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

Properties of Transition Metals02:58

Properties of Transition Metals

29.3K
Transition metals are defined as those elements that have partially filled d orbitals. As shown in Figure 1, the d-block elements in groups 3–12 are transition elements. The f-block elements, also called inner transition metals (the lanthanides and actinides), also meet this criterion because the d orbital is partially occupied before the f orbitals.
29.3K
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

1.7K
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,...
1.7K
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

511
Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
511
Ferromagnetism01:31

Ferromagnetism

2.9K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.9K
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

859
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
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...
859
Trends in Lattice Energy: Ion Size and Charge02:54

Trends in Lattice Energy: Ion Size and Charge

26.4K
An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
26.4K

You might also read

Related Articles

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

Sort by
Same author

Multisource Port Inspection Sensor Fusion with Causal Representation Learning for Cross-Border Anomaly Monitoring.

Sensors (Basel, Switzerland)·2026
Same author

Fabrication of atomically flat cleavage planes with ultrafast laser scribing.

Scientific reports·2026
Same author

Superconducting coherence boosted by outer-layer metallic screening in multilayered cuprates.

Nature communications·2026
Same author

Bound states in doped charge transfer insulators.

Nature communications·2026
Same author

Imaging Transmembrane Kinetics: An Asymmetric Phthalocyanine Enables Fast Cellular Entry and Golgi Targeting for Enhanced Photodynamic Therapy.

Journal of biophotonics·2026
Same author

Anion-Engineered Organic Electrochemical Transistors With Multi-Timescale Synaptic Dynamics for Task-Adaptive Spiking Neural Networks.

Small (Weinheim an der Bergstrasse, Germany)·2026

Related Experiment Video

Updated: Jan 6, 2026

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light
09:19

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light

Published on: July 29, 2013

11.9K

Disorder-driven non-Anderson transition in a Weyl semimetal.

Cong Li1, Yang Wang1, Jianfeng Zhang2

  • 1Department of Applied Physics, Kungliga Tekniska högskolan Royal Institute of Technology, Stockholm 11419, Sweden.

Proceedings of the National Academy of Sciences of the United States of America
|October 9, 2025
PubMed
Summary

Researchers experimentally observed a novel quantum phase transition driven by disorder in the Weyl semimetal NdAlSi. This non-Anderson transition suppresses topological surface states, providing the first direct evidence of this theoretically predicted phenomenon.

Keywords:
ARPESWeyl semimetalelectronic structurenon-Anderson transition

More Related Videos

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers
12:20

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers

Published on: October 5, 2013

15.0K
Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

8.5K

Related Experiment Videos

Last Updated: Jan 6, 2026

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light
09:19

Fabrication and Characterization of Disordered Polymer Optical Fibers for Transverse Anderson Localization of Light

Published on: July 29, 2013

11.9K
Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers
12:20

Sputter Growth and Characterization of Metamagnetic B2-ordered FeRh Epilayers

Published on: October 5, 2013

15.0K
Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope
09:06

Visualizing Uniaxial-strain Manipulation of Antiferromagnetic Domains in Fe1+YTe Using a Spin-polarized Scanning Tunneling Microscope

Published on: March 24, 2019

8.5K

Area of Science:

  • Condensed Matter Physics
  • Quantum Materials Science

Background:

  • A long-standing belief held that disordered electronic systems only exhibit Anderson localization-driven metal-insulator transitions.
  • Recent theories predict a distinct disorder-driven non-Anderson phase transition, but experimental evidence has been lacking.

Purpose of the Study:

  • To experimentally demonstrate and characterize the disorder-driven non-Anderson phase transition.
  • To visualize the electronic structure changes in a Weyl semimetal under varying disorder levels.

Main Methods:

  • Utilized angle-resolved photoemission spectroscopy (ARPES) to probe the electronic structure.
  • Investigated the Weyl semimetal NdAlSi with controlled surface disorder.

Main Results:

  • Observed suppression of all surface states, including topological Fermi arcs, in NdAlSi with increasing disorder.
  • Linked the disappearance of Fermi arcs to the vanishing of the topological invariant.
  • Identified a quantum phase transition from a Weyl semimetal to a diffusive metal.

Conclusions:

  • Provided the first direct experimental evidence of a non-Anderson disorder-driven quantum phase transition.
  • Confirmed theoretical predictions of a novel phase transition mechanism in quantum systems.
  • Highlighted the role of disorder in fundamentally altering topological properties of semimetals.