Related Experiment Videos
Conductance distributions in quasi-one-dimensional disordered wires
L S Froufe-Pérez1, P García-Mochales, P A Serena
1Departamento de Física de la Materia Condensada and Instituto Nicolás Cabrera, Universidad Autónoma de Madrid, Spain.
Physical Review Letters
|December 18, 2002
Summary
The distribution of conductances in disordered wires shows a sharp feature at g=1 in the metal-insulator crossover. This finding aligns with Monte Carlo simulations and tight-binding calculations.
Area of Science:
- Condensed Matter Physics
- Disordered Systems
- Quantum Transport
Background:
- Understanding electron transport in disordered systems is crucial for materials science.
- The metal-insulator crossover describes the transition between metallic and insulating behavior in materials.
- Quasi-one-dimensional disordered wires present a unique system for studying quantum transport phenomena.
Purpose of the Study:
- To analyze the distribution of conductances P(g) in quasi-one-dimensional disordered wires.
- To investigate the validity of perturbation theory in the metal-insulator crossover regime.
- To compare results from Monte Carlo simulations with numerical calculations and experimental observations.
Main Methods:
- Monte Carlo solution of the Dorokhov, Mello, Pereyra, and Kumar (DMPK) scaling equation.
- Tight-binding numerical calculations for bulk disordered wires.
- Perturbation theory analysis for conductances.
Main Results:
- The distribution of conductances P(g) obtained from DMPK equation matches tight-binding calculations.
- Perturbation theory is valid for mean dimensionless conductances
around 1. - A distinct sharp feature in P(g) at g=1 is observed in the crossover regime, differing from surface-disordered wires.
Conclusions:
- The DMPK equation accurately describes conductance distributions in disordered wires.
- Perturbation theory provides a reliable tool for analyzing transport properties even at low conductances.
- The observed feature at g=1 highlights differences between bulk and surface disorder effects.