z-logo
open-access-imgOpen Access
New measurement and reevaluation of the nuclear magnetic andquadrupole moments ofLi8andLi
Author(s) -
D. Borremans,
D. L. Balabanski,
K. Blaum,
W. Geithner,
S. Gheysen,
P. Himpe,
M. Kowalska,
J. Lassen,
Peter Lievens,
S. Mallion,
R. Neugart,
G. Neyens,
N. Vermeulen,
D. T. Yordanov
Publication year - 2005
Publication title -
physical review c
Language(s) - English
Resource type - Journals
eISSN - 1089-490X
pISSN - 0556-2813
DOI - 10.1103/physrevc.72.044309
Subject(s) - quadrupole , physics , magnetic moment , atomic physics , nuclear magnetic resonance , condensed matter physics
The nuclear magnetic moment of $^{9}$Li and the quadrupole moments of $^{8}$Li and $^{9}$Li have been measured using $\beta$-asymmetry detection of nuclear magnetic resonance ($\beta$-NMR) on optically polarized beams at ISOLDE/CERN. The radioactive beams were implanted in Si for g factor measurements and in Zn, LiNbO$_{3}$, and LiTaO$_{3}$ crystals for quadrupole moment measurements. The electric field gradient V$_{zz}$ = 4.26(4) $\times$10$^{15}$ V/cm$^{2}$ is deduced for Li in Zn. Using a recently adopted reference value Q($^{7}$Li) = -40.0(3) mb, we reevaluated all earlier reported nuclear quadrupole moments of $^{8}$Li and $^{9}$Li. Based on all available previous and present data, the adopted quadrupole moments for these isotopes are Q($^{8}$Li) = +31.4(2) mb and Q($^{9}$Li) = - 30.6(2) mb. The magnetic moment of $^{9}$Li is deduced as $\mu(^{9}$Li) = 3.43678(6)$\mu\scriptstyle_\textrm{N}$ . The values are compared to predictions from shell-model and cluster-model calculations

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