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Related Concept Videos

Semiconductors01:22

Semiconductors

1.1K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.1K
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

651
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...
651
Band Theory02:35

Band Theory

16.4K
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
16.4K
Fermi Level Dynamics01:12

Fermi Level Dynamics

462
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...
462
Fermi Level01:18

Fermi Level

1.2K
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,...
1.2K
Types of Semiconductors01:20

Types of Semiconductors

1.1K
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
1.1K

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Hall Coefficient of Semimetals.

Abhisek Samanta1, Daniel P Arovas2, Assa Auerbach1

  • 1Physics Department, Technion, Haifa 32000, Israel.

Physical Review Letters
|March 5, 2021
PubMed
Summary

A new formula for the Hall coefficient is applied to semimetals and semiconductors. This reveals deviations from standard models linked to electronic band structures and Fermi surface topology.

Area of Science:

  • Condensed matter physics
  • Solid-state physics
  • Materials science

Background:

  • The Hall coefficient is a fundamental property in condensed matter physics.
  • Understanding its behavior in novel materials like semimetals is crucial.
  • Existing models may not fully capture complex electronic structures.

Purpose of the Study:

  • To apply a new Hall coefficient formula to various electronic systems.
  • To investigate deviations from conventional theories.
  • To link these deviations to specific material properties.

Main Methods:

  • Application of a recently developed Hall coefficient formula.
  • Analysis of nodal line and Weyl semimetals, including graphene.
  • Examination of spin-orbit split semiconductor bands in 2D and 3D.

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  • Reduction of calculations to a ratio of equilibrium susceptibilities.
  • Main Results:

    • The formula simplifies to a ratio of equilibrium susceptibilities under weak disorder.
    • Deviations from Drude's inverse carrier density are identified.
    • These deviations are correlated with band degeneracies, Fermi surface topology, and interband currents.

    Conclusions:

    • The new formula provides insights into the Hall coefficient of complex materials.
    • Deviations offer a probe into electronic band structure and topology.
    • Experimental verification of these predictions is proposed.