Magnetic moment and electric quadrupole moment of the 18N ground state

被引:40
作者
Ogawa, H
Asahi, K
Sakai, K
Yoshimi, A
Tsuda, M
Uchiyama, Y
Suzuki, T
Kurokawa, N
Adachi, M
Izumi, H
Ueno, H
Shimoda, T
Tanimoto, S
Takahashi, N
Schmidt-Ott, WD
Schäfer, M
Fukuda, S
Yoshida, A
Notani, M
Kubo, T
Okuno, H
Sato, H
Aoi, N
Yoneda, K
Iwasaki, H
Fukuda, N
Fukunishi, N
Ishihara, M
Miyatake, H
机构
[1] Tokyo Inst Technol, Dept Phys, Meguro Ku, Tokyo 1528551, Japan
[2] Osaka Univ, Dept Phys, Osaka 5600043, Japan
[3] Univ Gottingen, Zweites Phys Inst, D-37073 Gottingen, Germany
[4] RIKEN, Wako, Saitama 35101, Japan
[5] Univ Tokyo, Dept Phys, Bunkyo Ku, Tokyo 1130033, Japan
[6] KEK, Tanashi Branch, Tokyo 1888501, Japan
关键词
N-18 ground state; magnetic moment; electric quadrupole moment; neutron-rich nuclei; beta-NMR projectile fragmentation; spin polarization; shell model; effective charge;
D O I
10.1016/S0370-2693(99)00219-1
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The magnetic moment and electric quadrupole moment of a neutron-rich nucleus N-18 have been determined by the beta-NMR method, taking advantage of the fragment spin polarization induced in the intermediate-energy projectile fragmentation reaction. To assure the existence of a sufficient polarization prior to the resonance search, a scheme of polarization measurement by means of an adiabatic field rotation has been developed and successfully incorporated in the beta-NMR experiment. From the observed resonance in a Pt stopper the magnetic moment for the N-18 ground state has been determined to be \mu\ = 0.3279 +/- 0.0013 mu(N). The N-18 fragments have also been implanted in a single crystal Mg stopper, and from the observed quadrupole frequency \eqQ/h\ = 73.2 +/- 1.4 kHz, the electric quadrupole moment \Q\ = 12.3 +/- 1.2 mb has been deduced. The obtained mu and Q are compared with shell model calculations. (C) 1999 Published by Elsevier Science B.V. All rights reserved.
引用
收藏
页码:11 / 18
页数:8
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