Conclusions
-
1.
The EPR spectrum of irradiated potassium silicate glasses having slight alkali contents (g varies from 2.000 to 2.025) cannot be produced by superimposing two lines, one of which is typical of glasses having a large alkali content α1, and the other of which is due to a paramagnetic center having S =1/2 and complete g-factor anisotropy.
-
2.
The agreement with experiment is better if we assume a completely anisotropic g-factor for α3 (one of the three lines α1, α2, α3).
Literature cited
E. A. Zamotrinskaya, Izv. Vuzov. Fizika, No. 9, 106 (1968).
I. W. H. Schreurs, J. Chem. Phys.,47, 818 (1967).
F. K. Kheubuhl, J. Chem. Phys.,33, 1047 (1960).
T.S. Johnston and H.G. Hecht, J. Mol. Spectrosc.,17, 98 (1965).
B. Bleaney, Proc.Phys.Soc.,A63, 407 (1950).
Author information
Authors and Affiliations
Additional information
Translated from Izvestiya Vysshikh Uchebnykh Zavedenii Fizika, No. 8, pp. 149–152, August, 1969.
Rights and permissions
About this article
Cite this article
Zamotrinskaya, E.A. Shape modeling of the epr spectrum of alkali silicate glasses. Soviet Physics Journal 12, 1096–1098 (1969). https://doi.org/10.1007/BF00820953
Received:
Issue Date:
DOI: https://doi.org/10.1007/BF00820953