Rotational Bands in the Doubly Magic Nucleus N[number sign]56i
Journal Article
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· Physical Review Letters
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- Department of Physics, Lund University, S-22100 Lund (Sweden)
- Physics Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831 (United States)
- Institut de Recherches Subatomiques, CNRS-IN2P3 et Universite Louis Pasteur, F-67037 Strasbourg (France)
- Chemistry Department, Washington University, St. Louis, Missouri 63130 (United States)
- Institute of Theoretical Physics, Warsaw University, PL-00681 Warsaw (Poland)
- Department of Physics, University of Tennessee, Knoxville, Tennessee 37996 (United States)
- Joint Institute for Heavy Ion Research, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831 (United States)
- Service de Physique Nucleaire Th
Structures of the medium- to high-spin states in the doubly magic nucleus [sup 56]Ni have been investigated using the reaction [sup 28]Si([sup 36]Ar,thinsp2[alpha]) and the [gamma] -ray spectrometer Gammasphere in conjunction with the 4[pi] charged-particle detector array Microball. Two well-deformed rotational bands have been identified. There is evidence that one of the bands, which is identical to a sequence in the odd-odd neighbor [sup 58]Cu , partially decays via proton emission into the ground state of [sup 55]Co . Predictions of extensive large-scale shell-model and cranked Hartree-Fock and Hartree-Fock-Bogolyubov calculations are compared with the experimental data. [copyright] [ital 1999] [ital The American Physical Society]
- DOE Contract Number:
- AC05-96OR22464; FG02-96ER40963; FG05-87ER40361; FG02-88ER40406
- OSTI ID:
- 6326268
- Journal Information:
- Physical Review Letters, Journal Name: Physical Review Letters Vol. 82:19; ISSN 0031-9007; ISSN PRLTAO
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
663110* -- General & Average Properties of Nuclei & Nuclear Energy Levels-- (1992-)
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ALPHA PARTICLES
ARGON
ARGON 36
ARGON ISOTOPES
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CALCULATION METHODS
CHARGED PARTICLES
COBALT
COBALT 55
COBALT ISOTOPES
COPPER
COPPER 58
COPPER ISOTOPES
DAYS LIVING RADIOISOTOPES
ELECTRON CAPTURE RADIOISOTOPES
ELEMENTS
ENERGY LEVELS
EVEN-EVEN NUCLEI
EXCITED STATES
FLUIDS
GAMMA SPECTRA
GASES
HARTREE-FOCK METHOD
HIGH SPIN STATES
HOURS LIVING RADIOISOTOPES
INTERMEDIATE MASS NUCLEI
ISOTOPES
LIGHT NUCLEI
MATHEMATICAL MODELS
METALS
NICKEL 56
NICKEL ISOTOPES
NONMETALS
NUCLEAR MODELS
NUCLEI
ODD-EVEN NUCLEI
ODD-ODD NUCLEI
RADIOISOTOPES
RARE GASES
ROTATIONAL STATES
SECONDS LIVING RADIOISOTOPES
SEMIMETALS
SHELL MODELS
SILICON
SILICON 28 TARGET
SPECTRA
STABLE ISOTOPES
TARGETS
TRANSITION ELEMENTS
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
ALPHA PARTICLES
ARGON
ARGON 36
ARGON ISOTOPES
BETA DECAY RADIOISOTOPES
BETA-PLUS DECAY RADIOISOTOPES
CALCULATION METHODS
CHARGED PARTICLES
COBALT
COBALT 55
COBALT ISOTOPES
COPPER
COPPER 58
COPPER ISOTOPES
DAYS LIVING RADIOISOTOPES
ELECTRON CAPTURE RADIOISOTOPES
ELEMENTS
ENERGY LEVELS
EVEN-EVEN NUCLEI
EXCITED STATES
FLUIDS
GAMMA SPECTRA
GASES
HARTREE-FOCK METHOD
HIGH SPIN STATES
HOURS LIVING RADIOISOTOPES
INTERMEDIATE MASS NUCLEI
ISOTOPES
LIGHT NUCLEI
MATHEMATICAL MODELS
METALS
NICKEL 56
NICKEL ISOTOPES
NONMETALS
NUCLEAR MODELS
NUCLEI
ODD-EVEN NUCLEI
ODD-ODD NUCLEI
RADIOISOTOPES
RARE GASES
ROTATIONAL STATES
SECONDS LIVING RADIOISOTOPES
SEMIMETALS
SHELL MODELS
SILICON
SILICON 28 TARGET
SPECTRA
STABLE ISOTOPES
TARGETS
TRANSITION ELEMENTS