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Semiconductors

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There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
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The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
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Biasing of Metal-Semiconductor Junctions

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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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In most substances, the current flow is proportional to the voltage applied to it. A simple relationship between the values of current, voltage, and resistance is known as Ohm's law. Nonohmic devices do not exhibit a linear relationship between voltage and current. One such device is the semiconducting circuit element known as a diode. A diode is a circuit device that allows current flow in only one direction.
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Types of Semiconductors01:20

Types of Semiconductors

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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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Voltage Dividers01:14

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In electrical circuits, resistors can be connected in series, sequentially linked one after the other. In a series configuration, the same current flows through each resistor. Ohm's law is a fundamental principle to understand the behavior of resistors in series. It expresses the voltage across these resistors in terms of the current and resistance.
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Valley splitting in a silicon quantum device platform.

Jill A Miwa1, Oliver Warschkow, Damien J Carter

  • 1Department of Physics and Astronomy, Interdisciplinary Nanoscience Center (iNANO), University of Aarhus , 8000 Aarhus C, Denmark.

Nano Letters
|February 28, 2014
PubMed
Summary
This summary is machine-generated.

Researchers measured the valley splitting in silicon

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Area of Science:

  • Solid State Physics
  • Materials Science
  • Quantum Mechanics

Background:

  • A buried two-dimensional electron gas (2DEG) in silicon is formed by an atomically sharp phosphorus dopant profile (a δ-layer).
  • The valley splitting of the 2DEG's most occupied bands (1Γ and 2Γ) is crucial for device properties but has been difficult to measure.
  • Surface Umklapp processes can obscure measurements of this valley splitting.

Purpose of the Study:

  • To directly measure the valley splitting of the 1Γ and 2Γ states in a silicon δ-layer 2DEG.
  • To experimentally verify theoretical calculations of the 2DEG band structure.
  • To investigate the impact of suppressing surface Umklapp processes.

Main Methods:

  • Utilized direct spectroscopic measurements.
  • Employed Density Functional Theory (DFT) for band structure calculations.
  • Suppressed undesirable surface Umklapp processes to enable measurement.

Main Results:

  • Achieved good qualitative agreement between experimental measurements and DFT calculations.
  • Determined a valley splitting of 132 ± 5 meV for the 2DEG states.
  • Reported effective mass, occupation, and compared dispersions and Fermi surface with DFT.

Conclusions:

  • Direct measurement of valley splitting in silicon δ-layer 2DEG is now possible.
  • The study provides experimental validation for DFT calculations in this system.
  • Understanding valley splitting is key for advancing silicon-based quantum devices.