Characterization of the negatively charged NV defect through the spin density distribution and the hyperfine coupling constants

Author(s):  
Anna M. Ferrari ◽  
Khaled E. El-Kelany ◽  
Francesco S. Gentile ◽  
Maddalena D'Amore ◽  
Eleonora Romeo ◽  
...  
1976 ◽  
Vol 31 (8) ◽  
pp. 1153-1154 ◽  
Author(s):  
Frank H. Köhler ◽  
G. Matsubayashi

The 13C NMR spectra of seven phenylated paramagnetic metallocenes have been recorded. From the spectra the 13C hyperfine coupling constants A(13C) have been extracted and compared with corresponding A(1H). It is found that the phenyl A′s in nickelocenes and cobaltocenes behave as in benzyl radical being reduced by a factor of 27. This offers a new route to informations about spin density distribution in substituted methyl radicals.


2004 ◽  
Vol 108 (31) ◽  
pp. 11529-11534 ◽  
Author(s):  
Mario Chiesa ◽  
Paola Martino ◽  
Elio Giamello ◽  
Cristiana Di Valentin ◽  
Annalisa del Vitto ◽  
...  

1966 ◽  
Vol 21 (11) ◽  
pp. 1036-1038 ◽  
Author(s):  
Franz A. Neugebauer ◽  
Peter H. H. Fischer

Bis- (4-R-aryl) -nitroxides show an excellent correlation between nitrogen hyperfine coupling constants and Hammett’ s σ-values. This can be explained through the effect of symmetric substitution and a vanishingly small dependence of aN on the oxygen spin density


1997 ◽  
Vol 52 (8) ◽  
pp. 919-926 ◽  
Author(s):  
Einar Möller ◽  
Joachim Sieler ◽  
Reinhard Kirmse

Abstract The molecular structure and X-as well as Q-band EPR studies of tetra-n-butylammonium-bis(1,1-dicyanoethene-2,2-dithiolato)nitrosyliron(I) enriched with 57Fe are reported, (n-Bu4N)2[Fe(NO)(i-mnt)2] crystallizes triclinically, space group P1̄ with a = 9,5147(7) Å, b = 10,4841(8) Å, c = 25,840(2) Å, α= 92,510(1)°, β= 92,895(1)°, γ= 111,156(1)° , Z = 2. The g and the hyperfine coupling tensors AN and AFe derived from the EPR spectra are rhombically-symmetric: g1 = 2,043, g2 = 2,039, g3 = 2,031, A1N = 13,8·10-4 cm-1, A2N = 11,6·10-4 cm-1, A3N = 15,2·10-4cm-1, A1Fe = 11,4·10-4cm-1, A2Fe = 15,7·10-4cm-1 and A3Fe = -2,6·10-4cm-1. The spin-density distribution within the first coordination sphere is discussed.


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