Abstract
We describe a calculation of the two-photon decays of heavy vector-mesons, B* → Bγγ and D* → Dγγ, by using the "heavy meson chiral Lagrangian". The decay amplitudes are expressed in terms of the strong coupling g of the Lagrangian at various powers and the strength of the anomalous magnetic dipole μB* Bγ (respectively μD* Dγ). In the charm case we are able to express the branching ratio Γ(D*0 → D0γγ)/Γ(D*0) as a function of g only and we expect it to be in the 10-6 - 10-5 range, depending on the value of g. The determination of μB*0 B0γ, μB*+B+γ requires a more involved analysis, including the consideration of bremsstrahlung radiation for the B*+ → B+γγ case.
| Original language | English |
|---|---|
| Pages (from-to) | 134-139 |
| Number of pages | 6 |
| Journal | Nuclear Physics B - Proceedings Supplements |
| Volume | 93 |
| Issue number | 1-3 |
| DOIs | |
| State | Published - Mar 2001 |
| Externally published | Yes |
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