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G. N. Ramachandran

Researcher at Indian Institute of Science

Publications -  89
Citations -  6104

G. N. Ramachandran is an academic researcher from Indian Institute of Science. The author has contributed to research in topics: Diamond & Hydrogen bond. The author has an hindex of 26, co-authored 89 publications receiving 5960 citations. Previous affiliations of G. N. Ramachandran include University of Madras & University of Chicago.

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On the transmission of light through a cloud of randomly distributed particles

TL;DR: In this article, the authors investigated the attenuation of light transmitted through a cloud of particles distributed at random in a transparent medium and found that the transmitted beam is progressively attenuated, the intensity diminishing exponentially with the increase in the thickness of the medium.
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Thermo-optic behaviour of solids: II. Fused quartz

Abstract: SummaryThe theory outlined in Part I of these series has been applied to calculate the thermal variation of refractive index of fused silica. It is found that the theory can account quantitatively for the experimental values ofdn/dt over the range of wavelengths from 1850 Å.U. to 6000 Å.U. Using the fact that the frequencies of vitreous silica are practically the same as those of crystalline quartz, the variation of the refractive index with temperature from −130°C. to 500°C. has been calculated and found to fit well with the experimental data.
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Anomalous Dispersion Method: Its Power for Protein Structure Analysis

TL;DR: Theoretical studies show that the method of resolving this ambiguity by choosing the phases closer to those of the heavy atoms has a good potentiality for solving complicated structures, in which the average heavy atom contribution to the intensity is as low as 10 percent.
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X-ray anti-reflections in crystals

TL;DR: In this article, it was shown that the intensity of the transmitted beam may exhibit a peak larger than the background when a Bragg reflection occurs in an absorbing crystal, and that the anti-reflection peak becomes more prominent, the greater the thickness of the crystal.