Abstract

We calculate the high frequency macroscopic dielectric function e(ω) of YBaCuO by treating the solid as a dense gas of polarizable cells. The cell polarizability is constructed from independent atomic contributions within a local-density based random phase approximation (LDRPA) and improvements thereof. In this way, interband transitions are treated very schematically but transitions from the core-like Ba 5p6 shell are treated quite well. This is important, because the intense Ba 5p–5d like giant dipole resonance provides about half of the optical conductivity around 20 eV and contributes strongly to the all-valence electron plasma frequency.

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