We have used photoelectron spectroscopy to study the filling of conduction band states of the layered semiconductors and as they are intercalated by Cs. Comparison is also made with `self-intercalated' . Even in the pure samples, occupied conduction band states due to excess Ti/Zr are found, but this occupancy is greatly increased by Cs intercalation. The stoichiometries are estimated from the extent in k -space of the occupied bands. A weak structure just below the conduction band minimum of is tentatively attributed to localized defect states.
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Starnberg et al. (1996) studied this question.
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