Quadrupole Moments of Neutron-Deficient $^{20, 21}$Na
| dc.creator | Minamisono, K. | |
| dc.creator | Matsuta, K. | |
| dc.creator | Minamisono, T. | |
| dc.creator | Levy, C. D. P. | |
| dc.creator | Nagatomo, T. | |
| dc.creator | Ogura, M. | |
| dc.creator | Sumikama, T. | |
| dc.creator | Behr, J. A. | |
| dc.creator | Jackson, K. P. | |
| dc.creator | Mihara, M. | |
| dc.creator | Fukuda, M. | |
| dc.date | 2009-01-08 | |
| dc.date.accessioned | 2026-07-07T13:02:18Z | |
| dc.date.available | 2026-07-07T13:02:18Z | |
| dc.description | The electric-quadrupole coupling constant of the ground states of the proton drip line nucleus $^{20}$Na($I^π$ = 2$^{+}$, $T_{1/2}$ = 447.9 ms) and the neutron-deficient nucleus $^{21}$Na($I^π$ = 3/2$^{+}$, $T_{1/2}$ = 22.49 s) in a hexagonal ZnO single crystal were precisely measured to be $|eqQ/h| = 690 \pm 12$ kHz and 939 $\pm$ 14 kHz, respectively, using the multi-frequency $β$-ray detecting nuclear magnetic resonance technique under presence of an electric-quadrupole interaction. A electric-quadrupole coupling constant of $^{27}$Na in the ZnO crystal was also measured to be $|eqQ/h| = 48.4 \pm 3.8$ kHz. The electric-quadrupole moments were extracted as $|Q(^{20}$Na)$|$ = 10.3 $\pm$ 0.8 $e$ fm$^2$ and $|Q(^{21}$Na)$|$ = 14.0 $\pm$ 1.1 $e$ fm$^2$, using the electric-coupling constant of $^{27}$Na and the known quadrupole moment of this nucleus as references. The present results are well explained by shell-model calculations in the full $sd$-shell model space. | |
| dc.description | Accepted for publication in Physics Letters B | |
| dc.identifier | https://arxiv.org/abs/0901.1059 | |
| dc.identifier | http://arxiv.org/abs/0901.1059 | |
| dc.identifier | Phys.Lett.B672:120-125,2009 | |
| dc.identifier | doi:10.1016/j.physletb.2009.01.006 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/226403 | |
| dc.subject | Nuclear Experiment | |
| dc.title | Quadrupole Moments of Neutron-Deficient $^{20, 21}$Na | |
| dc.type | text |