Thermal neutron capture cross-section to {sup 113}Cd isomer for the study of s-process origin of {sup 115}Sn
Journal Article
·
· AIP Conference Proceedings
- Kansai Photon Science Institute, Japan Atomic Energy Agency, Kizu, Kyoto 619-0215 (Japan)
- Japan Atomic Energy Agency, Tokai, Ibaraki 319-1195 (Japan)
- National Astronomical Observatory, Osawa, Mitaka, Tokyo 181-8588 (Japan)
The astrophysical origin of a p-nucleus {sup 115}Sn has remained still an open question. The nucleus {sup 115}Sn may be produced by a weak branch of the s-process through a beta-unstable isomer in {sup 113}Cd. However, a neutron capture cross-section to this isomer has not been measured with high accuracy at any energy. A neutron capture cross-section for the {sup 112}Cd(n,gamma){sup 113}Cd{sup m} reaction has been measured with neutrons provided from a nuclear reactor. The nucleus {sup 115}Sn may be produced by a nucleosynthesis flow through {sup 113}Cd{sup m} in the s-process. We have obtained the thermal neutron capture cross-section of 0.028+-0.009[b] and the resonance integral of 1.1+-0.3[b] using a cadmium difference method. The cross-section ratio of the isomer to the ground state has been calculated as a function of the incident neutron energy, E, by using a statistical model. The calculated ratios are almost constant over a wide range of E<100 keV. We have evaluated the s-process contribution to the solar abundance of {sup 115}Sn using the classical steady-flow model. This calculated result has shown that the production through {sup 113}Cd{sup m} may be minor contribution to {sup 115}Sn.
- OSTI ID:
- 21362108
- Journal Information:
- AIP Conference Proceedings, Journal Name: AIP Conference Proceedings Journal Issue: 1 Vol. 1238; ISSN APCPCS; ISSN 0094-243X
- Country of Publication:
- United States
- Language:
- English
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OSTI ID:21392590
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Related Subjects
79 ASTRONOMY AND ASTROPHYSICS
ABUNDANCE
ASTROPHYSICS
BARYON REACTIONS
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
CADMIUM 112
CADMIUM 112 TARGET
CADMIUM 113
CADMIUM ISOTOPES
CAPTURE
CROSS SECTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY RANGE
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
EVOLUTION
FERMIONS
FLUID FLOW
GROUND STATES
HADRON REACTIONS
HADRONS
INTEGRALS
INTERMEDIATE MASS NUCLEI
INTERNAL CONVERSION RADIOISOTOPES
ISOMERIC TRANSITION ISOTOPES
ISOMERS
ISOTOPES
KEV RANGE
KEV RANGE 10-100
MATHEMATICAL MODELS
NEUTRON REACTIONS
NEUTRONS
NUCLEAR REACTIONS
NUCLEI
NUCLEON REACTIONS
NUCLEONS
NUCLEOSYNTHESIS
PHYSICS
RADIOISOTOPES
RESONANCE INTEGRALS
S PROCESS
STABLE ISOTOPES
STAR EVOLUTION
STATISTICAL MODELS
STEADY FLOW
SYNTHESIS
TARGETS
THERMAL NEUTRONS
TIN 115
TIN ISOTOPES
YEARS LIVING RADIOISOTOPES
ABUNDANCE
ASTROPHYSICS
BARYON REACTIONS
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
CADMIUM 112
CADMIUM 112 TARGET
CADMIUM 113
CADMIUM ISOTOPES
CAPTURE
CROSS SECTIONS
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY RANGE
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
EVOLUTION
FERMIONS
FLUID FLOW
GROUND STATES
HADRON REACTIONS
HADRONS
INTEGRALS
INTERMEDIATE MASS NUCLEI
INTERNAL CONVERSION RADIOISOTOPES
ISOMERIC TRANSITION ISOTOPES
ISOMERS
ISOTOPES
KEV RANGE
KEV RANGE 10-100
MATHEMATICAL MODELS
NEUTRON REACTIONS
NEUTRONS
NUCLEAR REACTIONS
NUCLEI
NUCLEON REACTIONS
NUCLEONS
NUCLEOSYNTHESIS
PHYSICS
RADIOISOTOPES
RESONANCE INTEGRALS
S PROCESS
STABLE ISOTOPES
STAR EVOLUTION
STATISTICAL MODELS
STEADY FLOW
SYNTHESIS
TARGETS
THERMAL NEUTRONS
TIN 115
TIN ISOTOPES
YEARS LIVING RADIOISOTOPES