Related Experiment Video
Updated: Feb 19, 2026

Orientational Transition in a Liquid Crystal Triggered by the Thermodynamic Growth of Interfacial Wetting Sheets
Published on: May 15, 2017
Insulating Josephson Junction Chains as Pinned Luttinger Liquids
Karin Cedergren1, Roger Ackroyd1, Sergey Kafanov1
1Centre for Engineered Quantum Systems (EQuS), School of Physics, University of New South Wales, Sydney 2052, Australia.
Disordered Josephson junction chains realize a Bose glass state, validating quantum many-body theory. This finding impacts the development of novel quantum devices and a fundamental current standard.
Area of Science:
- Condensed matter physics
- Quantum physics
Background:
- One-dimensional quantum systems exhibit rich physics, often described by Luttinger liquid theory.
- Theoretical proposals for Josephson junction chains exist, but experimental realization is limited, especially concerning disorder effects.
Purpose of the Study:
- To experimentally investigate the role of disorder in linear chains of Josephson junctions.
- To establish the nature of the insulating state in these systems and its theoretical underpinnings.
Main Methods:
- Fabrication and characterization of submicron Josephson junction chains.
- Experimental measurement of the insulating state properties.
Main Results:
- The insulating state is identified as a Luttinger liquid pinned by random offset charges.
- This system serves as a one-dimensional implementation of the Bose glass.
- The results validate quantum many-body theory for disordered one-dimensional systems.
Conclusions:
- Disorder in Josephson junction chains leads to a Bose glass state, confirming theoretical predictions.
- This understanding is crucial for advancing quantum phase slip-based current standards and novel quantum devices.
Related Concept Videos
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...
Molecular and Ionic Solids
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
P-N junction
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,...
Biasing of P-N Junction
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...

