TY - JOUR
T1 - Energy levels of [Formula Presented] populated in the [Formula Presented] decay of [Formula Presented]
AU - Ahmad, I.
AU - Chasman, R. R.
AU - Greene, J. P.
AU - Kondev, F. G.
AU - Moore, E. F.
AU - Browne, E.
AU - Porter, C. E.
AU - Felker, L. K.
PY - 2003
Y1 - 2003
N2 - [Formula Presented]-Particle, conversion-electron, and [Formula Presented]-ray singles spectra of [Formula Presented] sources containing few Bq activities were measured with high-resolution semiconductor detectors. [Formula Presented] coincidence and level half-life measurements were also performed. On the basis of these measurements the following single-particle states have been identified in [Formula Presented]: [Formula Presented], 0 keV; [Formula Presented], 227.4 keV; [Formula Presented], 285.4 keV; [Formula Presented], 404.9 keV; [Formula Presented], [Formula Presented]. The measured single-particle energies are in good agreement with energies calculated with a Woods-Saxon single-particle potential. From the measured half-life of the [Formula Presented] level and the [Formula Presented] branching ratio, a [Formula Presented] value of [Formula Presented] has been deduced between the [Formula Presented] and [Formula Presented] bands. The large [Formula Presented] value is an indication of octupole mixing in the [Formula Presented] level.
AB - [Formula Presented]-Particle, conversion-electron, and [Formula Presented]-ray singles spectra of [Formula Presented] sources containing few Bq activities were measured with high-resolution semiconductor detectors. [Formula Presented] coincidence and level half-life measurements were also performed. On the basis of these measurements the following single-particle states have been identified in [Formula Presented]: [Formula Presented], 0 keV; [Formula Presented], 227.4 keV; [Formula Presented], 285.4 keV; [Formula Presented], 404.9 keV; [Formula Presented], [Formula Presented]. The measured single-particle energies are in good agreement with energies calculated with a Woods-Saxon single-particle potential. From the measured half-life of the [Formula Presented] level and the [Formula Presented] branching ratio, a [Formula Presented] value of [Formula Presented] has been deduced between the [Formula Presented] and [Formula Presented] bands. The large [Formula Presented] value is an indication of octupole mixing in the [Formula Presented] level.
UR - http://www.scopus.com/inward/record.url?scp=85035252395&partnerID=8YFLogxK
U2 - 10.1103/PhysRevC.68.044306
DO - 10.1103/PhysRevC.68.044306
M3 - Article
AN - SCOPUS:85035252395
SN - 0556-2813
VL - 68
SP - 8
JO - Physical Review C - Nuclear Physics
JF - Physical Review C - Nuclear Physics
IS - 4
ER -