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The correction of measured integrated intensities for the first-order thermal diffuse scattering (TDS) is considered on the basis of the existing theory of X-ray thermal diffuse scattering for an elastic wave of long wave length. Generalized formula for the TDS correction α is found to be represented by a quadratic form in the Miller indices h, k, l and a tensor Δβ, as α = Δβ11h2 + Δβ22k2 + Δβ33l2 + 2Δβ12hk + 2Δβ23kl + 2Δβ31lh. Δβ is a tensor introduced in this paper which characterizes the anisotropy of the TDS correction. The form of the tensor Δβ is shown to depend only on the crystallographic system. The relation between Δβ and the temperature-parameter tensor is presented.

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