It is shown that the conductance of an interacting one-dimensional system may be expressed in the form of a Landauer formula. An insulator-ideal-conductor transition is found as the interaction is varied at zero temperature.
Electron conduction in one-dimensional system is investigated explicitly taking into account the reservoirs to which 1D channel is connected at its ends. We calculate the current driven by the chemical potential difference of two reservoirs, using the linear response theory by Kubo. At 0K, the conductance of 1D channel is expressed in terms of one-electron Green's functions even in the presence of the interaction, in contrast to the theory based on Kubo formula, in which two-electron Green's functions are essentially involved. The formalism in this paper provides a new interpretation of Landauer formula. As regards the interaction effects, the conductance of Fermi liquid without potential scattering is 2 e 2 / h , while that of Tomonaga-Luttinger liquid deceases with power low as the length of 1D channel increases.
Using numerical diagonalization techniques we analyze the finite temperature/frequency conductance of a one-dimensional model of interacting spinless fermions. Depending on the interaction, the observed finite temperature charge stiffness and low-frequency conductance indicate a fundamental difference between integrable and nonintegrable cases. The integrable systems behave as ideal conductors in the metallic regime and as ideal insulators in the insulating one. The nonintegrable systems are, as expected, generic conductors in the metallic regime and activated ones in the insulating regime. \textcopyright{} 1996 The American Physical Society.
Impurity scattering is introduced in the Tomonaga model of an interacting one-dimensional Fermi system. The dynamic (frequency-dependent) conductivity is averaged over the random potential resulting from the impurities. To study this function the author exploits connections to two different two-dimensional classical models for which a Kosterlitz-Thouless-like transition is obtained. Thus, the system's conductivity changes from the usual insulating form to the ideal conducting behaviour of free fermions. Whether the system insulates or conducts depends on the sign and the strength of the fermionic interaction in qualitative agreement with the behaviour of the density response function and the pairing susceptibility of the pure system.
Dynamical conductivity in a disordered one-dimensional model of interacting fermions is studied numerically at high temperatures and in the weak-interaction regime in order to find a signature of many-body localization and vanishing dc transport coefficients. On the contrary, we find in the regime of moderately strong local disorder that the dc conductivity ${\ensuremath{\sigma}}_{0}$ scales linearly with the interaction strength while being exponentially dependent on the disorder. According to the behavior of the charge stiffness evaluated at the fixed number of particles, the absence of the many-body localization seems related to an increase in the effective localization length with the interaction.
Using the formalism of Ford-Kac-Mazur we study nonequilibrium transport in fermionic systems connected to general particle and thermal reservoirs. Several exact results on electrical and thermal transport in one-dimensional disordered non-interacting fermionic wires are obtained. Landauer’s formula is shown to follow for a special choice of reservoirs. For general reservoirs the currents in the system depend on the spectral properties of the reservoirs and Landauer’s formula needs modification. Some experimental implications are discussed.