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

Quantum Numbers02:43

Quantum Numbers

It is said that the energy of an electron in an atom is quantized; that is, it can be equal only to certain specific values and can jump from one energy level to another but not transition smoothly or stay between these levels.
Atomic Radii and Effective Nuclear Charge03:08

Atomic Radii and Effective Nuclear Charge

The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
First Law: Particles in Two-dimensional Equilibrium01:18

First Law: Particles in Two-dimensional Equilibrium

Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
Newton's first law tells us about the...
Atomic Number and Mass Number01:12

Atomic Number and Mass Number

The number of protons in the nucleus of an atom is its atomic number (Z). This is the defining trait of an element. Its value determines the identity of the atom. For example, any atom that contains six protons is the element carbon and has the atomic number 6, regardless of how many neutrons or electrons it may have. A neutral atom must contain the same number of positive and negative charges, so the number of protons equals the number of electrons. This means that the atomic number also...
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,...
Fermi Level Dynamics01:12

Fermi Level Dynamics

The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...

You might also read

Related Articles

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

Sort by
Same author

Emergence of intrinsic superconductivity below 1.178 K in the topologically non-trivial semimetal state of CaSn<sub>3</sub>.

Journal of physics. Condensed matter : an Institute of Physics journal·2019
Same author

Electrostatic tuning of the proximity-induced exchange field in EuS/Al bilayers.

Physical review letters·2013
Same author

Exchange field-mediated magnetoresistance in the correlated insulator phase of Be films.

Physical review letters·2012
Same author

Origin of excess low-energy states in a disordered superconductor in a Zeeman field.

Physical review letters·2011
Same author

Spin-resolved tunneling studies of the exchange field in EuS/Al bilayers.

Physical review letters·2011
Same author

Crystal growth, structure, and physical properties of Ln(Ag, Al, Si)₂ (Ln = Ce and Gd).

Journal of physics. Condensed matter : an Institute of Physics journal·2011

Related Experiment Video

Updated: May 10, 2026

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles
10:00

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles

Published on: July 5, 2016

Quantum metallicity in a two-dimensional insulator.

V Y Butko1, P W Adams

  • 1Department of Physics and Astronomy, Louisiana State University, Baton Rouge 70803, USA.

Nature
|February 24, 2001
PubMed
Summary

Strongly disordered beryllium films transition from insulator to a quantum metal phase when a magnetic field suppresses the Coulomb gap. This reveals new insights into electron interactions in disordered systems.

Area of Science:

  • Condensed-matter physics
  • Quantum mechanics
  • Materials science

Background:

  • Electron interactions and correlations significantly impact electronic properties in disordered 2D systems.
  • Disorder enhances interaction effects, typically causing a depletion in the density of electronic states, forming a 'Coulomb gap' in strongly disordered materials.
  • This Coulomb gap can transform metallic films into insulators, but their properties remain poorly understood.

Purpose of the Study:

  • To investigate the electronic properties of disordered beryllium films.
  • To differentiate the effects of the Coulomb gap from underlying disorder.
  • To understand the transition to a low-temperature metallic phase.

Main Methods:

  • Experimental investigation of disordered beryllium films.

More Related Videos

High Resolution Physical Characterization of Single Metallic Nanoparticles
09:56

High Resolution Physical Characterization of Single Metallic Nanoparticles

Published on: June 28, 2019

In Situ Measurement of Vacuum Window Birefringence using 25Mg+ Fluorescence
07:03

In Situ Measurement of Vacuum Window Birefringence using 25Mg+ Fluorescence

Published on: June 13, 2020

Related Experiment Videos

Last Updated: May 10, 2026

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles
10:00

Energy Dispersive X-ray Tomography for 3D Elemental Mapping of Individual Nanoparticles

Published on: July 5, 2016

High Resolution Physical Characterization of Single Metallic Nanoparticles
09:56

High Resolution Physical Characterization of Single Metallic Nanoparticles

Published on: June 28, 2019

In Situ Measurement of Vacuum Window Birefringence using 25Mg+ Fluorescence
07:03

In Situ Measurement of Vacuum Window Birefringence using 25Mg+ Fluorescence

Published on: June 13, 2020

  • Application of magnetic fields to observe changes in electronic properties.
  • Measurement of electrical resistance.
  • Main Results:

    • The Coulomb gap in beryllium films is suppressed by a magnetic field.
    • Strongly insulating beryllium films transition into a quantum metal phase at low temperatures.
    • The resistance in this quantum metal phase approaches the quantum resistance (RQ = h/e2).

    Conclusions:

    • Magnetic fields can suppress the Coulomb gap, altering the electronic state of disordered materials.
    • Disordered beryllium films exhibit a field-induced transition to a quantum metal state.
    • This study provides a clearer understanding of electron correlation effects in disordered systems and the nature of the Coulomb gap.