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Related Concept Videos

The Hall Effect01:30

The Hall Effect

Edwin H. Hall, in the year 1879, devised an experiment that could be used to identify the polarity of the predominant charge carriers in a conducting material. From a historical perspective, this experiment was the first to demonstrate that the charge carriers in most metals are negative.
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

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.
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Energy Bands in Solids01:01

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Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
 Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states that no two...
Types of Semiconductors01:20

Types of Semiconductors

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...

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Related Experiment Video

Updated: Jul 13, 2026

All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
11:33

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Integer quantum Hall effect on a six-valley hydrogen-passivated silicon (111) surface.

K Eng1, R N McFarland, B E Kane

  • 1Laboratory for Physical Sciences, University of Maryland at College Park, College Park, Maryland 20740, USA.

Physical Review Letters
|August 7, 2007
PubMed
Summary

Magnetotransport studies reveal broken valley degeneracy in a two-dimensional electron system on hydrogen-passivated Si(111). This leads to unequal valley occupation and resistance anisotropy, challenging noninteracting electron theories.

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Area of Science:

  • Condensed matter physics
  • Surface science
  • Materials science

Background:

  • Two-dimensional electron systems (2DES) are crucial for understanding quantum phenomena.
  • The Si(111) surface offers a unique platform for creating 2DES at the interface with vacuum.
  • Valley degeneracy in such systems is typically expected to be sixfold.

Purpose of the Study:

  • Investigate magnetotransport properties of a 2DES at a hydrogen-passivated Si(111)-vacuum interface.
  • Determine the valley occupation and its effect on electronic properties.
  • Explore the implications for theoretical models of quantum Hall effects.

Main Methods:

  • Magnetotransport measurements were performed.
  • Studies were conducted in the integer quantum Hall regime.
  • The two-dimensional electron system was formed in an inversion layer.

Main Results:

  • The expected sixfold valley degeneracy was found to be broken.
  • Unequal occupation of the six valleys was observed.
  • Anisotropy in electrical resistance was detected, correlating with valley occupation.

Conclusions:

  • Surface misorientation likely breaks valley states into unequally spaced pairs.
  • Observed odd filling factors present a challenge to noninteracting electron theories.
  • Further theoretical and experimental investigation is needed to fully explain the findings.