Module 7: High temperature Superconductors
  Discovery of High Temperature Superconductivity
 


7.5 Discovery of High Temperature Superconductivity

In 1986, 75 years after the discovery of superconductivity, George Bednorz and Karl Müller at IBM, Zurich demonstrated superconductivity in a perovskite structured lanthanum based cuprate oxide which showed a
TC of 35 K for which the inventors also won Physical Noble prize in 1987. This was a remarkable discovery as it later allowed chemical substitution in perovskite cuprates to push the transition temperatures well beyond the liquid nitrogen temperature (77 K) which is a much cheaper and easily accessible medium as compared to liquid helium.

This was realized by replacement of La by Y to give rise to YBa2Cu3O7-x(YBCO) which showed aTC of  ~92 K as first shown by Wu and his students at University of Alabama, Huntsville in 1987. The materials show highest TC when the materials are slightly oxygen deficient i.e. when x = 0.15. Superconductivity disappears at x ≈ 0.6, when structure of YBCO changes from orthorhombic to tetragonal.

Subsequently many other oxides such as thallium and mercury based oxide compounds showed even higher transition temperatures and these are usually called as type-II superconductors.

A list of important oxide superconductors is shown below with their structures and transition temperatures. If you recall, some of these structures were shown in Module 1. As you can see that critical temperature is dependent very strongly on how the chemical substitutions are made into the parent structure.
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Compound

Tc (K)

Crystal structure

Y-based

YBa2Cu3O7

92

Orthorhombic

Bi-based

Bi2Sr2CuO6

20

Tetragonal

Bi2Sr2CaCu2O8

85

Tetragonal

Bi2Sr2Ca2Cu3O6

110

Tetragonal

Tl-based

Tl2Ba2CuO6

84

Tetragonal

Tl2Ba2CaCu2O8

108

Tetragonal

Tl2Ba2Ca2Cu3O10

125

Tetragonal

TlBa2Ca3Cu4O11

122

Tetragonal

Hg-based

HgBa2CuO4

94

Tetragonal

HgBa2CaCu2O6

128

Tetragonal

HgBa2Ca2Cu3O8

134

Tetragonal