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Kanungo, R.*; Nociforo, C.*; Prochazka, A.*; Utsuno, Yutaka; Aumann, T.*; Boutin, D.*; Cortina-Gil, D.*; Davids, B.*; Diakaki, M.*; Farinon, F.*; et al.
Physics Letters B, 685(4-5), p.253 - 257, 2010/05
Times Cited Count:35 Percentile:87.73(Astronomy & Astrophysics)no abstracts in English
Qian, J.*; Heinz, A.*; Khoo, T. L.*; Janssens, R. V. F.*; Peterson, D.*; Seweryniak, D.*; Ahmad, I.*; Asai, Masato; Back, B. B.*; Carpenter, M. P.*; et al.
Physical Review C, 79(6), p.064319_1 - 064319_13, 2009/06
Times Cited Count:30 Percentile:83.94(Physics, Nuclear)-,
-, and conversion electron spectroscopy experiments for
Rf have been performed using Fragment Mass Analyzer at Argonne National Laboratory. A new isomer with a half-life of 160
s has been discovered in
Rf, and it is interpreted as a three-quasiparticle high-
isomer. Neutron configurations of one-quasiparticle states in
No, the
-decay daughter of
Rf, have been assigned on the basis of
-decay hindrance factors. Excitation energies of the 1/2
[620] states in
=151 isotones indicate that the deformed shell gap at
=152 increases with the atomic number.
Kanungo, R.*; Nociforo, C.*; Prochazka, A.*; Aumann, T.*; Boutin, D.*; Cortina-Gil, D.*; Davids, B.*; Diakaki, M.*; Farinon, F.*; Geissel, H.*; et al.
Physical Review Letters, 102(15), p.152501_1 - 152501_4, 2009/04
Times Cited Count:153 Percentile:96.74(Physics, Multidisciplinary)no abstracts in English
Doornenbal, P.*; Reiter, P.*; Grawe, H.*; Otsuka, Takaharu*; Al-Khatib, A.*; Banu, A.*; Beck, T.*; Becker, F.*; Bednarczyk, P.*; Benzoni, G.*; et al.
Physics Letters B, 647(4), p.237 - 242, 2007/04
Times Cited Count:30 Percentile:85.71(Astronomy & Astrophysics)The first excited state of Ca was measured at GSI for the first time. The measured
energy is found to be 3015(16) keV, which is lower than its mirror nucleus
S by as large as 276 keV. The structure of those nuclei is studied by the shell model. It is found that those nuclei can be well described by the
valence space. The large energy shift between them is caused by the Thomas-Ehrman effect. We presented that the energy shift in the
shell region can be explained by the shell model with a phenomenological treatment of the Thomas-Ehrman effect.