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Summary of Bases for Spin and Parity Assignments


Publisher
Elsevier Science
Year
2011
Tongue
English
Weight
76 KB
Volume
112
Category
Article
ISSN
0090-3752

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✦ Synopsis


Ground States

  1. The ground state of an even-even nucleus has JS = 0 + . 2. Spin determinations by such techniques as atomic-beam resonance, paramagnetic resonance, electron-spin resonance, and optical spectroscopy give correct values. * 'IV' and 'IS' stand for isovector and isoscalar † *J/*w(Upper Limit)=30 for A=90150 # *J/*w(Upper Limit)=0.1 for A=2144 Β§ *J/*w(Upper Limit)=0.003 for E1 (IS), 10 for E2 (IV), 0.03 for M1 (IS), 0.1 for M2 (IS) a From 1979En05 b From 1979En04 c From 1981En06 d Deduced from ENSDF by M. J. Martin e In super-deformed bands the E2 transitions can have *J/*w>1000.

πŸ“œ SIMILAR VOLUMES


Summary of Bases for Spin and Parity Ass
πŸ“‚ Article πŸ“… 2010 πŸ› Elsevier Science 🌐 English βš– 95 KB

## Ground States 1. The ground state of an even-even nucleus has J = 0 + . 2. Spin determinations by such techniques as atomic-beam resonance, paramagnetic resonance, electron-spin resonance, and optical spectroscopy give correct values.

Summary of bases for spin and parity ass
πŸ“‚ Article πŸ“… 1969 πŸ› Elsevier Science βš– 278 KB

This issue marks the further extension of the Nuclear Data Sheets to include the heavy elements. Nuclear Data Sheets for 213 < A < 228 were published in 1966 (Nuclear Data B1-5); a third compilation for 229 < A < 242 is in \_preParation. I Final corrections to this issue have been made by members of

Summary of bases for spin and parity ass
πŸ“‚ Article πŸ“… 1970 πŸ› Elsevier Science βš– 149 KB

## Ground States 1, The ground state of an even-even nucleus has j~=o +. 2. Spin determinations by such techniques as atomic-beam resonance, paramagnetic resonance, electron-spin resonance, and optical spectroscopy give correct values.

Summary of bases for spin and parity ass
πŸ“‚ Article πŸ“… 1975 πŸ› Elsevier Science 🌐 English βš– 142 KB

## Ground States 1. The ground state of an even-even nucleus has J~ = 0 +. 2. Spin determinations by such techniques as atomic-beam resonance, paramagnetic resonance, electron-spin resonance, and optical spectroscopy give correct values.