Path Integral Approach to the Scattering Theory of Quantum Transport
arXiv:cond-mat/9710202 · doi:10.1103/PhysRevB.57.12448
Abstract
The scattering theory of quantum transport relates transport properties of disordered mesoscopic conductors to their transfer matrix $\bbox{T}$. We introduce a novel approach to the statistics of transport quantities which expresses the probability distribution of $\bbox{T}$ as a path integral. The path integal is derived for a model of conductors with broken time reversal invariance in arbitrary dimensions. It is applied to the Dorokhov-Mello-Pereyra-Kumar (DMPK) equation which describes quasi-one-dimensional wires. We use the equivalent channel model whose probability distribution for the eigenvalues of $\bbox{TT}^{\dagger}$ is equivalent to the DMPK equation independent of the values of the forward scattering mean free paths. We find that infinitely strong forward scattering corresponds to diffusion on the coset space of the transfer matrix group. It is shown that the saddle point of the path integral corresponds to ballistic conductors with large conductances. We solve the saddle point equation and recover random matrix theory from the saddle point approximation to the path integral.
REVTEX, 9 pages, no figures
References in corpus (7)
- Mesoscopic Transport Through Ballistic Cavities: A Random S-Matrix Theory Approach
- Exact Solution for the Distribution of Transmission Eigenvalues in a Disordered Wire and Comparison with Random-Matrix Theory
- On the distribution of transmission eigenvalues in disordered wires
- Quantum Transport in Disordered Wires: Equivalence of One-Dimensional Sigma Model and Dorokhov-Mello-Pereyra-Kumar Equation
- Equivalence of Fokker-Planck approach and non-linear -model for disordered wires in the unitary symmetry class
- Universality of Weak Localization in Disordered Wires
- Fokker-Planck description of the transfer matrix limiting distribution in the scattering approach to quantum transport