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With the use of monocrystalline targets for bremsstrahlung and pair production experiments, interference phenomena are expected to occur which will markedly change the γ-ray spectrum as well as the pair energy distribution, for certain angles giving enhancement of radiation and pairs. The effect increases with energy; it sets in at δn₀(2πa), where δ is the minimum momentum transfer to the target atoms, a the lattice constant, and n₀ a number of the order 2 or 3. This corresponds to {~}200-Mev primary energy for bremsstrahlung, {~}1 Bev for pair production. The effect is confined to angles between the primary beam and a line of atoms, of order θ(ascreenλC)(mc²E). The temperature motion of the lattice reduces the interference effect to some extent. The Born approximation was used for the quantitative analysis of the problem.
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H. Überall (1956) studied this question.
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