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ABSTRACT THE thermal agitation of the atoms in solids results, as was shown by Raman (NATURE, Jan. 12, 1922, and Jan. 6, 1923), in a noticeable blue opalescence in the interior of such
transparent crystals as quartz or ice when they are traversed by a strong beam of sunlight. In his address on the discovery of a new type of secondary radiation (_Indian Journal of Physics_,
Mar. 31, 1928) Raman described observations showing that monochromatic light scattered in this manner by crystals is accompanied by radiations of altered wave-length in the same way as in
the case of gases and liquids. The difference between the incident and scattered frequencies corresponds, of course, to a characteristic infra-red frequency of the crystal. Access through
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BEING VIEWED BY OTHERS ANGULAR-SPECTRUM-DEPENDENT INTERFERENCE Article Open access 26 October 2021 SHAPING THE PROPAGATION OF LIGHT IN COMPLEX MEDIA Article 08 September 2022 COHERENT
ANTI-STOKES HYPER-RAMAN SPECTROSCOPY Article Open access 10 January 2025 AUTHOR INFORMATION AUTHORS AND AFFILIATIONS * 210 Bowbazar Street, Calcutta K. S. KRISHNAN Authors * K. S. KRISHNAN
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Raman Effect in Crystals. _Nature_ 122, 477–478 (1928). https://doi.org/10.1038/122477a0 Download citation * Issue Date: 29 September 1928 * DOI: https://doi.org/10.1038/122477a0 SHARE THIS
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