Fragmentation of Gamow-Teller strength observed in [sup 117,120]Sn([sup 3]He,[ital t])[sup 117,120]Sb charge-exchange reactions
Journal Article
·
· Physical Review, C (Nuclear Physics); (United States)
- Department of Physics, University of Michigan, Ann Arbor, Michigan 48109 (United States)
- Faculteit Natuurkunde en Sterrenkunde, Vrije Universiteit, 1081 HV Amsterdam (Netherlands)
- Indiana University Cyclotron Facility, Bloomington, Indiana 47405 (United States)
- Kernfysisch Versneller Instituut, 9747 AA Groningen (Netherlands)
- Engineering Physics Institute, 115 409 Moscow (Russian Federation)
The ([sup 3]He,[ital t]) charge-exchange reaction has been studied at [ital E]([sup 3]He)=200 MeV and angles near 0[degree] on targets of [sup 117]Sn and [sup 120]Sn. Fragmentation of the giant Gamow-Teller resonance into separate components of the particle-hole type has been observed in good agreement with theoretical predictions. These components are connected with what is usually referred to in the literature as direct-, core-polarization-, and back-spin-flip Gamow-Teller strength. The observed cross sections near [theta]=0[degree] suggest contributions from the isovector spin-flip interaction as well as the isovector tensor interaction. A theoretically predicted configuration splitting of the main Gamow-Teller component into two components involving the 1[ital h][sub 11/2] neutron orbital could not uniquely be identified. The data are compatible, though, with such a splitting since the observed widths of the main Gamow-Teller components in [sup 117]Sb and [sup 120]Sb exceed the predicted splittings.
- OSTI ID:
- 5801294
- Journal Information:
- Physical Review, C (Nuclear Physics); (United States), Journal Name: Physical Review, C (Nuclear Physics); (United States) Vol. 48:6; ISSN 0556-2813; ISSN PRVCAN
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
663300 -- Nuclear Reactions & Scattering
General-- (1992-)
663440* -- D-
T-
& He-induced Reactions & Scattering-- (1992-)
663560 -- Nuclear Mass Ranges-- A=90-149-- (1992-)
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ANTIMONY 117
ANTIMONY 120
ANTIMONY ISOTOPES
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CHARGE-EXCHANGE REACTIONS
CHARGED PARTICLES
CHARGED-PARTICLE REACTIONS
CROSS SECTIONS
DAYS LIVING RADIOISOTOPES
ELECTRON CAPTURE RADIOISOTOPES
ENERGY RANGE
FRAGMENTATION
GAMOW-TELLER RULES
HELIUM 3 REACTIONS
HOURS LIVING RADIOISOTOPES
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
MEV RANGE
MEV RANGE 100-1000
MINUTES LIVING RADIOISOTOPES
NANOSEC LIVING RADIOISOTOPES
NUCLEAR REACTIONS
NUCLEI
ODD-EVEN NUC
ODD-ODD NUCLEI
RADIOISOTOPES
RESONANCE
SPIN FLIP
TARGETS
TIN 117 TARGET
TIN 120 TARGET
TRITONS
General-- (1992-)
663440* -- D-
T-
& He-induced Reactions & Scattering-- (1992-)
663560 -- Nuclear Mass Ranges-- A=90-149-- (1992-)
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ANTIMONY 117
ANTIMONY 120
ANTIMONY ISOTOPES
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CHARGE-EXCHANGE REACTIONS
CHARGED PARTICLES
CHARGED-PARTICLE REACTIONS
CROSS SECTIONS
DAYS LIVING RADIOISOTOPES
ELECTRON CAPTURE RADIOISOTOPES
ENERGY RANGE
FRAGMENTATION
GAMOW-TELLER RULES
HELIUM 3 REACTIONS
HOURS LIVING RADIOISOTOPES
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
MEV RANGE
MEV RANGE 100-1000
MINUTES LIVING RADIOISOTOPES
NANOSEC LIVING RADIOISOTOPES
NUCLEAR REACTIONS
NUCLEI
ODD-EVEN NUC
ODD-ODD NUCLEI
RADIOISOTOPES
RESONANCE
SPIN FLIP
TARGETS
TIN 117 TARGET
TIN 120 TARGET
TRITONS