Crystal fields and second‐order magnetic hyperfine interactions in TmFe2Si2

1984 ◽  
Vol 55 (6) ◽  
pp. 2297-2299 ◽  
Author(s):  
A. M. Umarji ◽  
G. K. Shenoy ◽  
D. R. Noakes ◽  
S. Dattagupta
Symmetry ◽  
2020 ◽  
Vol 12 (4) ◽  
pp. 498 ◽  
Author(s):  
Timo Fleig ◽  
Leonid V. Skripnikov

We present state-of-the-art string-based relativistic general-excitation-rank configuration interaction and coupled cluster calculations of the electron electric dipole moment, the nucleon–electron scalar-pseudoscalar, and the magnetic hyperfine interaction constants ( α d e , α C S , A | | , respectively) for the thallium atomic ground state 2 P 1 / 2 . Our present best values are α d e = − 558 ± 28 , α C S = 6.77 ± 0.34 [ 10 − 18 e cm], and A | | = 21172 ± 1059 [MHz]. The central value of the latter constant agrees with the experimental result to within 0.7% and serves as a measurable probe of the P , T -violating interaction constants. Our findings lead to a significant reduction of the theoretical uncertainties for P , T -odd interaction constants for atomic thallium but not to stronger constraints on the electron electric dipole moment, d e , or the nucleon–electron scalar-pseudoscalar coupling constant, C S .


1976 ◽  
Vol 2 (1) ◽  
pp. 208-209
Author(s):  
B. Perscheid ◽  
H. B�chsler ◽  
K. Freitag ◽  
M. Forker

2008 ◽  
Vol 20 (4) ◽  
pp. 1381-1389 ◽  
Author(s):  
Thomas Fickenscher ◽  
Sudhindra Rayaprol ◽  
Jörg von Appen ◽  
Richard Dronskowski ◽  
Rainer Pöttgen ◽  
...  

ChemInform ◽  
2008 ◽  
Vol 39 (20) ◽  
Author(s):  
Thomas Fickenscher ◽  
Sudhindra Rayaprol ◽  
Joerg von Appen ◽  
Richard Dronskowski ◽  
Rainer Poettgen ◽  
...  

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