Energy dependence of fusion evaporation-residue cross sections in the sup 28 Si+ sup 28 Si reaction
Journal Article
·
· Physical Review, C (Nuclear Physics); (USA)
- Department of Physics, University of Richmond, Richmond, Virginia 23173 (USA)
- Physics Division, Argonne National Laboratory, Argonne, Illinois 60439 (USA)
- Department of Physics, University of Notre Dame, Notre Dame, Indiana 46556 (USA)
- Department of Physics Astronomy, Vanderbilt University, Nashville, Tennessee 37235 (USA)
- Division of Educational Programs, Argonne National Laboratory, Argonne, Illinois 60439 (USA)
- Department of Physics, University of Kansas, Lawrence, Kansas 66045 (USA)
- Laboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 (USA)
Velocity distributions of mass-identified evaporation residues produced in the {sup 28}Si+{sup 28}Si reaction have been measured at bombarding energies of 174, 215, 240, 309, 397, and 452 MeV using time-of-flight techniques. These distributions were used to identify evaporation residues and to separate the complete-fusion and incomplete-fusion components. Angular distributions and total cross sections were extracted at all six bombarding energies. The complete-fusion evaporation-residue cross sections and the deduced critical angular momenta are compared with lower energy data and the predictions of existing models.
- Research Organization:
- Argonne National Laboratory (ANL), Argonne, IL
- DOE Contract Number:
- W-31109-ENG-38
- OSTI ID:
- 6849234
- Journal Information:
- Physical Review, C (Nuclear Physics); (USA), Vol. 41:3; ISSN 0556-2813
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
SILICON 28 REACTIONS
HEAVY ION FUSION REACTIONS
SILICON 28 TARGET
ANGULAR DISTRIBUTION
ATLAS SUPERCONDUCTING LINAC
COMPOUND NUCLEI
CROSS SECTIONS
ENERGY DEPENDENCE
EVAPORATION MODEL
MEV RANGE 100-1000
NICKEL 56
TIME-OF-FLIGHT MASS SPECTROMETERS
ACCELERATORS
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CHARGED-PARTICLE REACTIONS
DAYS LIVING RADIOISOTOPES
DISTRIBUTION
DYNAMIC MASS SPECTROMETERS
ELECTRON CAPTURE RADIOISOTOPES
ENERGY RANGE
EVEN-EVEN NUCLEI
HEAVY ION ACCELERATORS
HEAVY ION REACTIONS
INTERMEDIATE MASS NUCLEI
ISOTOPES
LINEAR ACCELERATORS
MASS SPECTROMETERS
MATHEMATICAL MODELS
MEASURING INSTRUMENTS
MEV RANGE
NICKEL ISOTOPES
NUCLEAR MODELS
NUCLEAR REACTIONS
NUCLEI
RADIOISOTOPES
SPECTROMETERS
TARGETS
TIME-OF-FLIGHT SPECTROMETERS
651420* - Nuclear Properties & Reactions
A=20-38
Experimental
SILICON 28 REACTIONS
HEAVY ION FUSION REACTIONS
SILICON 28 TARGET
ANGULAR DISTRIBUTION
ATLAS SUPERCONDUCTING LINAC
COMPOUND NUCLEI
CROSS SECTIONS
ENERGY DEPENDENCE
EVAPORATION MODEL
MEV RANGE 100-1000
NICKEL 56
TIME-OF-FLIGHT MASS SPECTROMETERS
ACCELERATORS
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CHARGED-PARTICLE REACTIONS
DAYS LIVING RADIOISOTOPES
DISTRIBUTION
DYNAMIC MASS SPECTROMETERS
ELECTRON CAPTURE RADIOISOTOPES
ENERGY RANGE
EVEN-EVEN NUCLEI
HEAVY ION ACCELERATORS
HEAVY ION REACTIONS
INTERMEDIATE MASS NUCLEI
ISOTOPES
LINEAR ACCELERATORS
MASS SPECTROMETERS
MATHEMATICAL MODELS
MEASURING INSTRUMENTS
MEV RANGE
NICKEL ISOTOPES
NUCLEAR MODELS
NUCLEAR REACTIONS
NUCLEI
RADIOISOTOPES
SPECTROMETERS
TARGETS
TIME-OF-FLIGHT SPECTROMETERS
651420* - Nuclear Properties & Reactions
A=20-38
Experimental