Pseudovector versus pseudoscalar theory in kaon photoproduction from nucleons and nuclei
Journal Article
·
· Phys. Rev. C; (United States)
The reaction /sup 1/H(..gamma..,K/sup +/)..lambda../sup 0/ is used to compare pseudovector with pseudoscalar coupling for the K..lambda..N vertex. The operator is based on diagrammatic techniques and includes the Born terms along with the K/sup */ and ..sigma.. exchange terms. Obtaining the coupling constants from a least squares fit shows that the data do not prefer one coupling over the other. Implanting the process into the nucleus yields only small differences between the two interactions.
- Research Organization:
- Department of Physics and Astronomy, Ohio University, Athens, Ohio 45701
- OSTI ID:
- 6396371
- Journal Information:
- Phys. Rev. C; (United States), Journal Name: Phys. Rev. C; (United States) Vol. 36:1; ISSN PRVCA
- Country of Publication:
- United States
- Language:
- English
Similar Records
Electromagnetic production of. sigma. hypernuclei
ON THE EQUIVALENCE BETWEEN PSEUDOSCALAR AND PSEUDOVECTOR COUPLINGS
Pseudoscalar versus pseudovector pion-nucleon couplings in the nucleonic axion bremsstrahlung rate of neutron-star matter
Journal Article
·
Mon May 01 00:00:00 EDT 1989
· Phys. Rev. C; (United States)
·
OSTI ID:6065899
ON THE EQUIVALENCE BETWEEN PSEUDOSCALAR AND PSEUDOVECTOR COUPLINGS
Journal Article
·
Wed Aug 01 00:00:00 EDT 1962
· Nuovo Cimento (Italy) Divided into Nuovo Cimento A and Nuovo Cimento B
·
OSTI ID:4811525
Pseudoscalar versus pseudovector pion-nucleon couplings in the nucleonic axion bremsstrahlung rate of neutron-star matter
Journal Article
·
Sat Apr 15 00:00:00 EDT 1989
· Phys. Rev. D; (United States)
·
OSTI ID:6193212
Related Subjects
653003* -- Nuclear Theory-- Nuclear Reactions & Scattering
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BARYONS
BASIC INTERACTIONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
BORN APPROXIMATION
BORON 12
BORON ISOTOPES
BOSONS
CARBON 12 TARGET
COUPLING
COUPLING CONSTANTS
CROSS SECTIONS
ELECTROMAGNETIC INTERACTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY RANGE
FERMIONS
GAUGE INVARIANCE
GEV RANGE
GEV RANGE 01-10
HADRONS
HYDROGEN 1 TARGET
HYPERONS
IMPULSE APPROXIMATION
INTERACTIONS
INVARIANCE PRINCIPLES
ISOTOPES
KAONS
KAONS PLUS
LAMBDA BARYONS
LAMBDA PARTICLES
LEAST SQUARE FIT
LIGHT NUCLEI
MAXIMUM-LIKELIHOOD FIT
MESONS
NUCLEAR REACTIONS
NUCLEI
NUCLEONS
NUMERICAL SOLUTION
ODD-ODD NUCLEI
PARTICLE PRODUCTION
PHOTONUCLEAR REACTIONS
PHOTOPRODUCTION
PROPAGATOR
PSEUDOSCALAR MESONS
PSEUDOSCALARS
PSEUDOVECTOR COUPLING
RADIOISOTOPES
SECONDS LIVING RADIOISOTOPES
SIGMA BARYONS
SIGMA PARTICLES
STRANGE MESONS
STRANGE PARTICLES
TARGETS
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BARYONS
BASIC INTERACTIONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
BORN APPROXIMATION
BORON 12
BORON ISOTOPES
BOSONS
CARBON 12 TARGET
COUPLING
COUPLING CONSTANTS
CROSS SECTIONS
ELECTROMAGNETIC INTERACTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY RANGE
FERMIONS
GAUGE INVARIANCE
GEV RANGE
GEV RANGE 01-10
HADRONS
HYDROGEN 1 TARGET
HYPERONS
IMPULSE APPROXIMATION
INTERACTIONS
INVARIANCE PRINCIPLES
ISOTOPES
KAONS
KAONS PLUS
LAMBDA BARYONS
LAMBDA PARTICLES
LEAST SQUARE FIT
LIGHT NUCLEI
MAXIMUM-LIKELIHOOD FIT
MESONS
NUCLEAR REACTIONS
NUCLEI
NUCLEONS
NUMERICAL SOLUTION
ODD-ODD NUCLEI
PARTICLE PRODUCTION
PHOTONUCLEAR REACTIONS
PHOTOPRODUCTION
PROPAGATOR
PSEUDOSCALAR MESONS
PSEUDOSCALARS
PSEUDOVECTOR COUPLING
RADIOISOTOPES
SECONDS LIVING RADIOISOTOPES
SIGMA BARYONS
SIGMA PARTICLES
STRANGE MESONS
STRANGE PARTICLES
TARGETS