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The study of the photoconductivity quenching as a function of the electric field in the ternary compound ZnIn2S4 has given evidence of a level localized at about 1.77 eV above the valence band which is responsible for the capture of hot electrons and for the N-type negative resistance. By a rough estimate of the quenching compared with the experimental it was possible to determine the potential barrier offered by the centre to the electrons, for a fixed illumination intensity of the gap energy light upon the crystal.
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Romeo et al. (1972) studied this question.
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