Abstract

We study the conductance of a spinless non-interacting electron system consisting of randomly coupled N R right-moving channels and N L left-moving channels. This system serves as a model of disordered quantum wires with unitary symmetry. We focus on the case of N R = 1 with an arbitrary N L . In this case, the dimensionless conductance g for the left-moving channels is by m ≡ N L -1 greater than the dimensionless conductance g ' for the right-moving channels due to the presence of m perfectly conducting channels. That is, g = g '+ m . Using a superspin approach, we obtain the average and second moment of g ' as a function of wire length L . The resulting asymptotic forms in the long- L regime are consistent with those obtained from the existing scaling theory.

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.