega_{ccc}^{++}$ and calculate the form factors for...
The semileptonic decays of heavy spin-1/2, Xi(b(c)) and Xi(b(c))' baryons to the light spin-1/2, Xi ...
In this work, we calculate the transition form factors of $\Lambda_b$ decaying into $\Lambda_c$ with...
Abstract As a continuation of our previous work, we investigate the weak decays of doubly heavy bary...
Abstract Very recently, the LHCb collaboration has observed in the final state $$\Lambda _c^+ K^-\pi...
Without contamination from the final state interactions, the calculation of the branching ratios of ...
We revisit the calculation of the strong couplings D∗Dπ and B∗Bπ from the QCD light-cone sum rules u...
The semileptonic decays of heavy spin-1/2, Ξ b(c) and Ξ′ b(c) baryons to the light spin-1/2, Ξ an...
We review recent developments in QCD sum rule applications to semileptonic B->pi and D->pi transitio...
The transition magnetic dipole and electric quadrupole moments of the radiative decays of the sextet...
Very recently, the LHCb collaboration has observed in the final state $$\Lambda _c^+ K^-\pi ^+\pi ^+...
AbstractIn this article, we calculate the B→a1(1260) form-factors V1(q2), V2(q2), V3(q2) and A(q2) w...