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AbstractAbstract
[en] The nuclear states in 23F have been investigated following the β decay of 23O. The measurement of 23O was carried out at the National Superconducting Cyclotron Laboratory using fragments from the reaction of a 48Ca beam in a Be target. The half-life and total neutron emission probability were determined to be 97(8) ms and 7(2)%, respectively, for 23O β decay. Ten γ-ray decays in 23F and a single γ-ray in 22F were observed to establish the β decay scheme for 23O. Shell model calculations are in reasonable agreement with the measured β branching and B(GT) values for the lowest energy state. The excitation energies of the first 1/2+ and 3/2+ states have been determined to be 2243(8) and 4066(16) keV, respectively, indicating a widening of the 5/2+-1/2+ state gap in 23F. The decay scheme of the largest contaminant 26Ne in the experiment was established
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(c) 2007 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA)
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Journal Article
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ACCELERATORS, ALKALINE EARTH ISOTOPES, BETA DECAY RADIOISOTOPES, BETA-MINUS DECAY RADIOISOTOPES, CALCIUM ISOTOPES, CYCLIC ACCELERATORS, CYCLOTRONS, DECAY, DIMENSIONLESS NUMBERS, ELECTROMAGNETIC RADIATION, EMISSION, ENERGY RANGE, ENERGY-LEVEL TRANSITIONS, EVEN-EVEN NUCLEI, EVEN-ODD NUCLEI, FLUORINE ISOTOPES, INTERMEDIATE MASS NUCLEI, IONIZING RADIATIONS, ISOTOPES, LIGHT NUCLEI, MATHEMATICAL MODELS, MILLISECONDS LIVING RADIOISOTOPES, NEON ISOTOPES, NUCLEAR DECAY, NUCLEAR MODELS, NUCLEI, ODD-EVEN NUCLEI, ODD-ODD NUCLEI, OXYGEN ISOTOPES, RADIATIONS, RADIOISOTOPES, SECONDS LIVING RADIOISOTOPES, STABLE ISOTOPES
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