Cultural advice

The Australian National University acknowledges, celebrates and pays our respects to the Ngunnawal and Ngambri people of the Canberra region and to all First Nations Australians on whose traditional lands we meet and work, and whose cultures are among the oldest continuing cultures in human history.

Aboriginal and Torres Strait Islander peoples are advised that ANU Library collections may include images, names, voices, and other representations of deceased persons.

Material in the collection may contain terms, language or views that reflect the period in which the item was created and may be considered inappropriate today.

High-spin states in <sup>183</sup>Hg and shape coexistence in the odd-mass mercury isotopes

Loading...
Thumbnail Image

Authors

Lane, G. J.
Dracoulis, G. D.
Byrne, A. P.
Anderssen, S. S.
Davidson, P. M.
Fabricius, B.
Kibédi, T.
Stuchbery, A. E.
Baxter, A. M.

Journal Title

Journal ISSN

Volume Title

Publisher

Access Statement

Research Projects

Organizational Units

Journal Issue

Abstract

High-spin states in 183Hg have been identified using the reaction 155Gd(32S,4n). Three prolate-deformed rotational bands associated with the 1 2-[521], 7 2-[514] and mixed i 13 2 neutron orbitals are observed, while the existence of an oblate 13 2+ bandhead is inferred, implying co-existing prolate and oblate nuclear shapes. A two-band mixing model used to fit the state energies of the i 13 2 neutron bands in 183,185,187Hg gives parameter values which are consistent with the existence of two bands with different deformations. The B(E2) ratios of the intra- and inter-band transitions in these coexisting bands are also investigated. Many of the features can be reproduced but difficulties remain, for example the results are not consistent with the assumption of coexistence between simple prolate and oblate shapes, a problem noted previously for the even-mass isotopes. Systematics of the prolate-oblate energy differences show that the energy of the prolate well relative to the oblate well is ∼ 350 keV lower in the odd-mass isotopes than in the even-mass isotopes. Possible reasons for this are described. The nature of the first alignment in the prolate bands in the mercury isotopes is discussed within the cranked shell model.

Description

Keywords

Citation

Source

Nuclear Physics, Section A

Book Title

Entity type

Publication

Access Statement

License Rights

Restricted until