Multipole amplitudes in parity-changing one-photon transitions of charmonium
Journal Article
·
· Physical Review, D (Particles Fields); (United States)
- Department of Physics, University of Lowell, Lowell, Massachusetts 01854 (United States)
- Department of Physics, The Pennsylvania State University, University Park, Pennsylvania 16802 (United States)
- The Pennsylvania State University, New Kensington Campus, New Kensington, Pennsylvania 15068 (United States)
We calculate the normalized helicity and multipole amplitudes in the one-photon transitions {psi}{prime}{prime}{r arrow}{chi}{sub {ital J}}+{gamma}, {psi}{prime}{r arrow}{chi}{sub {ital J}}+{gamma}, and {chi}{sub {ital J}}{r arrow}{psi}+{gamma} in any potential model. In the {chi}{sub 2}{r arrow}{psi}+{gamma} and {chi}{sub 1}{r arrow}{psi}+{gamma} decays the normalized {ital M}2 amplitude is independent of the potential to order {ital k}/{ital m} (where {ital k} is the photon energy and {ital m} the {ital c}-quark mass) so long as {psi} has no {ital D}-state mixing and {chi}{sub {ital J}} has no {ital F}-state mixing. They are a multiple of {ital k}/{ital m} and can be quite appreciable. Also the {ital E}3 amplitude in {chi}{sub 2}{r arrow}{psi}+{gamma} is zero with the same approximations. The same statement can be made about the {psi}{prime}{prime}{r arrow}{chi}{sub {ital J}}+{gamma} and {psi}{prime}{r arrow}{chi}{sub {ital J}}+{gamma} decays, so long as {psi}{prime} has no {ital D}-state mixing or {psi}{prime}{prime} has no {ital S}-state mixing. But if {psi}{prime} has a significant {ital D}-state mixing or {psi}{prime}{prime} has an {ital S}-state mixing, which is quite probable, the result will be a function of certain overlap integrals which may depend on the potential. The {ital M}2 amplitude depends sensitively on any possible anomalous magnetic moment of the {ital c} quark. We also calculate the numerical values of the multipole amplitudes in {psi}{prime}{r arrow}{chi}{sub {ital J}}+{gamma}, {psi}{prime}{prime}{r arrow}{chi}{sub {ital J}}+{gamma}, and {chi}{sub {ital J}}{r arrow}{psi}+{gamma} ({ital J}=1,2) in two different potential models.
- OSTI ID:
- 7301741
- Journal Information:
- Physical Review, D (Particles Fields); (United States), Journal Name: Physical Review, D (Particles Fields); (United States) Vol. 45:9; ISSN PRVDA; ISSN 0556-2821
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
662340 -- Hadron Interactions-- (1992-)
662350* -- Decays of Mesons-- (1992-)
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
ANGULAR DISTRIBUTION
BARYON-BARYON INTERACTIONS
BOSONS
CHARMONIUM
D STATES
DISTRIBUTION
ELECTRON-POSITRON INTERACTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY SPECTRA
ENERGY-LEVEL TRANSITIONS
F STATES
FERMIONS
HADRON-HADRON INTERACTIONS
HADRONS
HELICITY
INTERACTIONS
LEPTON-LEPTON INTERACTIONS
M2-TRANSITIONS
MAGNETIC MOMENTS
MASS
MASSLESS PARTICLES
MESONS
MULTIPOLE TRANSITIONS
MULTIPOLES
NUCLEON-ANTINUCLEON INTERACTIONS
PARTICLE INTERACTIONS
PARTICLE PRODUCTION
PARTICLE PROPERTIES
PHOTONS
POSTULATED PARTICLES
POTENTIALS
PROTON-ANTIPROTON INTERACTIONS
QUARKONIUM
QUARKS
SPECTRA
662350* -- Decays of Mesons-- (1992-)
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
ANGULAR DISTRIBUTION
BARYON-BARYON INTERACTIONS
BOSONS
CHARMONIUM
D STATES
DISTRIBUTION
ELECTRON-POSITRON INTERACTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY SPECTRA
ENERGY-LEVEL TRANSITIONS
F STATES
FERMIONS
HADRON-HADRON INTERACTIONS
HADRONS
HELICITY
INTERACTIONS
LEPTON-LEPTON INTERACTIONS
M2-TRANSITIONS
MAGNETIC MOMENTS
MASS
MASSLESS PARTICLES
MESONS
MULTIPOLE TRANSITIONS
MULTIPOLES
NUCLEON-ANTINUCLEON INTERACTIONS
PARTICLE INTERACTIONS
PARTICLE PRODUCTION
PARTICLE PROPERTIES
PHOTONS
POSTULATED PARTICLES
POTENTIALS
PROTON-ANTIPROTON INTERACTIONS
QUARKONIUM
QUARKS
SPECTRA