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The observation of a sharp cusp in the temperature derivative of the magnetic susceptibility d chi /dT is often used as a signature of a second-order structural phase transition. Such behaviour is particularly prominent in low-dimensional compounds undergoing a Peierls transition, where there is a large change in the density of states. Using general arguments borrowed from magnetism, the author shows that it is short-range order parameter fluctuations close to T c that lead to the observed behaviour of chi ; the addition of impurities produces rounding of the d chi /dT cusp when the true phase transition is destroyed by disorder. The theory compares favourably with experiment.
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Premala Chandra (1989) studied this question.
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