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Related Concept Videos

Semiconductors01:22

Semiconductors

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...
Types Of Superconductors01:28

Types Of Superconductors

A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
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.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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 semiconductor's...
Superconductor01:24

Superconductor

A substance that reaches superconductivity, a state in which magnetic fields cannot penetrate, and there is no electrical resistance, is referred to as a superconductor. In 1911, Heike Kamerlingh Onnes of Leiden University, a Dutch physicist, observed a relation between the temperature and the resistance of the element mercury. The mercury sample was then cooled in liquid helium to study the linear dependence of resistance on temperature. It was observed that, as the temperature decreased, the...
Theory of Metallic Conduction01:17

Theory of Metallic Conduction

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,...

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Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
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Soft superconducting gap in semiconductor Majorana nanowires.

So Takei1, Benjamin M Fregoso, Hoi-Yin Hui

  • 1Department of Physics, Condensed Matter Theory Center and Joint Quantum Institute, University of Maryland, College Park, Maryland 20742-4111, USA.

Physical Review Letters
|May 21, 2013
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The soft gap in semiconductor-superconductor devices, potentially indicating Majorana bound states, is likely caused by interface inhomogeneity and dissipation. Improving interface quality could lead to a harder induced gap, crucial for future research.

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Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Quantum Computing

Background:

  • Semiconductor-superconductor hybrid structures are key for exploring exotic quantum phenomena.
  • The presence of a soft gap in tunneling conductance measurements has been a puzzle.
  • This soft gap has been linked to potential signatures of Majorana bound states.

Purpose of the Study:

  • To theoretically investigate the origins of the soft gap in semiconductor-superconductor hybrid structures.
  • To determine the most plausible mechanism responsible for the observed soft gap.
  • To provide guidance for optimizing material interfaces for future experiments.

Main Methods:

  • Theoretical modeling of tunneling conductance.
  • Systematic analysis of various contributing factors: magnetic/nonmagnetic disorder, temperature, dissipative Cooper pair breaking, and interface inhomogeneity.
  • Comparison of theoretical predictions with experimental observations.

Main Results:

  • Disorder, temperature, and dissipative Cooper pair breaking alone do not fully explain the soft gap.
  • Interface inhomogeneity, combined with moderate dissipation, emerges as the most consistent explanation for the soft gap.
  • The study identifies specific parameters that influence the gap's characteristics.

Conclusions:

  • Interface inhomogeneity and dissipation are identified as the primary drivers of the soft gap in these systems.
  • Enhancing the quality and uniformity of the superconductor-semiconductor interface is critical.
  • Future efforts should focus on interface engineering to achieve harder induced gaps, potentially improving the search for Majorana bound states.