Conductance of Tomonaga-Luttinger liquid wires and junctions with resistances
arXiv:1011.5058 · doi:10.1209/0295-5075/93/57007
Abstract
We study the effect that resistive regions have on the conductance of a quantum wire with interacting electrons which is connected to Fermi liquid leads. Using the bosonization formalism and a Rayleigh dissipation function to model the power dissipation, we use both scattering theory and Green's function techniques to derive the DC conductance. The resistive regions are generally found to lead to incoherent transport. For a single wire, we find that the resistance adds in series to the contact resistance of h/e^2 for spinless electrons, and the total resistance is independent of the Luttinger parameter K_W of the wire. We numerically solve the bosonic equations to illustrate what happens when a charge density pulse is incident on the wire; the results depend on the parameters of the resistive and interacting regions in interesting ways. For a junction of Tomonaga-Luttinger liquid wires, we use a dissipationless current splitting matrix to model the junction. For a junction of three wires connected to Fermi liquid leads, there are two families of such matrices; we find that the conductance matrix generally depends on K_W for one family but is independent of K_W for the other family, regardless of the resistances present in the system.
6 pages, 3 figures; added a discussion of time reversal invariance; this is the published version
References in corpus (6)
- Junctions of anyonic Luttinger wires
- Junctions of three quantum wires for spin 1/2 electrons
- Frustration of decoherence in -shaped superconducting Josephson networks
- Resistivity of inhomogeneous quantum wires
- Line junction in a quantum Hall system with two filling fractions
- Electronic transport in inhomogeneous quantum wires