Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Fermi Level01:18

Fermi Level

The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
Atomic Nuclei: Nuclear Spin State Population Distribution01:14

Atomic Nuclei: Nuclear Spin State Population Distribution

Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
Phase Transitions: Melting and Freezing02:39

Phase Transitions: Melting and Freezing

Heating a crystalline solid increases the average energy of its atoms, molecules, or ions, and the solid gets hotter. At some point, the added energy becomes large enough to partially overcome the forces holding the molecules or ions of the solid in their fixed positions, and the solid begins the process of transitioning to the liquid state or melting. At this point, the temperature of the solid stops rising, despite the continual input of heat, and it remains constant until all of the solid is...
Phase Transitions: Sublimation and Deposition02:33

Phase Transitions: Sublimation and Deposition

Some solids can transition directly into the gaseous state, bypassing the liquid state, via a process known as sublimation. At room temperature and standard pressure, a piece of dry ice (solid CO2) sublimes, appearing to gradually disappear without ever forming any liquid. Snow and ice sublimate at temperatures below the melting point of water, a slow process that may be accelerated by winds and the reduced atmospheric pressures at high altitudes. When solid iodine is warmed, the solid sublimes...
Imperfections in Crystal Structure: Stoichiometric Point Defects01:26

Imperfections in Crystal Structure: Stoichiometric Point Defects

Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

The conduction of free electrons inside a conductor is best described by quantum mechanics. However, a classical model makes predictions close to the results of quantum mechanics. It is called the 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,...

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Letter to the editor: Efficacy of gabapentin and pregabalin for the treatment of neurogenic claudication in lumbar spinal stenosis: a double-blind randomized placebo-controlled trial.

Asian spine journal·2026
Same author

Electron Viscosity and Device-Dependent Variability in Four-Probe Electrical Transport in Ultraclean Graphene Field-Effect Transistors.

Nano letters·2026
Same author

Thermal conductivity modulation as a mechanism of inducible thermotolerance in the eutardigrade Paramacrobiotus sp.

Journal of the Royal Society, Interface·2026
Same author

Comparative Performance of Seven Mainstream Large Language Models on the 2022 American College of Radiology Diagnostic Imaging In-Training Examination.

Cureus·2026
Same author

Dual Implementation of Phrenic and Hypoglossal Nerve Stimulators in a Patient With Obstructive and Central Sleep Apnea and Associated Cardiac Arrhythmias.

Cureus·2026
Same author

Linking hypertension and TyG-WC circumference index among Indian adults: A cross-sectional study.

Bioinformation·2026

Related Experiment Video

Updated: Jul 7, 2026

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures
08:53

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures

Published on: October 9, 2012

Low-temperature collapse of electron localization in two dimensions.

Matthias Baenninger1, Arindam Ghosh, Michael Pepper

  • 1Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. matthias.baenninger@cantab.net

Physical Review Letters
|February 1, 2008
PubMed
Summary

The insulating phase of two-dimensional electron systems becomes unstable at low temperatures, transitioning to metal-like behavior. This occurs even at high resistivity, challenging previous understandings of electron transport.

More Related Videos

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
10:36

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials

Published on: January 21, 2016

Related Experiment Videos

Last Updated: Jul 7, 2026

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures
08:53

Angle-resolved Photoemission Spectroscopy At Ultra-low Temperatures

Published on: October 9, 2012

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving
11:21

Cooling an Optically Trapped Ultracold Fermi Gas by Periodical Driving

Published on: March 30, 2017

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials
10:36

Advanced Experimental Methods for Low-temperature Magnetotransport Measurement of Novel Materials

Published on: January 21, 2016

Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Phenomena

Background:

  • Disordered two-dimensional electron systems (2DES) often exhibit insulating behavior at low temperatures.
  • Strong electron-electron interactions complicate the understanding of transport properties in these systems.
  • The interplay between disorder, interactions, and temperature is crucial for determining electronic phase transitions.

Purpose of the Study:

  • To experimentally investigate the stability of the insulating phase in a disordered, strongly interacting 2D electron system.
  • To determine the temperature dependence of transport behavior in such systems.
  • To explore the influence of varying disorder strength on the observed electronic transitions.

Main Methods:

  • Transport measurements were conducted on a mesoscopic length scale.
  • Systematic variation of the disorder strength was employed.
  • Temperature was systematically decreased to observe changes in resistivity and transport characteristics.

Main Results:

  • Direct experimental evidence shows the insulating phase becomes unstable at low temperatures.
  • A transition from insulating to metal-like transport behavior was observed as temperature decreased.
  • This transition persisted even when resistivity significantly exceeded the quantum of resistivity (h/e²).

Conclusions:

  • The insulating state in disordered, strongly interacting 2D electron systems is not always stable at low temperatures.
  • Metal-like transport can emerge under conditions previously thought to be exclusively insulating.
  • These findings necessitate a re-evaluation of theories describing electron transport in disordered quantum systems.