Phonons have been measured in {β}-Ti and {β}-Zr over the whole range of existence of the high-temperature bcc phase. Low-frequency and strongly damped longitudinal phonons at q=(2/3(111) produce the necessary displacements for the martensitic {β}-{ω} transition. The displacements needed for the martensitic {β}-{α} transition are produced by low-frequency and damped transverse phonons at q=(1/2(110), which on approaching the phase transition soften further but not completely. The low-frequency and strongly damped phonons are precursor fluctuations of the {α} or {ω} phase within the {β} phase.
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Heiming et al. (1989) studied this question.
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