TY - JOUR
T1 - Optical-pumping determination of the nuclear magnetic moments of the radioisotopes mercury-193, -193m, -195m, and -197m
AU - Moskowitz, P. A.
AU - Liu, C. H.
AU - Fulop, G.
AU - Stroke, H. H.
N1 - Copyright:
Copyright 2015 Elsevier B.V., All rights reserved.
PY - 1971
Y1 - 1971
N2 - The technique of optical pumping has been used to determine the nuclear magnetic dipole moment of spin-32, 4-h Hg193, and the spin-132 isomers, 10-h Hg193m, 40-h Hg195m, and 24-h Hg197m. Nuclear magnetic resonance was observed following orientation of the 6s2 S01 ground state. The results are |μ193|=0.61763(18)μN, |μ193m|=1.0416(3)μN, |μ195m|=1.0280(2)μN, and |μ197m|=1.0112(3)μN, all without diamagnetic correction. Differential hfs anomalies, Δ, have been calculated with respect to stable Hg199 with the use of the previously determined values of the magnetic dipole hfs interaction constants for the 6s6p P13 level. We obtain Δ199193=0.0054(27), Δ199193m=0.0108(3), Δ199195m=0.0106(2), and Δ199197m=0.0105(6).
AB - The technique of optical pumping has been used to determine the nuclear magnetic dipole moment of spin-32, 4-h Hg193, and the spin-132 isomers, 10-h Hg193m, 40-h Hg195m, and 24-h Hg197m. Nuclear magnetic resonance was observed following orientation of the 6s2 S01 ground state. The results are |μ193|=0.61763(18)μN, |μ193m|=1.0416(3)μN, |μ195m|=1.0280(2)μN, and |μ197m|=1.0112(3)μN, all without diamagnetic correction. Differential hfs anomalies, Δ, have been calculated with respect to stable Hg199 with the use of the previously determined values of the magnetic dipole hfs interaction constants for the 6s6p P13 level. We obtain Δ199193=0.0054(27), Δ199193m=0.0108(3), Δ199195m=0.0106(2), and Δ199197m=0.0105(6).
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U2 - 10.1103/PhysRevC.4.620
DO - 10.1103/PhysRevC.4.620
M3 - Article
AN - SCOPUS:4244025150
SN - 0556-2813
VL - 4
SP - 620
EP - 631
JO - Physical Review C
JF - Physical Review C
IS - 2
ER -