Decay of /sup 149/Er/sup g//sup +//sup m/ by positron and delayed proton emission and by electron capture
In this study the decay of /sup 149/Er/sup g//sup +//sup m/ by positron emission, electron capture, and ..beta..-delayed proton emission was investigated. Gamma rays associated with /sup 149/Er/sup m/ decay were placed in a decay scheme on the basis of ..gamma gamma.. and x..gamma.. coincidences and half-life. We assigned 120 ..gamma.. rays deexciting 91 levels in /sup 149/Ho to 8.9 +- 0.2 s /sup 149/Er/sup m/ decay. The ..pi..s/sub 1/2/ single-particle state in /sup 149/Ho was observed to occur at 49.0 keV above the ..pi..h/sub 11/2/ ground state. A (3.5 +- 0.7) % isomeric transition decay branch and a (0.18 +- 0.07) % ..beta..-delayed proton decay branch were determined for /sup 149/Er/sup m/ decay. Three additional ..gamma.. rays were assigned to 4 +- 2 s /sup 149/Er/sup g/ decay and a (7 +- 2) % ..beta..-delayed proton decay branch was determined. Measured EC/..beta../sup +/ ratios to proton emitting states in /sup 149/Ho resulted in a (Q/sub E//sub C/-S/sub p/) = 7.0/sup +5.0//sub -0.4/ MeV for /sup 149/ER/sup 8/ decay and a S/sub p/ = 1.4/sup +10//sub -0.6/ MeV for Ho. The ..beta..-delayed proton spectrum from /sup 149/Er/sup g/ consisted of a highly structured component corresponding to the deexcitation of levels between 4 and 5 MeV in /sup 149/Ho and a structureless component corresponding to decay from higher levels. The ..beta..-strength function for /sup 149/Er/sup g//sup +//sup m/ decay is discussed in terms of single-particle shell-model structure, weak coupling to the /sup 148/Dy core, and decay of ..pi..h/sub 11/2/ protons across the shell closure to the ..nu..h/sub 9/2/ neutron orbital.
- Research Organization:
- Lawrence Berkeley Laboratory, University of California, Berkeley, California 94720
- OSTI ID:
- 6535540
- Journal Information:
- Phys. Rev. C; (United States), Vol. 39:1
- Country of Publication:
- United States
- Language:
- English
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651720* - Nuclear Properties & Reactions
A=90-149
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