Calculation of Long-Distance Effects in Exclusive Weak Radiative Decays of B-Mesons

We calculate the contribution of the weak annihilation to the $B\rightarrow \rho\gamma$ decay amplitude by means of QCD sum rules using the photon light-cone wave function. We find that this long-distance contribution amounts to about 10\% of the leading short-distance effect in $B^-\rightarrow \rho^-\gamma$. On the other hand, weak annihilation is the dominant source of the corresponding $D$ meson decays and according to our estimates, yields branching ratios of $O(10^{-4})$ for $D^0\rightarrow \bar{K}^{*0}\gamma$, $O(10^{-5})$ for $D_s\rightarrow \rho^+\gamma$, and $O(10^{-6})$ for $D^-\rightarrow \rho^-\gamma$ and for $D^0\rightarrow \rho^0\gamma$.Comment: 14 pages, Latex, two figures added as an uuencoded .ps fil

Magnetic dipole moment of the light tensor mesons in light cone QCD sum rules

The magnetic dipole moments of the light tensor mesons $f_2$, $a_2$ and strange $K_2^{\ast 0} (1430)$ tensor meson are calculated in the framework of the light cone QCD sum rules. It is observed that the values of the magnetic dipole moment for the charged tensor particles are considerably different from zero. These values are very close to zero for the light neutral $f_2$ and $a_2$ tensor mesons, while it has a small nonzero value for the neutral strange $K_2^{\ast 0} (1430)$ tensor meson.Comment: 12 Pages and 1 Tabl