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

Bulletin of the American Physical Society

Critical Behavior of a Strongly-Interacting 2D Electron System

Myriam P. Sarachik

Published Mar 18, 2013• 0 citations
OpenAlex

Related papers

Collective motion of electrons in a strongly interacting 2D electron system

Pedro Brussarski, S. Li, S. V. Kravchenko +2 more

•Apr 14, 2017•0 citations

Spectroscopy of emergent states in strongly interacting 2D electron systems

Cyrus F. Hirjibehedin

•Jan 1, 2004•0 citations

Critical behavior of the Pauli spin susceptibility in a strongly correlated 2D electron liquid

A. A. Shashkin, S. Anissimova, Mohammed R. Sakr +3 more

•Sep 6, 2004•0 citations

Metallic state in a strongly interacting spinless two-valley electron system in 2D

S. V. Kravchenko

•Apr 23, 2019•0 citations

Two-dimensional Ising criticality in interacting electron systems

Hiromi Otsuka, Masaaki Nakamura

Physica B Condensed Matter•Mar 1, 2005•0 citations

Critical Behavior of a Strongly Interacting 2D Electron System

A. Mokashi, Shiqi Li, B. Wen +4 more

With decreasing density n(s) the thermopower S of a low-disorder two-dimensional electron system in silicon is found to exhibit a sharp increase by more than an order of magnitude tending to a divergence at a finite disorder-independent density n(t) consistent with the critical form (-T/S) is proportional to (n(s)-n(t))(x) with x=1.0±0.1 (T is the temperature). Our results provide clear evidence for an interaction-induced transition to a new phase at low density in a strongly interacting 2D electron system.

arXiv:1111.7238•Physical Review Letters•Aug 28, 2012•60 citations
With decreasing density n(s) the thermopower S of a low-disorder two-dimensional electron system in silicon is found to exhibit a sharp increase by more than an order of magnitude tending to a divergence at a finite disorder-independent density n(t) consistent with the critical form (-T/S) is proportional to (n(s)-n(t))(x) with x=1.0±0.1 (T is the temperature). Our results provide clear evidence for an interaction-induced transition to a new phase at low density in a strongly interacting 2D electron system.