Abstract
The frequency and temperature dependence of the optical conductivity of AlCuFe in quasicrystalline and rhombohedral phases is linear from ∼ 0.03eV up to energies E c h ̵ ω max ∼ 1 eV . A microscopic compartmentalization model explains how this happens in AlCuFe and predicts E c in other quasicrystals. The model explains the various signs of the Hall voltages in the crystalline, quasicrystalline and amorphous phases of AlCuFe. It also explains both the successes and the failures of the pair hopping model for the linear conductivity of weakly compensated semiconductor impurity bands.
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