Download Optical Properties of Solids by Frederick Wooten (Auth.) PDF

By Frederick Wooten (Auth.)

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M. Lifshitz, "Electrodynamics of Continuous Media," Pergamon Press, Oxford, 1960. Chapter 3 ABSORPTION AND DISPERSION This chapter consists mostly of a rather elementary treatment of absorp­ tion and dispersion. It includes some simple examples of applications to optical properties and photoemission. The classical theory of absorption and dispersion is due mainly to Lorentz and Drude. , all transitions for which the final state of an electron lies in a different band but with no change in k-vector in the reduced zone scheme.

5 Define a complex conductivity à = σ1 + ia& where σχ is the usual real conductivity σ that appears in Maxwell's equations. Maxwell's equa­ tions, including the properties of the medium, can now be written in terms of a complex conductivity rather than a complex dielectric function. What is the relationship of σ to έ? What is the relationship of Jind(q, ω) to E(q, co) in terms of â(q, ω)? Define a transverse "optical" conductivity σ τ . What is the relationship of στ to

The only apparent similarity between Eqs. 119) is that each provides a relation­ ship between a total electric field and an induced current density. Before proceeding with a simplification of Eq. 119), it is worth noting that the real dielectric function ε that appears in Maxwell's equations is a longitudinal dielectric function. 120) This is the reason for the relative simplicity of Eq. 113). It is clear from Eq. 120) that the dielectric function appearing in Maxwell's equations is a longitudinal dielectric function.

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