Exclusive heavy meson pair production by γγ collision in heavy quark effective theory
暂无分享,去创建一个
[1] A. Falk. Hadrons of arbitrary spin in the heavy quark effective theory , 1992 .
[2] B. Grinstein,et al. Leading mass corrections to the heavy quark effective theory , 1991 .
[3] T. Mannel,et al. Baryons in the heavy quark effective theory , 1991 .
[4] B. Grinstein,et al. Heavy meson pair production in e+e− annihilation from the static quark effective theory , 1990 .
[5] T. Mannel,et al. Spin symmetry in nonleptonic B decays , 1990 .
[6] T. Mannel,et al. Spin symmetry in e+e− annihilation into heavy mesons , 1990 .
[7] B. Grinstein. The Static Quark Effective Theory , 1990 .
[8] H. Georgi. An Effective Field Theory for Heavy Quarks at Low-energies , 1990 .
[9] M. Wise,et al. Weak transition form factors between heavy mesons , 1990 .
[10] Estia Eichten,et al. A Fermi National Accelerator Laboratory FERMILAB-PUB-891184-T An Effective Field Theory for the Calculation of Matrix Elements Involving Heavy Quarks , 1998 .
[11] M. Wise,et al. Weak decays of heavy mesons in the static quark approximation , 1989 .
[12] H. Politzer,et al. Effective field theory approach to processes involving both light and heavy fields , 1988 .
[13] S. Cooper. Meson Production in Two-Photon Collisions , 1988 .
[14] S. Brodsky,et al. Large-angle two-photon exclusive channels in quantum chromodynamics , 1981 .