Abstract

We examine here our spectroscopic modification of the Pippard relation which is a linear variation of the thermal expansivity α p with the frequency shifts (1/ ν)(∂ ν/∂ p) T close to the melting point in ammonia solid II. For this we use our calculated frequencies for the Raman mode of ν (51 cm −1) in ammonia solid II for the pressures of 3.65, 5.02 and 6.57 kbars. We establish this linearity between α p and (1/ ν)(∂ ν/∂ p) T for the pressures studied in ammonia solid II close to the melting point. The observed behaviour of ammonia solid II is explained in terms of our spectroscopic relation given here.

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