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

Metal-insulator transitions and low energy states in low dimensional strongly correlated systems

Masatoshi Imada, 今田 正俊

Published Jan 1, 1995• 0 citations
OpenAlex

Related papers

Metal-Insulator Transitions in Strongly Correlated Systems

Masatoshi Imada

Springer proceedings in physics•Jan 1, 1998•0 citations

Filling dependence of correlation exponents and metal-Mott insulator transition in strongly correlated electron systems

Ming-Xi Lin, SHeng-Wen Qi

Using a universal relation between electron filling factor and ground state energy, this paper studies the dependence of correlation exponents on the electron filling factor of one-dimensional extended Hubbard model in a strong coupling regime, and demonstrates that in contrast to the usual Hubbard model ( g c = 1/2), the dimensionless coupling strength parameter g c heavily depends on the electron filling, and it has a "particle-hole" symmetry about electron quarter filling point. As increasing the nearest neighbouring repulsive interaction, the single particle spectral weight is transferred from low energy to high energy regimes. Moreover, at electron quarter filling, there is a metal-Mott insulator transition at the strong coupling point g c = 1/4, and this transition is a continuous phase transition.

Chinese Physics B•Dec 1, 2010•0 citations

Chapter 5 Metal-Insulator Transition in Correlated Two-Dimensional Systems with Disorder

Dragana Popović

This chapter focuses on studies of the critical behavior of conductivity in two-dimensional electron systems (2DES) with different amounts and types of disorder as well as different ranges of Coulomb interactions, in order to identify possible universality classes of the 2D metal-insulator transition (MIT). It discusses the manifestations of glassiness in both low- and high-disorder samples. The chapter examines the critical region near the 2D MIT in particular on describing conductivity measurements that have demonstrated dynamical scaling, the main signature of the MIT as a quantum phase transition. It also focuses on experiments that probe the nature of the insulating state, as well as charge dynamics across the MIT, in both high- and low-disorder 2DESs. There is substantial evidence that in many materials near the MIT both strong electronic correlations and disorder play an important role, and thus their competition is expected to lead to glassy behavior of electrons, in analogy with other frustrated systems.

•May 25, 2017•2 citations

Metal-insulator transition in highly correlated systems

C. A. Büsser, E. V. Anda, Laura Urba +2 more

Journal of Magnetism and Magnetic Materials•Jan 1, 1998•2 citations

Metal-insulator transition in correlated systems: A new numerical approach

Daniel J. García, E. Miranda, K. Hallberg +1 more

Physica B Condensed Matter•Apr 23, 2007•8 citations

Critical Properties of the Mott Transition in the Hubbard Model

Goetz Moeller, Qimiao Si A, Gabriel Kotliar +1 more

We introduce a systematic low-energy approach to strongly correlated electron systems in infinite dimensions, and apply it to the problem of the correlation-induced metal-insulator transition in the half-filled Hubbard model. We determine the low-energy scaling functions of the metallic state, including the single-particle Green function and dynamical spin susceptibility, as well as thermodynamic properties and relate them to experimental data in transition metal oxides.

arXiv:cond-mat/9402047•Feb 10, 1994•0 citations
Using a universal relation between electron filling factor and ground state energy, this paper studies the dependence of correlation exponents on the electron filling factor of one-dimensional extended Hubbard model in a strong coupling regime, and demonstrates that in contrast to the usual Hubbard model ( g c = 1/2), the dimensionless coupling strength parameter g c heavily depends on the electron filling, and it has a "particle-hole" symmetry about electron quarter filling point. As increasing the nearest neighbouring repulsive interaction, the single particle spectral weight is transferred from low energy to high energy regimes. Moreover, at electron quarter filling, there is a metal-Mott insulator transition at the strong coupling point g c = 1/4, and this transition is a continuous phase transition.
This chapter focuses on studies of the critical behavior of conductivity in two-dimensional electron systems (2DES) with different amounts and types of disorder as well as different ranges of Coulomb interactions, in order to identify possible universality classes of the 2D metal-insulator transition (MIT). It discusses the manifestations of glassiness in both low- and high-disorder samples. The chapter examines the critical region near the 2D MIT in particular on describing conductivity measurements that have demonstrated dynamical scaling, the main signature of the MIT as a quantum phase transition. It also focuses on experiments that probe the nature of the insulating state, as well as charge dynamics across the MIT, in both high- and low-disorder 2DESs. There is substantial evidence that in many materials near the MIT both strong electronic correlations and disorder play an important role, and thus their competition is expected to lead to glassy behavior of electrons, in analogy with other frustrated systems.