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Explicite solutions for the neutron wave function are calculated for the following situations: the quasioptical case (where the wavelength is large compared with the lattice constants) and both the symmetrical Bragg‐ and Laue‐cases. The calculation is based on the results of two foregoing papers. The discussions are concentrated especially on the following two points: firstly on the quasioptical case where the crystal behaves like a homogeneous medium with a refractive index containing an effective scattering amplitude f/(1 + i k f) being real for non‐absorbing nuclei, secondly on the modifications of the standing wave fields in both the symmetrical Bragg‐ and Laue‐cases if the Bragg‐conditions are not exactly fulfilled. The theory remains applicable for strong resonance absorption by the nuclei too.
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H. Solbrig (1972) studied this question.
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