Chiral Perturbation Theory for $f_{D_S}/f_D$ and $B_{B_S}/B_{B}$
| dc.creator | Grinstein, B. | |
| dc.creator | Jenkins, E. | |
| dc.creator | Manohar, A. V. | |
| dc.creator | Savage, M. J. | |
| dc.creator | Wise, M. B. | |
| dc.date | 1992-04-03 | |
| dc.date.accessioned | 2026-07-07T10:34:53Z | |
| dc.date.available | 2026-07-07T10:34:53Z | |
| dc.description | The decay constants for the $D$ and $D_S$ mesons, denoted $f_D$ and $f_{D_S}$ respectively, are equal in the $SU(3)_V$ limit, as are the hadronic amplitudes for $B_S-\bar B_S$ and $B^0-\bar B^0$ mixing. The leading $SU(3)_V$ violating contribution to $\left( f_{D_S} / f_D \right)$ and to the ratio of hadronic matrix elements relevant for $B_S-\bar B_S$ and $B^0-\bar B^0$ mixing amplitudes are calculated in chiral perturbation theory. We discuss the formalism needed to include both meson and anti-meson fields in the heavy quark effective theory. | |
| dc.description | 10 pages, 2 figures | |
| dc.identifier | https://arxiv.org/abs/hep-ph/9204207 | |
| dc.identifier | http://arxiv.org/abs/hep-ph/9204207 | |
| dc.identifier | Nucl.Phys.B380:369-376,1992 | |
| dc.identifier | doi:10.1016/0550-3213(92)90248-A | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/179585 | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Chiral Perturbation Theory for $f_{D_S}/f_D$ and $B_{B_S}/B_{B}$ | |
| dc.type | text |