Dielectric Susceptibility of(KBr)0.50(KCN)0.50: Is It a Dipole Glass?

1982 ◽  
Vol 48 (18) ◽  
pp. 1267-1270 ◽  
Author(s):  
S. Bhattacharya ◽  
Sidney R. Nagel ◽  
L. Fleishman ◽  
S. Susman
2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Wanrong Gao

AbstractIn this work, we introduce the concept of anisotropic dielectric susceptibility matrix of anisotropic medium for both nondepolarizing and depolarizing medium. The concept provides a new way of analyzing light scattering properties of anisotropic media illuminated by polarized light. The explicit expressions for the elements of the scattering matrix are given in terms of the elements of the Fourier transform of the anisotropic dielectric susceptibility matrix of the medium. Finally, expressions for the elements of the Jones matrix of a thin layer of a deterministic anisotropic medium and the elements of the Mueller matrix of a depolarizing medium are given. The results obtained in this work is helpful for deriving information about the correlated anisotropic structures in depolarizing media from measured Mueller matrices. The findings in this work may also well prove stimulating to researchers working on new methods for analyzing light scattering properties.


1993 ◽  
Vol 10 (9) ◽  
pp. 558-561 ◽  
Author(s):  
Baodong Qu ◽  
Chunlei Wang ◽  
Weilie Zhong ◽  
Zhonglie Wang

2010 ◽  
Vol 400 (1) ◽  
pp. 427-433 ◽  
Author(s):  
P. N. Timonin
Keyword(s):  

2004 ◽  
Vol 833 ◽  
Author(s):  
Nadia K. Pervez ◽  
Jiwei Lu ◽  
Susanne Stemmer ◽  
Robert A. York

ABSTRACTIn universal relaxation, a material's complex dielectric susceptibility follows a fractional power law f1-n where 0 < n < 1 over multiple decades of frequency. In a variety of materials, including Ba0.5Sr0.5Ti03, dielectric relaxation has been observed to follow this universal relaxation model with values of n close to 1. In this work we have shown that the universal relaxation model can be used to calculate dielectric loss even when n is very close to 1. Our calculated Q-factors agree with measured values at 1 MHz; this agreement suggests that this technique may be used for higher frequencies where network analyzer measurements and electrode parasitics complicate Q-factor determination.


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