Abstract The Holifield Radioactive Ion Beam Facility (HRIBF) provides high-quality Isotope
Separator Online beams of short-lived, radioactive nuclei for nuclear structure and reaction …

The present review takes steps from the domain of the shell model into open shell nuclei.
The question posed in the title is to dramatize how far shell model approaches, ie, many …

The 2 2+ state in 132 Te is identified as the one-phonon mixed-symmetry state in a projectile
Coulomb excitation experiment presenting a firm example of a mixed-symmetry state in …

A collective S and D nucleon pair approximation of the shell model is applied to even-even
Sn, Te, Xe, Ba, and Ce isotopes with mass number A~ 120–150 and neutron number …

Radioactive Te 136 has two valence protons and two valence neutrons outside of the Sn
132 double shell closure, providing a simple laboratory for exploring the emergence of …

We present results from large-scale shell model calculations of even and odd tin isotopes
from Sn 134 to Sn 142 with a shell model space defined by the 1 f 7/2, 2 p 3/2, 0 h 9/2, 2 p …

The g factor and B (E 2) of the first excited 2+ state have been measured following Coulomb
excitation of the neutron-rich semimagic nuclide 134 Te (two protons outside 132 Sn) …

Magnetic moments have in general provided substantial information on the microscopic
structure of nuclear states. Advances in technology have made it possible to measure, with …

In the light of new g factor results for the stable isotopes between Te 122 and Te 130, the
calibration and modeling of the recoil-in-vacuum (RIV) interaction for Te ions is reexamined …

Background: The g factors and lifetimes of the 2 1+ states in the stable, proton-rich Sn
isotopes have been measured, but there is scant information on neutron-rich Sn isotopes …