2001
DOI: 10.1007/0-306-47915-x_3
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High Spin Properties of Atomic Nuclei

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Cited by 15 publications
(23 citation statements)
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“…Furthermore the gaps do not exist for all isotopes. On the neutron side, S 2n show distinguishable gaps at N =138, 172,184,198,228,238,252,258, and 274 with all the effective interactions. Apart from these, there are also other gaps which appear only for some effective interactions, e.g., N = 164 for NLSH, TW99, DD-ME1, PK1 and PK1R, and N = 216 for NLSH, TW99, PK1, and PK1R.…”
Section: Two Nucleon Separation Energiesmentioning
confidence: 97%
“…Furthermore the gaps do not exist for all isotopes. On the neutron side, S 2n show distinguishable gaps at N =138, 172,184,198,228,238,252,258, and 274 with all the effective interactions. Apart from these, there are also other gaps which appear only for some effective interactions, e.g., N = 164 for NLSH, TW99, DD-ME1, PK1 and PK1R, and N = 216 for NLSH, TW99, PK1, and PK1R.…”
Section: Two Nucleon Separation Energiesmentioning
confidence: 97%
“…At present superdeformed bands have been observed in various atomic mass regions [5]. The most notable regions are at A ∼ 130, 150, and 190 in which axis ratios are, respectively, close to 1.5:1, 2:1, and 1.7:1 [6].…”
Section: Introductionmentioning
confidence: 90%
“…High-spin states in nuclei show a rich variety of phenomena as, e.g., deformation alignment, back-bending, pairing breakdown, Coriolis anti-pairing, having thus attracted much attention in the past, for reviews see [1][2][3]. High-spin states in the doubly magic 208 Pb are special in that the large proton and neutron shell gaps inhibit deformation and pairing.…”
Section: Introductionmentioning
confidence: 99%