Structure of {sup 26}Na from the {sup 14}C({sup 14}C, d) reaction

The {sup 14}C({sup 14}C, d) reaction at 22 MeV was used to study T{sub z}=2 {sup 26}Na. Charged particles were detected with a Si detector telescope at 0 deg., and {gamma} transitions in coincidence were detected with an array of three Compton-suppressed 'clover' detectors and seven Compto...

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Bibliographic Details
Published in:Physical review. C, Nuclear physics Nuclear physics, 2006-04, Vol.73 (4)
Main Authors: Lee, Sangjin, Tabor, S.L., Baldwin, T., Campbell, D.B., Calderin, I., Chandler, C., Cooper, M.W., Hoffman, C.R., Kemper, K.W., Pavan, J., Pipidis, A., Riley, M.A., Wiedeking, M.
Format: Article
Language:English
Subjects:
ANGULAR DISTRIBUTION
BETA DECAY
CARBON 14
CARBON 14 REACTIONS
CARBON 14 TARGET
CHARGE-EXCHANGE REACTIONS
COINCIDENCE SPECTROMETRY
DEUTERONS
GAMMA DECAY
MEV RANGE
MIXING RATIO
NUCLEAR PHYSICS AND RADIATION PHYSICS
NUCLEAR STRUCTURE
SI SEMICONDUCTOR DETECTORS
SODIUM 26
TELESCOPE COUNTERS
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Summary:The {sup 14}C({sup 14}C, d) reaction at 22 MeV was used to study T{sub z}=2 {sup 26}Na. Charged particles were detected with a Si detector telescope at 0 deg., and {gamma} transitions in coincidence were detected with an array of three Compton-suppressed 'clover' detectors and seven Compton-suppressed single Ge crystals. The Deuteron-{gamma} and d-{gamma}-{gamma} coincidence data were analyzed to study the structure of {sup 26}Na. New levels were found, and precise energies and {gamma}-decay patterns were determined for many states previously observed in charge-exchange reactions. Candidates were observed for the 1{sup +} state missing in {beta} decay. Mixing ratios were determined for some {gamma} transitions from angular distribution information. There is reasonable agreement with the model based on the universal s-d shell (USD) interaction.
ISSN:0556-2813
1089-490X
DOI:10.1103/PhysRevC.73.044321