$B^0 \to ωη^{(\prime)}$ and $φη^{(\prime)}$ decays in the perturbative QCD approach

$B^0$--$\overline{B}^0$ mixing and $ε_K$ parameter in the minimal supergravity model

$B^0(\pm)$ decays into two vector mesons. Physical motivations and a general method for simulations

$B^0-\bar{B}^0$ mixing in quenched lattice QCD

$B^0_d-{\bar B}^0_d$ mixing in the left-right supersymmetric model

$B^0_s - \bar{B^0_s}$ Mixing Parameters from Unquenched Lattice QCD

$B^0_s$ Mixing Studies At The Tevatron

$B^0_{d,s}\to μ^-μ^+$ in the MSSM

$B^0_{s(d)} - \bar{B}^0_{s(d)} $ mixing and new physics effects in a top quark two-Higgs doublet model

$B^{(*)}\bar B^{(*)}$ intermediate state contribution to $Υ(4S,5S)\to η_b+γ$ radiative decay

$B^{\ast}B^{\ast}ρ$ vertex from QCD sum rules

$B^{\ast}_{s1}B^{\ast}K$ form factor from QCD sum rules

$B_7$, $B_8$ and chiral Ward identities

$B_c$ and $Υ$ Spectra from Lattice NRQCD - Results at $β$ = 5.7

$B_c$ Meson at LHC

$B_c$ Meson Production around the $Z^0$ Peak at a High Luminosity $e^+ e^-$ Collider

$B_c$ meson production at the Tevatron Revisited

$B_c$ Meson Productions Via Induced Gluon Fragmentation

$B_c$ mesons in a Bethe-Salpeter model

$B_c$ Mesons Production at Hadron Colliders by Heavy Quark Fragmentation