z-logo
open-access-imgOpen Access
Triple configuration coexistence inS44
Author(s) -
D. Santiago-Gonzalez,
I. Wiedenhöver,
Volha Abramkina,
M. L. Avila,
T. Baugher,
D. Bazin,
B. A. Brown,
P. D. Cottle,
A. Gade,
T. Glasmacher,
K. W. Kemper,
S. McDaniel,
A. Rojas,
A. Ratkiewicz,
R. Meharchand,
E. C. Simpson,
J. A. Tostevin,
Alexander Volya,
D. Weißhaar
Publication year - 2011
Publication title -
physical review c
Language(s) - English
Resource type - Journals
eISSN - 1089-490X
pISSN - 0556-2813
DOI - 10.1103/physrevc.83.061305
Subject(s) - excited state , physics , neutron , proton , atomic physics , energy (signal processing) , ground state , deformation (meteorology) , nuclear physics , quantum mechanics , meteorology
The neutron-rich $N=28$ nucleus $^{44}\mathrm{S}$ was studied using the two-proton knockout reaction from $^{46}\mathrm{Ar}$ at intermediate beam energy. We report the observation of four new excited states, one of which is a strongly prolate deformed 4${}^{+}$ state, as indicated by a shell-model calculation. Its deformation originates in a neutron configuration which is fundamentally different from the ``intruder'' configuration responsible for the ground-state deformation. Consequently, we do not have three coexisting shapes in $^{44}\mathrm{S}$, but three coexisting configurations, corresponding to zero-, one-, and two-neutron particle-hole excitations.

The content you want is available to Zendy users.

Already have an account? Click here to sign in.
Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom