Exclusive charmless nonleptonic decays of the B sub d sup 0 meson in the standard model
Abstract
We have studied the charmless nonleptonic decay such as the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{pi}{sup {minus}}, {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{rho}{sup {minus}}, {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup *+}{pi}{sup {minus}} decays, which include contributions from both Born process and penguin process, in the standard model. The branching ratios of these three decays are predicted to be {similar to}10{sup {minus}5}, {similar to}10{sup {minus}5}--10{sup {minus}6}, and {similar to}10{sup {minus}5}, respectively. For the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{pi}{sup {minus}} decay, the amplitude is dominated by the timelike penguin process. For the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{rho}{sup {minus}} decay, the dominant amplitude follows from the spacelike penguin process, which is ambiguous due to the annihilation form factor. For the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup *+}{pi}{sup {minus}} decay, the contributions of the three processes are comparable to each other. The precise determination of the annihilation form factor is necessary to predict reliably the branching ratios of the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{rho}{sup {minus}} and {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup *+}{pi}{sup {minus}} decays.
- Authors:
-
- Science Education Laboratory, Ehime University, 790 Matsuyama, Japan (JP)
- Department of Physics, Ehime University, 790 Matsuyama, Japan (JP)
- Publication Date:
- OSTI Identifier:
- 5121782
- Resource Type:
- Journal Article
- Journal Name:
- Physical Review (Section) D: Particles and Fields; (USA)
- Additional Journal Information:
- Journal Volume: 40:9; Journal ID: ISSN 0556-2821
- Country of Publication:
- United States
- Language:
- English
- Subject:
- 72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; B NEUTRAL MESONS; WEAK HADRONIC DECAY; ANNIHILATION; BRANCHING RATIO; EXCLUSIVE INTERACTIONS; FLAVOR MODEL; FORM FACTORS; GLUONS; HAMILTONIANS; KAONS PLUS; KOBAYASHI-MASKAWA MATRIX; PIONS MINUS; QUANTUM CHROMODYNAMICS; STANDARD MODEL; B MESONS; BASIC INTERACTIONS; BOSONS; COMPOSITE MODELS; DECAY; ELECTROMAGNETIC INTERACTIONS; ELEMENTARY PARTICLES; FIELD THEORIES; HADRONS; INTERACTIONS; KAONS; MATHEMATICAL MODELS; MATHEMATICAL OPERATORS; MATRICES; MESONS; PARTICLE DECAY; PARTICLE INTERACTIONS; PARTICLE MODELS; PARTICLE PROPERTIES; PIONS; POSTULATED PARTICLES; PSEUDOSCALAR MESONS; QUANTUM FIELD THEORY; QUANTUM OPERATORS; QUARK MODEL; STRANGE MESONS; STRANGE PARTICLES; UNIFIED GAUGE MODELS; UNIFIED-FIELD THEORIES; WEAK PARTICLE DECAY; 645203* - High Energy Physics- Particle Interactions & Properties-Theoretical- Weak Interactions & Properties
Citation Formats
Tanimoto, M, Shinmoto, T, Hirayama, K, and Senba, K. Exclusive charmless nonleptonic decays of the B sub d sup 0 meson in the standard model. United States: N. p., 1989.
Web. doi:10.1103/PhysRevD.40.2934.
Tanimoto, M, Shinmoto, T, Hirayama, K, & Senba, K. Exclusive charmless nonleptonic decays of the B sub d sup 0 meson in the standard model. United States. https://doi.org/10.1103/PhysRevD.40.2934
Tanimoto, M, Shinmoto, T, Hirayama, K, and Senba, K. 1989.
"Exclusive charmless nonleptonic decays of the B sub d sup 0 meson in the standard model". United States. https://doi.org/10.1103/PhysRevD.40.2934.
@article{osti_5121782,
title = {Exclusive charmless nonleptonic decays of the B sub d sup 0 meson in the standard model},
author = {Tanimoto, M and Shinmoto, T and Hirayama, K and Senba, K},
abstractNote = {We have studied the charmless nonleptonic decay such as the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{pi}{sup {minus}}, {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{rho}{sup {minus}}, {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup *+}{pi}{sup {minus}} decays, which include contributions from both Born process and penguin process, in the standard model. The branching ratios of these three decays are predicted to be {similar to}10{sup {minus}5}, {similar to}10{sup {minus}5}--10{sup {minus}6}, and {similar to}10{sup {minus}5}, respectively. For the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{pi}{sup {minus}} decay, the amplitude is dominated by the timelike penguin process. For the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{rho}{sup {minus}} decay, the dominant amplitude follows from the spacelike penguin process, which is ambiguous due to the annihilation form factor. For the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup *+}{pi}{sup {minus}} decay, the contributions of the three processes are comparable to each other. The precise determination of the annihilation form factor is necessary to predict reliably the branching ratios of the {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup +}{rho}{sup {minus}} and {ital B}{sub {ital d}}{sup 0}{r arrow}{ital K}{sup *+}{pi}{sup {minus}} decays.},
doi = {10.1103/PhysRevD.40.2934},
url = {https://www.osti.gov/biblio/5121782},
journal = {Physical Review (Section) D: Particles and Fields; (USA)},
issn = {0556-2821},
number = ,
volume = 40:9,
place = {United States},
year = {Wed Nov 01 00:00:00 EST 1989},
month = {Wed Nov 01 00:00:00 EST 1989}
}