Hole crystallization in semiconductors
arXiv:cond-mat/0512376 · doi:10.1088/0305-4470/39/17/S63
Abstract
When electrons in a solid are excited to a higher energy band they leave behind a vacancy (hole) in the original band which behaves like a positively charged particle. Here we predict that holes can spontaneously order into a regular lattice in semiconductors with sufficiently flat valence bands. The critical hole to electron effective mass ratio required for this phase transition is found to be of the order of 80.
accepted for publication in J. Phys. A: Math. Gen
References in corpus (5)
- Wigner Crystallization in mesoscopic 2D electron systems
- Thermodynamics of hot dense H-plasmas: Path integral Monte Carlo simulations and analytical approximations
- Crystallization in two-component Coulomb systems
- Three-body crystallization diagrams and the cooling of white dwarfs
- Exciton formation and dissociation in mass-asymmetric electron-hole plasmas
Cited by in corpus (8)
- First principles simulations of dense hydrogen
- Classical and quantum Coulomb crystals
- Comment on "Discussion on `Novel attractive force between ions in quantum plasmas -- failure of simulations based on a density functional approach"
- Correlation effects in partially ionized mass asymmetric electron-hole plasmas
- Color path-integral Monte-Carlo simulations of quark-gluon plasma: Thermodynamic and transport properties
- Structural transitions of finite spherical Yukawa crystals
- Equation of state of strongly coupled quark--gluon plasma -- Path integral Monte Carlo results
- Quantum simulations of strongly coupled quark-gluon plasma