(p,pxn) and (p,xn) reactions and mechanisms on /sup 133/Cs at 550 MeV
Journal Article
·
· Phys. Rev., C; (United States)
The mechanism of the (p,pn) reaction on /sup 133/Cs with 550 MeV protons was deduced by measuring the recoil angular distribution between 0/sup 0/ and 180/sup 0/, and the differential range distribution at 0/sup 0/ and 90/sup 0/, for /sup 132/Cs recoil nuclei. Similar measurements were made for the (p,p4n) and (p,3n) reaction products from /sup 133/Cs. Cross sections were also measured for the production of (p,pxn) and (p,xn) products. The experimental data were compared to predictions derived from Monte Carlo cascade and evaporation calculations, as well as from simple kinematic models of possible reaction mechanisms. The results indicate that about 80% of the (p,pn) reaction takes place by (p,p') events followed by neutron evaporation.
- Research Organization:
- Department of Chemistry, Carnegie-Mellon University, Pittsburgh, Pennsylvania 15213
- OSTI ID:
- 7329703
- Journal Information:
- Phys. Rev., C; (United States), Journal Name: Phys. Rev., C; (United States) Vol. 15:2; ISSN PRVCA
- Country of Publication:
- United States
- Language:
- English
Similar Records
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(p,xn), (p,pxn), and (p,2pxn) reactions for medium-mass nuclei at 12 GeV
Technical Report
·
Sun Dec 30 23:00:00 EST 1973
·
OSTI ID:4934888
Investigation of Spallation Reactions on {sup 120}Sn and (d, xn), (d, pxn), (p, xn), and (p, pxn) Reactions on Enriched Tin Isotopes
Journal Article
·
Mon Jan 31 23:00:00 EST 2005
· Physics of Atomic Nuclei
·
OSTI ID:20692729
(p,xn), (p,pxn), and (p,2pxn) reactions for medium-mass nuclei at 12 GeV
Journal Article
·
Sat Oct 01 00:00:00 EDT 1983
· Phys. Rev. C; (United States)
·
OSTI ID:5466686
Related Subjects
651726* -- Nuclear Properties & Reactions
A=90-149
Experimental-- Spontaneous & Induced Fission-- (-1987)
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ALKALI METAL ISOTOPES
ALKALINE EARTH ISOTOPES
ANGULAR DISTRIBUTION
BARIUM 131
BARIUM ISOTOPES
BARYON REACTIONS
BARYONS
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CESIUM 129
CESIUM 132
CESIUM 133 TARGET
CESIUM ISOTOPES
CHARGED-PARTICLE REACTIONS
CROSS SECTIONS
DAYS LIVING RADIOISOTOPES
DISTRIBUTION
ELECTRON CAPTURE RADIOISOTOPES
ELEMENTARY PARTICLES
ENERGY RANGE
EVAPORATION MODEL
EVEN-ODD NUCLEI
FERMIONS
HADRON REACTIONS
HADRONS
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
KINETICS
MATHEMATICAL MODELS
MEV RANGE
MEV RANGE 100-1000
MINUTES LIVING RADIOISOTOPES
MONTE CARLO METHOD
NEUTRONS
NUCLEAR CASCADES
NUCLEAR MODELS
NUCLEAR REACTION KINETICS
NUCLEAR REACTIONS
NUCLEI
NUCLEON REACTIONS
NUCLEONS
ODD-EVEN NUCLEI
ODD-ODD NUCLEI
PROTON REACTIONS
PROTONS
RADIOISOTOPES
REACTION KINETICS
RECOILS
SPALLATION
TARGETS
A=90-149
Experimental-- Spontaneous & Induced Fission-- (-1987)
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ALKALI METAL ISOTOPES
ALKALINE EARTH ISOTOPES
ANGULAR DISTRIBUTION
BARIUM 131
BARIUM ISOTOPES
BARYON REACTIONS
BARYONS
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CESIUM 129
CESIUM 132
CESIUM 133 TARGET
CESIUM ISOTOPES
CHARGED-PARTICLE REACTIONS
CROSS SECTIONS
DAYS LIVING RADIOISOTOPES
DISTRIBUTION
ELECTRON CAPTURE RADIOISOTOPES
ELEMENTARY PARTICLES
ENERGY RANGE
EVAPORATION MODEL
EVEN-ODD NUCLEI
FERMIONS
HADRON REACTIONS
HADRONS
INTERMEDIATE MASS NUCLEI
ISOMERIC TRANSITION ISOTOPES
ISOTOPES
KINETICS
MATHEMATICAL MODELS
MEV RANGE
MEV RANGE 100-1000
MINUTES LIVING RADIOISOTOPES
MONTE CARLO METHOD
NEUTRONS
NUCLEAR CASCADES
NUCLEAR MODELS
NUCLEAR REACTION KINETICS
NUCLEAR REACTIONS
NUCLEI
NUCLEON REACTIONS
NUCLEONS
ODD-EVEN NUCLEI
ODD-ODD NUCLEI
PROTON REACTIONS
PROTONS
RADIOISOTOPES
REACTION KINETICS
RECOILS
SPALLATION
TARGETS