Actinide Neutron-Induced Fission Cross Section Measurements At LANSCE
Journal Article
·
· AIP Conference Proceedings
- Los Alamos National Laboratory, Los Alamos NM 87545 (United States)
- Idaho National Laboratory, Idaho Falls ID 83415 (United States)
Fission cross sections of a range of actinides have been measured at the Los Alamos Neutron Science Center (LANSCE) in support of nuclear energy applications in a wide energy range from sub thermal energies up to 200 MeV. Parallel-plate ionization chambers are used to measure fission cross sections ratios relative to the {sup 235}U standard while incident neutron energies are determined using the time-of-flight method. Recent measurements include the {sup 233,238}U, {sup 239-242}Pu and {sup 243}Am neutron-induced fission cross sections. Obtained data are presented in comparison with existing evaluations and previous data.
- OSTI ID:
- 21513431
- Journal Information:
- AIP Conference Proceedings, Vol. 1336, Issue 1; Conference: CAARI 2010: 21. International Conference on the Application of Accelerators in Research and Industry, Fort Worth, TX (United States), 8-13 Aug 2010; Other Information: DOI: 10.1063/1.3586173; (c) 2011 American Institute of Physics; ISSN 0094-243X
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ACTINIDES
AMERICIUM 243
COMPARATIVE EVALUATIONS
CROSS SECTIONS
FISSION
IONIZATION CHAMBERS
LINEAR ACCELERATORS
MEV RANGE 100-1000
NEUTRON SOURCES
NEUTRONS
NUCLEAR ENERGY
PLUTONIUM 239
PLUTONIUM 240
PLUTONIUM 241
PLUTONIUM 242
TIME-OF-FLIGHT METHOD
URANIUM 233
URANIUM 235
URANIUM 238
ACCELERATORS
ACTINIDE NUCLEI
ALPHA DECAY RADIOISOTOPES
AMERICIUM ISOTOPES
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
ELEMENTARY PARTICLES
ELEMENTS
ENERGY
ENERGY RANGE
EVALUATION
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
FERMIONS
HADRONS
HEAVY ION DECAY RADIOISOTOPES
HEAVY NUCLEI
INTERNAL CONVERSION RADIOISOTOPES
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
MEASURING INSTRUMENTS
METALS
MEV RANGE
MINUTES LIVING RADIOISOTOPES
NEON 24 DECAY RADIOISOTOPES
NUCLEAR REACTIONS
NUCLEI
NUCLEONS
ODD-EVEN NUCLEI
PARTICLE SOURCES
PLUTONIUM ISOTOPES
RADIATION DETECTORS
RADIATION SOURCES
RADIOISOTOPES
SPONTANEOUS FISSION RADIOISOTOPES
URANIUM ISOTOPES
YEARS LIVING RADIOISOTOPES
ACTINIDES
AMERICIUM 243
COMPARATIVE EVALUATIONS
CROSS SECTIONS
FISSION
IONIZATION CHAMBERS
LINEAR ACCELERATORS
MEV RANGE 100-1000
NEUTRON SOURCES
NEUTRONS
NUCLEAR ENERGY
PLUTONIUM 239
PLUTONIUM 240
PLUTONIUM 241
PLUTONIUM 242
TIME-OF-FLIGHT METHOD
URANIUM 233
URANIUM 235
URANIUM 238
ACCELERATORS
ACTINIDE NUCLEI
ALPHA DECAY RADIOISOTOPES
AMERICIUM ISOTOPES
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
ELEMENTARY PARTICLES
ELEMENTS
ENERGY
ENERGY RANGE
EVALUATION
EVEN-EVEN NUCLEI
EVEN-ODD NUCLEI
FERMIONS
HADRONS
HEAVY ION DECAY RADIOISOTOPES
HEAVY NUCLEI
INTERNAL CONVERSION RADIOISOTOPES
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
MEASURING INSTRUMENTS
METALS
MEV RANGE
MINUTES LIVING RADIOISOTOPES
NEON 24 DECAY RADIOISOTOPES
NUCLEAR REACTIONS
NUCLEI
NUCLEONS
ODD-EVEN NUCLEI
PARTICLE SOURCES
PLUTONIUM ISOTOPES
RADIATION DETECTORS
RADIATION SOURCES
RADIOISOTOPES
SPONTANEOUS FISSION RADIOISOTOPES
URANIUM ISOTOPES
YEARS LIVING RADIOISOTOPES