Electronegativity, Charge Transfer, Crystal Field Strength, and the Point Charge Model Revisited

2013 ◽  
Vol 117 (7) ◽  
pp. 1503-1507 ◽  
Author(s):  
Peter A. Tanner ◽  
Lixin Ning
1977 ◽  
Vol 55 (10) ◽  
pp. 937-942 ◽  
Author(s):  
A. F. Leung ◽  
Ying-Ming Poon

The absorption spectra of UCl5 single crystal were observed in the region between 0.6 and 2.4 μm at room, 77, and 4.2 K temperatures. Five pure electronic transitions were assigned at 11 665, 9772, 8950, 6643, and 4300 cm−1. The energy levels associated with these transitions were identified as the splittings of the 5f1 ground configuration under the influence of the spin–orbit coupling and a crystal field of C2v symmetry. The number of crystal field parameters was reduced by assuming the point-charge model where the positions of the ions were determined by X-ray crystallography. Then, the crystal field parameters and the spin–orbit coupling constant were calculated to be [Formula: see text],[Formula: see text], [Formula: see text], and ξ = 1760 cm−1. The vibronic analysis showed that the 90, 200, and 320 cm−1 modes were similar to the T2u(v6), T1u(v4), and T1u(v3) of an UCl6− octahedron, respectively.


1999 ◽  
Vol 110 (2) ◽  
pp. 741-754 ◽  
Author(s):  
Jay L. Banks ◽  
George A. Kaminski ◽  
Ruhong Zhou ◽  
Daniel T. Mainz ◽  
B. J. Berne ◽  
...  

1968 ◽  
Vol 23 (12) ◽  
pp. 1980-1987 ◽  
Author(s):  
H. J. Gläser ◽  
D. Geist

The EPR-parameters of Eu2+ substituted for Cd2+ in CdF2 have been measured at 300, 77 and 1,5°K. They are summarized in Table 1. The EPR spectrum is that of an S-state-ion in a cubic environment. As with Eu2+ inCaF2, SrF2 or BaF2 there is in CdF2 a superhyperfine (SHF) -interaction between the Eu2+- and F–-ions, which results mostly in an inhomogeneous broadening of the lines but sometimes in CdF2 in a splitting. There are some indications that the point charge model is not fully correct and that a slight deviation from the cubic environment does exist.


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