Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Duality at a B=0 metal-insulator transition in two dimensions

D. Simonian, S. V. Kravchenko, Myriam P. Sarachik

Published Nov 19, 1996• 0 citations
OpenAlex

Related papers

Metal–insulator transition in two dimensions

V. M. Pudalov, Gerhard Brunthaler, A. Prinz +1 more

Physica E Low-dimensional Systems and Nanostructures•Oct 1, 1998•48 citations

Flow diagram of the metal–insulator transition in two dimensions

S. Anissimova, S. V. Kravchenko, Alexander Punnoose +2 more

arXiv:cond-mat/0609181•Nature Physics•Aug 5, 2007•94 citations

Critical properties of metal-insulator transition in low dimensions

Masatoshi Imada

Journal of Low Temperature Physics•May 1, 1995•5 citations

The Mott-Hubbard metal-insulator transition in the limit of large dimensions—Insights and outlook

Stefan K. Kehrein

Advances in Solid State Physics•Nov 10, 2007•0 citations

Three-dimensional network model for strong topological insulator transitions

Jun Ho Son, S. Raghu

We construct a three-dimensional (3D), time-reversal symmetric generalization of the Chalker-Coddington network model for the integer quantum Hall transition. In addition to a weak topological insulator phase already accommodated by the network model framework in the preexisting literature, our network model hosts strong topological insulator phases. We unambiguously demonstrate that strong topological insulator phases emerge as intermediate phases between a trivial insulator phase and a weak topological phase. Additionally, we found a duality that relates a trivial insulator phase and a weak topological phase in our network model. Remarkably, strong topological phases are mapped to themselves under this duality. We show that upon adding sufficiently strong disorder, the strong topological insulator phases undergo phase transitions into a metallic phase. We numerically determine the critical exponent of the insulator-metal transition. Our network model explicitly shows how a semiclassical percolation picture of topological phase transitions in two dimensions can be generalized to 3D and opens up a venue for studying 3D topological phase transitions.

arXiv:2008.03315•Physical review. B./Physical review. B•Sep 27, 2021•4 citations

Metal—insulator transition in one-dimensional metals

H. Heyszenau

Solid State Communications•Jan 1, 1976•3 citations
We construct a three-dimensional (3D), time-reversal symmetric generalization of the Chalker-Coddington network model for the integer quantum Hall transition. In addition to a weak topological insulator phase already accommodated by the network model framework in the preexisting literature, our network model hosts strong topological insulator phases. We unambiguously demonstrate that strong topological insulator phases emerge as intermediate phases between a trivial insulator phase and a weak topological phase. Additionally, we found a duality that relates a trivial insulator phase and a weak topological phase in our network model. Remarkably, strong topological phases are mapped to themselves under this duality. We show that upon adding sufficiently strong disorder, the strong topological insulator phases undergo phase transitions into a metallic phase. We numerically determine the critical exponent of the insulator-metal transition. Our network model explicitly shows how a semiclassical percolation picture of topological phase transitions in two dimensions can be generalized to 3D and opens up a venue for studying 3D topological phase transitions.