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The photoneutron angular distributions from carbon and beryllium have been measured by using bremsstrahlung of maximum energies of 23 Mev and 18 Mev, respectively. The results are 1+(1.35±0.88)sin²θ for carbon and (1.26±0.11)+sin²θ for beryllium.
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Fabricand et al. (1956) studied this question.
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