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Fluctuation corrections to Lifshitz tails in disordered systems
Enrique Rozas Garcia1, Johannes Hofmann1,2
1Department of Physics, Gothenburg University, 41296 Gothenburg, Sweden.
Disordered semiconductors exhibit localized electronic states, forming a universal Lifshitz tail in their density of states. This study provides analytical and numerical results for this tail, including its fluctuation prefactor, using advanced theoretical methods.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Semiconductor Physics
Background:
- Quenched disorder in semiconductors creates localized electronic states near the band edge.
- These states result in an exponential tail in the density of states.
- For high impurity densities, this tail follows a universal Lifshitz form driven by potential fluctuations.
Purpose of the Study:
- To derive analytical expressions and numerical values for the Lifshitz tail in a parabolic conduction band.
- To determine the exact fluctuation prefactor of the Lifshitz tail.
- To provide a revised result for the disorder band tail in two-dimensional systems.
Main Methods:
- Utilized a replica field integral approach to analyze the electronic states.
- Identified the instanton profile for the leading exponential scaling of the Lifshitz tail.
- Employed the Gel'fand-Yaglom formalism to compute the determinant of the fluctuation operator, avoiding full spectral calculations.
Main Results:
- Derived analytical expressions for the Lifshitz tail, including its exact fluctuation prefactor.
- Obtained numerical values for the Lifshitz tail in a parabolic conduction band.
- Presented a revised calculation for the disorder band tail in two dimensions.
Conclusions:
- The study successfully characterizes the Lifshitz tail in disordered semiconductors.
- The replica field integral and Gel'fand-Yaglom formalism provide a robust framework for analyzing disorder effects.
- The findings offer a more precise understanding of electronic states at the band edge in disordered materials.
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