Shape coexistence and isomeric states in neutron-rich {sup 112}Tc and {sup 113}Tc
Journal Article
·
· Physical Review. C, Nuclear Physics
- School of Computing, Engineering and Mathematics, University of Brighton, Brighton BN2 4GJ (United Kingdom)
- Gesellschaft fuer Schwerionenforschung mbH, Planckstrasse 1, D-64291 Darmstadt (Germany)
- Department of Physics, University of Surrey, Guildford GU2 7XH (United Kingdom)
Isomeric states in {sup 112}Tc and {sup 113}Tc, with half-lives of 150(17) ns and 500(100) ns, respectively, have been observed following the relativistic fission of {sup 238}U. The fission fragments have been separated in a fragment separator and identified by means of energy-loss and time-of-flight techniques. In both nuclei, the ground-state configuration is calculated to have an oblate shape and the isomerism is proposed to arise due to transitions from a triaxial excited state to a low-lying oblate state.
- OSTI ID:
- 21419604
- Journal Information:
- Physical Review. C, Nuclear Physics, Journal Name: Physical Review. C, Nuclear Physics Journal Issue: 4 Vol. 82; ISSN 0556-2813; ISSN PRVCAN
- Country of Publication:
- United States
- Language:
- English
Similar Records
First observation of isomeric states in 111Zr, 113Nb, and 115Mo
Decays of very neutron-rich fission products {sup 113}Ru and {sup 113}Rh
Half-life measurements for neutron-rich Tc, Ru, Rh, and Pd isotopes. Identification of the new isotopes /sup 111/Tc, /sup 113/Ru, and /sup 113/Rh
Journal Article
·
Sun Dec 25 19:00:00 EST 2022
· Physical Review. C
·
OSTI ID:1907837
Decays of very neutron-rich fission products {sup 113}Ru and {sup 113}Rh
Journal Article
·
Sun Dec 20 23:00:00 EST 1998
· AIP Conference Proceedings
·
OSTI ID:21207866
Half-life measurements for neutron-rich Tc, Ru, Rh, and Pd isotopes. Identification of the new isotopes /sup 111/Tc, /sup 113/Ru, and /sup 113/Rh
Journal Article
·
Mon Aug 01 00:00:00 EDT 1988
· Phys. Rev. C; (United States)
·
OSTI ID:6967911
Related Subjects
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ACTINIDE NUCLEI
ALPHA DECAY RADIOISOTOPES
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
CONFIGURATION
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY LOSSES
ENERGY RANGE
EVEN-EVEN NUCLEI
EXCITED STATES
FERMIONS
FISSION
FISSION FRAGMENTS
GROUND STATES
HADRONS
HALF-LIFE
HEAVY NUCLEI
INTERMEDIATE MASS NUCLEI
ISOTOPES
LOSSES
MILLISECONDS LIVING RADIOISOTOPES
NEUTRON-RICH ISOTOPES
NEUTRONS
NUCLEAR FRAGMENTS
NUCLEAR REACTIONS
NUCLEI
NUCLEONS
ODD-EVEN NUCLEI
ODD-ODD NUCLEI
RADIOISOTOPES
RELATIVISTIC RANGE
SPONTANEOUS FISSION RADIOISOTOPES
TECHNETIUM 112
TECHNETIUM 113
TECHNETIUM ISOTOPES
TIME-OF-FLIGHT METHOD
URANIUM 238
URANIUM ISOTOPES
YEARS LIVING RADIOISOTOPES
ACTINIDE NUCLEI
ALPHA DECAY RADIOISOTOPES
BARYONS
BETA DECAY RADIOISOTOPES
BETA-MINUS DECAY RADIOISOTOPES
CONFIGURATION
ELEMENTARY PARTICLES
ENERGY LEVELS
ENERGY LOSSES
ENERGY RANGE
EVEN-EVEN NUCLEI
EXCITED STATES
FERMIONS
FISSION
FISSION FRAGMENTS
GROUND STATES
HADRONS
HALF-LIFE
HEAVY NUCLEI
INTERMEDIATE MASS NUCLEI
ISOTOPES
LOSSES
MILLISECONDS LIVING RADIOISOTOPES
NEUTRON-RICH ISOTOPES
NEUTRONS
NUCLEAR FRAGMENTS
NUCLEAR REACTIONS
NUCLEI
NUCLEONS
ODD-EVEN NUCLEI
ODD-ODD NUCLEI
RADIOISOTOPES
RELATIVISTIC RANGE
SPONTANEOUS FISSION RADIOISOTOPES
TECHNETIUM 112
TECHNETIUM 113
TECHNETIUM ISOTOPES
TIME-OF-FLIGHT METHOD
URANIUM 238
URANIUM ISOTOPES
YEARS LIVING RADIOISOTOPES