1988
DOI: 10.1016/0370-2693(88)91402-5
|View full text |Cite
|
Sign up to set email alerts
|

Evidence for shape coexistence in odd-mass rhodium nuclei

Abstract: Results from the study of the '@'Ru ('He, d) "'Rh reaction reveal evidence for shape coexistence in odd-mass rhodium isotopes. The strongly excited states at 786, 806, 969, 1019 and 1355 keV in "'Rh are good candidates for a rotational-like positive-parity band with J"= l/2+, 3/2+, 5/2+, 7/2+ and 9/2+, respectively, coexisting with spherical shell-model states like lg,,,, 2p,,,, 2p,,, and lfsjz as well as core-coupled configurations.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
4
0

Year Published

1990
1990
2022
2022

Publication Types

Select...
5
4

Relationship

1
8

Authors

Journals

citations
Cited by 16 publications
(5 citation statements)
references
References 11 publications
1
4
0
Order By: Relevance
“…and B(E2; 7/2 + → 3/2 + )=136(5) W.u. confirm the enhanced collectivity indicated by previous measurements [57,59,60], lending support to the large deformations suggested in prior studies of the nearby isotopes [44,45,54,58]. These B(E2) values are among the largest in the region [79], comparable to those observed in the strongly-deformed bands found in the Z≤42 isotopes [22,28,29,31,37,38].…”
Section: Resultssupporting
confidence: 90%
See 1 more Smart Citation
“…and B(E2; 7/2 + → 3/2 + )=136(5) W.u. confirm the enhanced collectivity indicated by previous measurements [57,59,60], lending support to the large deformations suggested in prior studies of the nearby isotopes [44,45,54,58]. These B(E2) values are among the largest in the region [79], comparable to those observed in the strongly-deformed bands found in the Z≤42 isotopes [22,28,29,31,37,38].…”
Section: Resultssupporting
confidence: 90%
“…However, such an idea about the occurrence of triaxiality and its role in shape-coexisting mass regions may not be complete, especially considering past measurements of shape coexistence in the Z>42 region, particularly in odd-mass isotopes, combined now with the recent experimental and theoretical works mentioned above pertaining to the isotopes at lower Z. Despite the apparent regularity of triaxiality above Mo, shape coexistence does remain an important feature in the low energy structure of Tc [53][54][55][56], Rh [44,[57][58][59], Ag [60], In [61,62] and to a lesser extent, the even-even isotopes of Ru [63,64], Pd [65], and Cd [66]. As discussed by Heyde and Wood [11], many have attributed this, perhaps erroneously, to specific, deformation-driving single-particle orbitals crossing the Z=50 shell gap, so-called intruder orbitals.…”
Section: Introductionmentioning
confidence: 99%
“…Guided by the observation of the 2p − 2h and 2p − 4h intruder states in the Sn and Cd isotopes, respectively, and the presence of deformed bands in the odd-A Ag and Rh isotopes (see, e.g., Refs. [411][412][413][414][415]), suggestions were made that such structures appear in the Pd isotopes as well [416][417][418]. Recent studies [419] of 106 Pd using the (n, n γ) reaction have measured a large number of level lifetimes and significantly expanded the level scheme.…”
Section: Pd Isotopesmentioning
confidence: 99%
“…In[23], 47 Ag[23,24], 45 Rh[25,26,27,28], and 43 Tc[29] isotopes, but not for 41 Nb isotopes. It is well known, from previous studies of the in-…”
mentioning
confidence: 99%