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Xinheng, Guo

Publications and source records attributed to Xinheng, Guo.

Studies of heavy hadron physics

In the diquark picture, we establish Bethe-Salpeter equations for ground states of heavy baryons containing one heavy quark and two heavy quarks in the heavy quark limit, respectively. The Bethe-Salpeter equations for both heavy and light diquarks are also established. Assuming kernels to consist of a scalar confinement term and a one-gluon-exchange term we solve Bethe-Salpeter wave functions numerically in the covariant instantaneous approximation and give some applications including semileptonic and nonleptonic decay widths of heavy baryons, the average kinetic energy of the heavy quark in {Lambda}{sub Q}, {Sigma}{sub Q}{sup (*)}{yields}{Lambda}{sub Q}+{pi} decay widths, and heavy quark distribution functions. We also study possible molecular heavy bound states in the Bethe-Salpeter approach. Proof of QCD factorization for {Lambda}{sub b}{yields}{Lambda}{sub c}{pi} is presented in the framework of QCD factorization.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

QCD factorization for {Lambda}{sub b}{sup 0}{yields}{Lambda}{sub c}{sup +}{pi}{sup -}

We prove that in the limit m{sub b},m{sub c}{yields}{infinity}, with m{sub c}/m{sub b} fixed, factorization holds at order {alpha}{sub s} for the decay {Lambda}{sub b}{sup 0}{yields}{Lambda}{sub c}{sup +}{pi}{sup -}. This proof is done in the infinite-momentum frame in which the momenta of {pi}, {Lambda}{sub c}, and {Lambda}{sub b} go to infinity. Our result is renormalization-scale- and scheme-independent at O({alpha}{sub s}). This is the same as the QCD factorization for B{yields}D{pi}.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Possible BK molecular structure of B{sub s0}*(5725) in the Bethe-Salpeter approach

We interpret the scalar B{sub s0}*(5725) as an S-wave BK molecular bound state in the Bethe-Salpeter approach. In the ladder and instantaneous approximation, with the kernel induced by {rho} and {omega} exchanges, we establish the Bethe-Salpeter equation for B{sub s0}*(5725). We find that the bound state of BK can exist. We also calculate the isospin-violating decay width of the process B{sub s0}*(5725){yields}B{sub s}{pi}{sup 0} through exchanging K{sup *} and B{sup *} mesons including the {eta}-{pi}{sup 0} mixing effect. We hope that the obtained decay width is instructive for the forthcoming experiment.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗