Optical responses in two-dimensional tilted semi-Dirac bands

Abstract

Within linear response theory, the absorptive part of optical conductivities are analytically calculated for distinct tilts in two-dimensional (2D) tilted semi-Dirac bands (TSDBs). The transverse optical conductivities always vanish ReΟƒxy(Ο‰)=ReΟƒyx(Ο‰)=0\mathrm{Re}\sigma_{xy}(\omega)=\mathrm{Re}\sigma_{yx}(\omega)=0. The interband longitudinal optical conductivities (LOCs) in 2D TSDBs differ qualitatively in the power-law scaling of Ο‰\omega as ReΟƒxxIB(Ο‰)βˆΟƒ0Ο‰\mathrm{Re}\sigma_{xx}^{\mathrm{IB}}(\omega)\propto\sigma_0\sqrt{\omega} and ReΟƒyyIB(Ο‰)βˆΟƒ0/Ο‰\mathrm{Re}\sigma_{yy}^{\mathrm{IB}}(\omega)\propto\sigma_0/\sqrt{\omega}. By contrast, the intraband LOCs in 2D TSDBs depend on ΞΌ\mu in the power-law scaling ReΟƒxxD(Ο‰)βˆΟƒ0ΞΌΞΌ\mathrm{Re}\sigma_{xx}^{\mathrm{D}}(\omega)\propto\sigma_0\mu \sqrt{\mu} and ReΟƒyyD(Ο‰)βˆΟƒ0ΞΌ/ΞΌ\mathrm{Re}\sigma_{yy}^{\mathrm{D}}(\omega)\propto\sigma_0\mu/\sqrt{\mu}. The power-law scaling is similar to that in 2D untilted SDBs but distincts from a uniform behavior independent of Ο‰\omega (or ΞΌ\mu) as ReΟƒxx/yyIB(Ο‰)βˆΟƒ0\mathrm{Re}\sigma_{xx/yy}^{\mathrm{IB}}(\omega)\propto\sigma_0 (or ReΟƒxx/yyD(Ο‰)βˆΟƒ0ΞΌ\mathrm{Re}\sigma_{xx/yy}^{\mathrm{D}}(\omega)\propto\sigma_0\mu) in 2D tilted Dirac bands (TDBs). The universal power-law scaling further dictates significant differences in the angular dependence of LOCs, which can be used to characterize 2D TSDBs from 2D TDBs in the optical measurements. The tilt-dependent behaviors of LOCs can qualitatively tell 2D TSDBs from 2D untilted SDBs, but show similarities in the impact of band tilting between 2D TSDBs and 2D TDBs.Comment: 16 pages, 3 figure

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