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The authors observe a peak close to the Fermi level in the photoelectron spectrum of both ordered and disordered Cu 3 Au(111) near normal emission. They have studied this feature as a function of photon incidence angle, emission angle and photon energy, and conclude that it is due to a surface state whose character is similar to those previously observed on Cu(111) and Au(111).
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Jordan et al. (1982) studied this question.
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