We measured the energy distribution of electrons emitted from a copper single crystal at 60^∘{} to the surface normal, using plane polarized light at normal incidence in the near uv region. Rotating the plane of polarization produced changes in the electron distribution between 5 and 28%. No such changes could be detected upon substituting a polycrystalline sample. The energy distribution of the single crystal differs considerably from that of the polycrystal. The results imply direct, →k-conserving transitions and no scattering for a large fraction of those excited electrons which leave the crystal.
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Gerhardt et al. (1971) studied this question.
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