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Related Concept Videos

Semiconductors01:22

Semiconductors

1.9K
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...
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Quantum Numbers02:43

Quantum Numbers

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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.
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The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

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Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
61.6K
Types of Semiconductors01:20

Types of Semiconductors

1.8K
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...
1.8K
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

1.3K
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...
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Ampere-Maxwell's Law: Problem-Solving01:17

Ampere-Maxwell's Law: Problem-Solving

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A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
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Silicon Metal-oxide-semiconductor Quantum Dots for Single-electron Pumping
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A surface code quantum computer in silicon.

Charles D Hill1, Eldad Peretz2, Samuel J Hile2

  • 1Centre for Quantum Computation and Communication Technology, School of Physics, University of Melbourne, Victoria 3010, Australia.

Science Advances
|November 25, 2015
PubMed
Summary
This summary is machine-generated.

This study introduces a novel silicon quantum computing architecture using phosphorus donor nuclear spins. It enables parallel qubit operations for error correction, overcoming fabrication and control challenges for scalable quantum computers.

Keywords:
Donors in siliconSilicon quantum computingSpin qubits

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Area of Science:

  • Quantum computing
  • Solid-state physics
  • Nanotechnology

Background:

  • Silicon-based quantum computing offers long coherence times and scalability.
  • Topological quantum error correction requires 2D qubit arrays, posing fabrication and control challenges.
  • Existing architectures struggle with the complexity of independent qubit control.

Purpose of the Study:

  • To present a novel architecture for scalable quantum information processing in silicon.
  • To address the challenges of fabricating and controlling 2D qubit arrays for quantum error correction.
  • To leverage the uniformity of phosphorus donor nuclear spin qubits for efficient control.

Main Methods:

  • A shared-control paradigm utilizing a 2D lattice of phosphorus donor qubits.
  • A crisscross gate array architecture with vertically separated control layers.
  • Global spin control for activating multiple qubits in parallel for surface code operations.

Main Results:

  • The proposed architecture simplifies control by avoiding independent qubit manipulation and complex interconnects.
  • Simulated quantum operations are demonstrated to be below the surface code error threshold.
  • The design is compatible with demonstrated fabrication and control techniques.

Conclusions:

  • The architecture offers a new pathway for large-scale quantum information processing in silicon.
  • The shared-control approach effectively exploits the uniformity of phosphorus donor qubits.
  • This design paves the way for building fault-tolerant quantum computers.