By M. V. Fok (auth.), Academician D. V. Skobel’tsyn (eds.)
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Extra info for Luminescence and Nonlinear Optics
E. E. Bukke, T. 1. Voznesenskaya, N. P. Golubeva, N. A. Gorbacheva, Z. P. Kaleeva, E. I. Panasyuk, and M. V. Fok, Zh. Prikl. , 12:1047 (1970). V. F. Tunitskaya, Zh. Prikl. , 10:1004 (1969). K. Era, S. Shionoya, and Y. Washizawa, J. Phys. Chem. Solids, 29:1827 (1968); K. Era, S. Shionoya, Y. Washizawa, and H. Ohmatsu, J. Phys. Chem. Solids, 29:1843 (1968). M. V. Fok, This volume, p. 1. T. 1. Voznesenskaya and M. V. Fok, Opt. , 15:249 (1963). PREPARATION OF ZINC SULFIDE CRYSTALS AND NATURE OF BLUE LUMINESCENCE CENTERS IN SELF-ACTIV ATED ZnS Z.
7 eV. 4 eV is converted into heat in each recombination event in such centers. If this energy is evolved at the moment of charge localization, the levels at which such localization occurs cannot be re- E. E. BUKKE ET AL. , the first eondition is not satisfied. , the seeond eondition is not satisfied. If both eonditions are satisfied, the energy lost as a result of reeombination eannot be large. , the lumineseenee bands in question must lie in the ultraviolet part of the spectrum. APPENDIX List of Sampies Investigated a) Single Crystals Grown from the Vapor Phase in Closed (But Not Sealed) Ampoules by the Grillot Method No.
Mum and overestimated in the case of a spectral minimum. Therefore, it is best to use the smallest number of points in the determination of the average ordinate of the horizontal part: if this is done the random scatter introduces smaller errors than the systematic deviation because in subsequent operations the systematic errors are cumulated and the random scatter is averaged out. " In other words, the horizontal region is considered as bounded by horizontallines and not vertical ones. The continuous curve in Fig.