Related Experiment Video
Updated: Mar 28, 2026

Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
Nonergodic metallic and insulating phases of Josephson junction chains
Manuel Pino1, Lev B Ioffe2, Boris L Altshuler3
1Department of Physics and Astronomy, Rutgers, The State University of New Jersey, New Brunswick, NJ 08901;
Conventional statistical physics laws require a heat bath, but new research on Josephson junctions reveals a high-temperature nonergodic phase with finite resistance, challenging these foundations.
Area of Science:
- Statistical Physics
- Quantum Devices
- Condensed Matter Physics
Background:
- Conventional statistical physics relies on heat bath presence and ergodicity.
- Weak coupling to heat baths was assumed sufficient for real systems.
- Recent advances in quantum devices allow study of systems with reduced bath coupling.
Purpose of the Study:
- Revisit the foundations of statistical mechanics for systems with weak heat bath coupling.
- Investigate the behavior of Josephson junction chains under these conditions.
- Identify novel phases and properties in reduced-bath-coupling systems.
Main Methods:
- Theoretical examination of Josephson junction chains.
- Analysis of systems with dramatically reduced coupling to a heat bath.
- Investigating high-temperature nonergodic phases.
Main Results:
- A Josephson junction chain exhibits a novel high-temperature nonergodic phase with finite resistance.
- At higher temperatures, the system transitions to a fully localized state.
- This localized state is characterized by infinite resistance and long relaxation times.
Conclusions:
- The study challenges the universal applicability of conventional statistical mechanics.
- Novel nonergodic phases can emerge in systems with weak heat bath coupling.
- Josephson junction chains serve as a model system for exploring these phenomena.
Related Concept Videos
Theory of Metallic Conduction
In this theory, Newton's second law of motion is used to determine the acceleration of an electron in the presence of an applied electric field. Then, its velocity is expressed via this acceleration.
An electron moves through the crystal, containing positive ions,...
Metal-Semiconductor Junctions
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Biasing of Metal-Semiconductor Junctions
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Phase Transitions: Melting and Freezing
Types Of Superconductors
Phase Transitions

