We report ab initio calculations of the electronic structure of large-unit-cell approximant phases to icosahedral Ti-transition-metal quasi-crystals and of disordered alloys of the same composition. Our results demonstrate that the approximant phase is stabilized relative to the body-centred solid solution by the formation of a broad pseudogap at the Fermi level. The conditions for the formation of the pseudogap are discussed in relation to the atomic structure.
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Krajčı́ et al. (1994) studied this question.
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