Determining the weak phase γ from chargedBdecays

A quadrangle relation is shown to be satisfied by the amplitudes for ${\mathit{B}}^{+}$→${\mathrm{\pi }}^0$ ${\mathit{K}}^{+}$, ${\mathrm{\pi }}^{+}$ ${\mathit{K}}^0$, η${\mathit{K}}^{+}$, and ${\mathrm{\eta }}^{\prime }$ ${\mathit{K}}^{+}$. By comparison with the corresponding relation satisfied by ${\mathit{B}}^{\mathrm{-}}$ decay amplitudes, it is shown that the relative phases of all the amplitudes can be determined up to discrete ambiguities. Making use of an SU(3) relation between amplitudes contributing to the above decays and those contributing to ${\mathit{B}}^{\pm }$→${\mathrm{\pi }}^{\pm }$ ${\mathrm{\pi }}^0$, it is then shown that one can determine the weak phase γ≡Arg(${\mathit{V}}_{\mathit{ub}}^{\mathrm{*}}$ ${\mathit{V}}_{\mathit{cb}}$ /${\mathit{V}}_{\mathit{us}}^{\mathrm{*}}$ ${\mathit{V}}_{\mathit{cs}}$), where V is the Cabibbo-Kobayashi-Maskawa matrix describing the charge-changing weak interactions between the quarks (u,c,t) and (d,s,b). © 1996 The American Physical Society.