Titlebook: Radiative Recombination in Semiconducting Crystals; D. V. Skobel’tsyn (Director) Book 1975 Springer Science+Business Media New York 1975

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Radiative Recombination in Cadmium Telluride Crystals,et the majority of the observed luminescence lines and bands. A study was made of the strength of the electron — phonon interaction in optical transitions as a function of the nature of the centers involved. The profiles of the luminescence bands resulting from the recombination at deep levels were explained.

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Ultraviolet Cathodoluminescence and Photoluminescence of Zinc Sulfide,gy and spectral characteristics. The radiative transitions explaining the results were identified. The explanation of the edge luminescence was based on a donor-acceptor model of radiative transitions at local levels associated with intrinsic lattice defects.

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Ionization Domains in Strong Fields and Motion of Luminous Regions in Crystals,on the experimentally determined values indicated that the field intensity in a double layer associated with such domains was of the order of 2 × 10. V/cm. The effective ionization cross section of donors was estimated to be of the order of 3 × 10. cm..

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Ionization Domains in Strong Fields and Motion of Luminous Regions in Crystals,e at a velocity of about 4 × 10. cm/sec. These luminous regions were due to a new type of instability called ionization domains. An analysis was made of the processes of impact ionization in high fields, which can generate and maintain space-charge regions in a crystal. Quantitative estimates based

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Investigation of the Energy Band Structure of Semiconductors by Differential Optical Methods,sults were used to determine the gaps between the energy bands and the values of the spin — orbit splitting of the valence band at the symmetry points Γ, L, and A of the Brillouin zone. Single crystals of CdTe were studied and it was found that the Coulomb interaction between electrons and holes sho

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Luminescence Delay and Determination of Nonradiative Relaxation Times,ime ..) under the influence of excitation pulses of duration t. to an upper state (lifetime .. < ..) from which the system relaxes back to the metastable state. It is shown that if t. ? ., the luminescence is delayed after the end of excitation and this delay can be used to calculate the nonradiativ

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