Hyperfine interactions in the J = 5 states of 147Sm and 149Sm

1968 ◽  
Vol 46 (22) ◽  
pp. 2499-2507 ◽  
Author(s):  
R. G. H. Robertson ◽  
J. C. Waddington ◽  
R. G. Summers-Gill

The hyperfine interaction constants Ak(5) have been measured in 147Sm and 149Sm. Consideration of the k = 2 results together with Woodgate's values of A2(J) for J = 1 to 4 shows that his nonrelativistic treatment of the electric quadrupole interaction in samarium is inadequate but that a relativistic one gives excellent agreement. The effect cannot be confused with a possible configuration interaction as it can in the case of the magnetic dipole interaction. Allowance for the effects of octupolelike second-order corrections and more precise computation of the dipole- and quadrupole-like corrections markedly affect the published results for the hyperfine constants in the lower J states, but the revision does not improve the agreement with the theoretical expressions. It would appear that Conway and Wybourne's analysis of the breakdown of L–S coupling in the nominally 7F ground term is not adequate, particularly for the computation of the coefficient of the sC2 term.

1963 ◽  
Vol 40 ◽  
pp. 656-669 ◽  
Author(s):  
E. Matthias ◽  
L. Boström ◽  
Alice Maciel ◽  
M. Salomon ◽  
T. Lindqvist

1993 ◽  
Vol 74 (3) ◽  
pp. 399-414 ◽  
Author(s):  
Per Jönsson ◽  
Claes-Göran Wahlström ◽  
Charlotte Froese Fischer

1991 ◽  
Vol 69 (7) ◽  
pp. 808-812 ◽  
Author(s):  
J. Sagle ◽  
W. A. van Wijngaarden

Quantum beats arising from the hyperfine interaction were observed in the fluorescence produced when the 8D3/2, 9D3/2, and 10D3/2 states of 133Cs radiatively decayed to the 6P1/2 state. The period of the beats equals the reciprocal of the magnetic dipole coupling constant a since the 133Cs nucleus has a negligibly small electric quadrupole moment. The results are a = 3.95 ± 0.01, 2.38 ± 0.01, and 1.54 ± 0.02 MHz for the 8D3/2, 9D3/2, and 10D3/2 states, respectively.


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