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VOLUME 20 | ISSUE 1 | PAGE 11
Use of the anomalous passage effect to obtain stimulated emission of γ quanta in a crystal
The possibility of increasing the coherent active region in the generation of the paired Bragg state of γ quanta in a crystal by nuclei is demonstrated. To this end it is necessary that the Borrman effect be realized for one of the polarizations, that the suppression effect be simultaneously absent, and that the state with this polarization be an eigenstate of the crystal.




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