2009
DOI: 10.1016/j.nds.2009.06.002
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Nuclear Data Sheets for A = 102

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Cited by 128 publications
(94 citation statements)
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“…In all even-nuclei examined here, K was taken as zero, whereas for the odd nuclei the bandhead value of K was used. Since it is usually difficult to determine the centroid energy of the Doppler-broadened lineshapes to a level of accuracy comparable to experiments that produce narrow lineshapes, we have consistently used the evaluated γ-ray energies [26][27][28][29][30][31][32][33][34][35][36][37][38][39][40][41] in our fits and calculations of the state lifetimes.…”
Section: Experimental Details and Analysis Techniquesmentioning
confidence: 99%
“…In all even-nuclei examined here, K was taken as zero, whereas for the odd nuclei the bandhead value of K was used. Since it is usually difficult to determine the centroid energy of the Doppler-broadened lineshapes to a level of accuracy comparable to experiments that produce narrow lineshapes, we have consistently used the evaluated γ-ray energies [26][27][28][29][30][31][32][33][34][35][36][37][38][39][40][41] in our fits and calculations of the state lifetimes.…”
Section: Experimental Details and Analysis Techniquesmentioning
confidence: 99%
“…Finally, the contribution in the feeding of some low-energy transitions that were not observed in the spectra due to internal conversion was approximated by the inclusion of transitions that feed the corresponding emitting levels. For instance, the 13.7-keV transition that is emitted from the 154-keV level of 102 Rh [3] to the isomer in Fig. 1.b was not observed and its contribution was estimated from the 205.1-, 223.6-, and 528.4-keV transitions, and also, the 32.46-keV transition emitted from the 126-keV level of 107 Ag [10] in Fig.…”
Section: Resultsmentioning
confidence: 94%
“…1.b which feed ground state and isomer, respectively. The cross section of the former can be estimated from the experimentally obtained cross section for the 51.27-keV transition emitted from the same level of 102 Rh and using the known relative intensities of the two transitions [3]. Thus, the cross section for the 156.6-keV transition can then be deduced by subtraction from the total cross section obtained for the double peak in the spectra.…”
Section: Resultsmentioning
confidence: 99%
“…A shape change to large deformation is also evident in the band structure of the odd-mass Pd isotopes [41][42][43][44][45][46][47][48] (Fig. 5) and suggested by B(E2) systematics [21,[55][56][57][58][59]. Yet, Stefanova et al [48] have recently suggested a transition to γ-softness beyond N =61 which may be maximal at 109 Pd 63 and 111 Pd 65 .…”
mentioning
confidence: 76%