Calculation of 1/m^{2}_{b} corrections to <Λ_{b}(v,s)|\bar{b}γ^λγ_{5}b|Λ_{b}(v,s)> for polarized Λ_{b} in the Bethe-Salpeter equation approach
arXiv:1305.1078 · doi:10.1103/PhysRevD.87.076013
Abstract
The heavy baryon Λ_{Q} (Q=b or c) can be regarded as composed of a heavy quark and a scalar light diquark which has good spin and isospin quantum numbers. In this picture we establish the Bethe-Salpeter (BS) equation for Λ_{Q} to second order in the 1/m_{Q} expansion. With the kernel containing both the scalar confinement and the one-gluon-exchange terms we solve the BS equation numerically. The value of the spin-dependant form factor for the matrix element <Λ_{b}{(v,s)}|\bar{b}γ^λγ_{5}b|Λ_{b}(v,s)>, ε_{b}, which is non-zero at order 1/m^{2}_{b}, is obtained numerically from our model.
References in corpus (4)
- Moments of semileptonic B decay distributions in the 1/m_b expansion
- On the photon energy moments and their `bias' corrections in B -> X_s+γ
- Perturbative corrections to the semileptonic b-decay moments: E^\ell_{cut} dependence and running-α_s effects in the OPE approach
- The Average Kinetic Energy of the Heavy Quark in in the Bethe-Salpeter Equation Approach
Cited by in corpus (9)
- The mass spectra and wave functions for the doubly heavy baryons with heavy diquark core
- Possible open-charmed pentaquark molecule --- the bound state --- in the Bethe-Salpeter formalism
- Electromagnetic form factors of in the Bethe-Salpeter equation approach
- FCNC transitions of to neutron in Bethe-Salpeter equation approach
- Rare decay in the Bethe-Salpeter equation approach
- Studying the bound state of the system in the Bethe-Salpeter formalism
- Mass spectra, wave functions and mixing effects of the baryon
- Forward-backward asymmetries in in Bethe-Salpeter equation approach
- Electromagnetic form factors of in the Bethe-Salpeter equation approach