Exclusive charmless nonleptonic decays of the B sub d sup 0 meson in the standard model
Journal Article
·
· Physical Review (Section) D: Particles and Fields; (USA)
- Science Education Laboratory, Ehime University, 790 Matsuyama, Japan (JP)
- Department of Physics, Ehime University, 790 Matsuyama, Japan (JP)
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.
- OSTI ID:
- 5121782
- Journal Information:
- Physical Review (Section) D: Particles and Fields; (USA), Journal Name: Physical Review (Section) D: Particles and Fields; (USA) Vol. 40:9; ISSN PRVDA; ISSN 0556-2821
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
645203* -- High Energy Physics-- Particle Interactions & Properties-Theoretical-- Weak Interactions & Properties
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
ANNIHILATION
B MESONS
B NEUTRAL MESONS
BASIC INTERACTIONS
BOSONS
BRANCHING RATIO
COMPOSITE MODELS
DECAY
ELECTROMAGNETIC INTERACTIONS
ELEMENTARY PARTICLES
EXCLUSIVE INTERACTIONS
FIELD THEORIES
FLAVOR MODEL
FORM FACTORS
GLUONS
HADRONS
HAMILTONIANS
INTERACTIONS
KAONS
KAONS PLUS
KOBAYASHI-MASKAWA MATRIX
MATHEMATICAL MODELS
MATHEMATICAL OPERATORS
MATRICES
MESONS
PARTICLE DECAY
PARTICLE INTERACTIONS
PARTICLE MODELS
PARTICLE PROPERTIES
PIONS
PIONS MINUS
POSTULATED PARTICLES
PSEUDOSCALAR MESONS
QUANTUM CHROMODYNAMICS
QUANTUM FIELD THEORY
QUANTUM OPERATORS
QUARK MODEL
STANDARD MODEL
STRANGE MESONS
STRANGE PARTICLES
UNIFIED GAUGE MODELS
UNIFIED-FIELD THEORIES
WEAK HADRONIC DECAY
WEAK PARTICLE DECAY
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
ANNIHILATION
B MESONS
B NEUTRAL MESONS
BASIC INTERACTIONS
BOSONS
BRANCHING RATIO
COMPOSITE MODELS
DECAY
ELECTROMAGNETIC INTERACTIONS
ELEMENTARY PARTICLES
EXCLUSIVE INTERACTIONS
FIELD THEORIES
FLAVOR MODEL
FORM FACTORS
GLUONS
HADRONS
HAMILTONIANS
INTERACTIONS
KAONS
KAONS PLUS
KOBAYASHI-MASKAWA MATRIX
MATHEMATICAL MODELS
MATHEMATICAL OPERATORS
MATRICES
MESONS
PARTICLE DECAY
PARTICLE INTERACTIONS
PARTICLE MODELS
PARTICLE PROPERTIES
PIONS
PIONS MINUS
POSTULATED PARTICLES
PSEUDOSCALAR MESONS
QUANTUM CHROMODYNAMICS
QUANTUM FIELD THEORY
QUANTUM OPERATORS
QUARK MODEL
STANDARD MODEL
STRANGE MESONS
STRANGE PARTICLES
UNIFIED GAUGE MODELS
UNIFIED-FIELD THEORIES
WEAK HADRONIC DECAY
WEAK PARTICLE DECAY