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Related Concept Videos

Semiconductors01:22

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.
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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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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Superconductor01:24

Superconductor

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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...
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Types Of Superconductors01:28

Types Of Superconductors

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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...
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Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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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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Valence Bond Theory02:42

Valence Bond Theory

10.5K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
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Related Experiment Video

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All-electronic Nanosecond-resolved Scanning Tunneling Microscopy: Facilitating the Investigation of Single Dopant Charge Dynamics
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Superconductivity in a Hole-Doped Mott-Insulating Triangular Adatom Layer on a Silicon Surface.

Xuefeng Wu1, Fangfei Ming2, Tyler S Smith3

  • 1Department of Physics, Southern University of Science and Technology, Shenzhen, Guangdong 518055, China.

Physical Review Letters
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Superconductivity was discovered in a two-dimensional triangular lattice of tin (Sn) atoms on silicon (Si). This novel finding in a Mott insulator system opens new avenues for exploring unconventional superconductivity in low-dimensional materials.

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Area of Science:

  • Surface Science
  • Condensed Matter Physics
  • Materials Science

Background:

  • A two-dimensional triangular lattice of tin (Sn) adatoms on a silicon (Si) substrate forms a Mott insulator with unpaired electrons.
  • Modulation doping of this system with heavily doped p-type Si(111) substrates can induce metallicity.

Purpose of the Study:

  • To investigate the superconducting properties of hole-doped Sn adatom layers on degenerately doped p-type Si(111).
  • To explore the nature of superconductivity in this dilute, two-dimensional system.

Main Methods:

  • Fabrication of a two-dimensional triangular adatom lattice of Sn on Si(111).
  • Hole doping using degenerately doped p-type Si(111) substrates.
  • Measurement of superconducting critical temperature (Tc).

Main Results:

  • The hole-doped Sn adatom layer exhibits superconductivity with a critical temperature of 4.7±0.3 K.
  • The observed superconductivity occurs in a system with Mott correlations.

Conclusions:

  • The discovered superconductivity in the Sn/Si(111) system, a Mott insulator, suggests potentially unconventional pairing mechanisms.
  • While phonon-mediated coupling is plausible, Mott correlations may influence the s-wave pairing channel, indicating a departure from conventional BCS theory.