Angle-resolved photoemission spectroscopy utilizing synchrotron radiation has been used to study the electronic structure of a TiC0.96(111) surface. A sharp emission from a surface state is observed at just below the Fermi level (0.20 eV at the {Γ}{} point) which is rapidly quenched by hydrogen adsorption. In addition, a weak emission peak is observed at 0.55 eV, which is also derived from the polar structure of the (111) surface but is insensitive to hydrogen adsorption. The two-dimensional band dispersion of the surface state is not found directly, but off-normal-emission measurements suggest that the state disperses upwards for both the {Γ}{}{→}M{} and {Γ}{}{→}K{} directions above the Fermi level. A resonant enhancement of the surface-state emission is found at h{ν}{~}45 eV.
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Edamoto et al. (1992) studied this question.
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