  Several new strategies to extract CKM phases, including a determination of
$\gamma$ from $B_{s(d)}\to J/\psi K_S$ decays and a general approach, which
makes use of the angular distributions of certain $B_{d,s}$ modes, such as
$B_d\to J/\psi \rho^0$ and $B_s\to J/\psi \phi$, are discussed. Special
emphasis is put on a simultaneous determination of $\beta$ and $\gamma$ with
the help of the decays $B_d\to \pi^+ \pi^-$ and $B_s\to K^+ K^-$, which relies
only on the $U$-spin flavour symmetry of strong interactions and is not
affected by any penguin or final-state-interaction effects.
