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Expressions for the real, static part ε 1 ( 0 ) and the imaginary part ε 2 ( ω ) of the dielectric constant of semiconductors in the long-wavelength limit are obtained using the isotropic nearly-free-electron band approximation (Penn model). Earlier calculations of these functions do not satisfy the Kramers-Kronig relations and yield an excessively large result for the f -sum rule. The corrected expressions eliminate these inconsistencies. Values of the energy gap between the bonding and antibonding states are obtained for diamond, silicon, and germanium, respectively. ε 1 ( ω ) is obtained from ε 2 ( ω ) through the use of the Kramers-Kronig relation. The theoretical curves for ε 1 ( ω ) and ε 2 ( ω ) are compared with experimental results.
Physical Review B – American Physical Society (APS)
Published: Sep 15, 1974
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