Cross sections for {alpha}-particle induced reactions on {sup 115,116}Sn around the Coulomb barrier
Journal Article
·
· Physical Review. C, Nuclear Physics
- 'Horia Hulubei' National Institute for Physics and Nuclear Engineering, P.O. Box MG-6, 077125 Bucharest-Magurele (Romania)
- Nuclear Physics Department, University of Bucharest, Bucharest (Romania)
- Physics Department, University Politehnica of Bucharest, Bucharest (Romania)
The cross sections of the {sup 115}Sn({alpha},{gamma}){sup 119}Te, {sup 115}Sn({alpha},n){sup 118}Te, and {sup 116}Sn({alpha},n){sup 119}Te reactions (both on ground and isomeric states) have been measured at effective center-of-mass energies from 9.3 to 14.8 MeV. During a first experiment, enriched self-supporting {sup 115}Sn (51.2%) + {sup 116}Sn (24.4%) foils were bombarded with an {alpha} beam delivered by the Bucharest IFIN-HH Tandem Accelerator. In a second experiment, a highly enriched {sup 116}Sn target was irradiated in order to disentangle the experimental cross section contributions due to {sup 115}Sn({alpha},{gamma}){sup 119}Te and {sup 115}Sn({alpha},n){sup 118}Te reactions obtained in the first measurement. The beam-induced activity was measured with two large volume HPGe detectors in close geometry. The experimental results were compared with theoretical predictions obtained in the framework of the statistical model.
- OSTI ID:
- 21502793
- Journal Information:
- Physical Review. C, Nuclear Physics, Journal Name: Physical Review. C, Nuclear Physics Journal Issue: 6 Vol. 83; ISSN 0556-2813; ISSN PRVCAN
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ACCELERATORS
ALPHA PARTICLES
ALPHA REACTIONS
BEAMS
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CENTER-OF-MASS SYSTEM
CHARGED PARTICLES
CHARGED-PARTICLE REACTIONS
COULOMB FIELD
CROSS SECTIONS
DAYS LIVING RADIOISOTOPES
DECAY
ELECTRIC FIELDS
ELECTRON CAPTURE RADIOISOTOPES
ELECTROSTATIC ACCELERATORS
EMISSION
ENERGY RANGE
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
FOILS
FORECASTING
GAMMA DECAY
GE SEMICONDUCTOR DETECTORS
HIGH-PURITY GE DETECTORS
HOURS LIVING RADIOISOTOPES
INTERMEDIATE MASS NUCLEI
IONIZING RADIATIONS
ISOTOPES
MATHEMATICAL MODELS
MEASURING INSTRUMENTS
MEV RANGE
MEV RANGE 10-100
NEUTRON EMISSION
NUCLEAR DECAY
NUCLEAR REACTIONS
NUCLEI
RADIATION DETECTORS
RADIATIONS
RADIOISOTOPES
SEMICONDUCTOR DETECTORS
STABLE ISOTOPES
STATISTICAL MODELS
TANDEM ELECTROSTATIC ACCELERATORS
TELLURIUM 118
TELLURIUM 119
TELLURIUM ISOTOPES
TIN 115
TIN 116
TIN ISOTOPES
ACCELERATORS
ALPHA PARTICLES
ALPHA REACTIONS
BEAMS
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CENTER-OF-MASS SYSTEM
CHARGED PARTICLES
CHARGED-PARTICLE REACTIONS
COULOMB FIELD
CROSS SECTIONS
DAYS LIVING RADIOISOTOPES
DECAY
ELECTRIC FIELDS
ELECTRON CAPTURE RADIOISOTOPES
ELECTROSTATIC ACCELERATORS
EMISSION
ENERGY RANGE
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
FOILS
FORECASTING
GAMMA DECAY
GE SEMICONDUCTOR DETECTORS
HIGH-PURITY GE DETECTORS
HOURS LIVING RADIOISOTOPES
INTERMEDIATE MASS NUCLEI
IONIZING RADIATIONS
ISOTOPES
MATHEMATICAL MODELS
MEASURING INSTRUMENTS
MEV RANGE
MEV RANGE 10-100
NEUTRON EMISSION
NUCLEAR DECAY
NUCLEAR REACTIONS
NUCLEI
RADIATION DETECTORS
RADIATIONS
RADIOISOTOPES
SEMICONDUCTOR DETECTORS
STABLE ISOTOPES
STATISTICAL MODELS
TANDEM ELECTROSTATIC ACCELERATORS
TELLURIUM 118
TELLURIUM 119
TELLURIUM ISOTOPES
TIN 115
TIN 116
TIN ISOTOPES