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Related Concept Videos

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...
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Network Covalent Solids

Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
Types Of Superconductors01:28

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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...
Alkali Metals03:06

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Group 1 elements are soft and shiny metallic solids. They are malleable, ductile, and good conductors of heat and electricity. The melting points of the alkali metals are unusually low for metals and decrease going down the group, while the density increases going down the group with the exception of potassium (Table 1).
Table 1: Properties of the alkali metals
Semiconductors01:22

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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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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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Superconductivity in heavy alkaline-Earth intercalated graphites.

J S Kim1, L Boeri, J R O'Brien

  • 1Max-Planck-Institut für Festkörperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany.

Physical Review Letters
|August 7, 2007
PubMed
Summary

Superconductivity was discovered in strontium-intercalated graphite (SrC6) at 1.65 K. This finding, along with reduced anisotropy and an anisotropic gap, offers new insights into superconducting materials.

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Superconductivity

Background:

  • Alkaline earth metal-intercalated graphite compounds (AeC6) are known superconductors.
  • Calcium-intercalated graphite (CaC6) exhibits superconductivity with anisotropic properties.

Purpose of the Study:

  • To investigate the superconducting properties of strontium-intercalated graphite (SrC6).
  • To compare the superconductivity of SrC6 with CaC6 and understand the factors influencing critical temperature (Tc).

Main Methods:

  • Magnetic susceptibility measurements.
  • Specific heat (Cp) measurements.
  • Analysis of upper critical fields and superconducting gap anisotropy.

Main Results:

  • Superconductivity was observed in SrC6 below 1.65(6) K.
  • SrC6 showed significantly reduced anisotropy in upper critical fields compared to CaC6.
  • The specific heat anomaly at Tc was smaller than BCS predictions, indicating an anisotropic superconducting gap.

Conclusions:

  • The lower Tc in SrC6, compared to CaC6, is attributed to "negative" pressure effects reducing electron-phonon coupling.
  • SrC6 exhibits an anisotropic superconducting gap, similar to CaC6.
  • No superconductivity was observed in BaC6 down to 0.3 K.