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Updated: Feb 17, 2026

Setting Limits on Supersymmetry Using Simplified Models
Published on: November 15, 2013
The tight-binding formulation of the Kronig-Penney model
1Department of Physics, University of Alberta, Edmonton, AB, T6G 2E1, Canada. fm3@ualberta.ca.
This study derives the tight-binding model from exact solutions for particles in periodic potentials. It reveals that next-nearest-neighbor hopping is crucial for accurate electronic band structure descriptions.
Area of Science:
- Condensed Matter Physics
- Quantum Mechanics
- Materials Science
Background:
- Electronic band structure calculations are often approximated using the tight-binding model.
- The tight-binding model is widely applied in studying electron correlations in materials.
Purpose of the Study:
- To derive the tight-binding model from the exact solution of a particle in a periodic array of square wells.
- To analyze the necessity of next-nearest-neighbor hopping and electron-hole asymmetry in this model.
Main Methods:
- Exact solution of a particle bound in a periodic one-dimensional array of square well potentials.
- Derivation of the dispersion relation for the tight-binding model.
- Analysis of transition amplitudes for a two-state effective model of a double-well potential.
Main Results:
- An effective next-nearest-neighbor hopping parameter is required for an accurate description of the derived band structure.
- Electron-hole asymmetry is observed, except in the extreme tight-binding limit, arising from the effective next-nearest-neighbor hopping term.
- The necessity of a next-nearest-neighbor tunneling parameter in a simplified double-well model does not imply actual next-nearest-neighbor tunneling.
Conclusions:
- The derived tight-binding model provides a more accurate description by including effective next-nearest-neighbor hopping.
- The study clarifies the origin of electron-hole asymmetry in such models.
- The findings offer insights into the parametrization and interpretation of tight-binding models in condensed matter physics.
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