Abstract
In Ti–44.0 Ni–6.0 Fe alloy, diffuse satellites appear at incommensurate positions given by gB2 + q when the zone axis is [1 1 1] or [0 0 1], but not [1 1 0]. This result implies that the satellites appear because of a transverse wave consistent with the displacement of atoms in the 〈1 1 0〉 direction, which is perpendicular to the propagation vector q = 〈ζ ζ ¯ 0〉∗, for ζ ∼ 1/3. This transverse wave occurs as a result of the phonon softening of the TA2 branch.
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