Superconducting coherence length

In superconductivity, the superconducting coherence length, usually denoted as ${\displaystyle \xi }$ (Greek lowercase xi), is the characteristic exponent of the variations of the density of superconducting component.

The superconducting coherence length is one of two parameters in the Ginzburg–Landau theory of superconductivity. It is given by:[1]

${\displaystyle \xi ={\sqrt {\frac {\hbar ^{2}}{2m|\alpha |}}}}$

where ${\displaystyle \alpha }$ is a constant in the Ginzburg–Landau equation for ${\displaystyle \psi }$ with the form ${\displaystyle \alpha _{0}(T-T_{c})}$.

In Landau mean-field theory, at temperatures T near the superconducting critical temperature T_c , ξ(T) ∝ (1-T/T_c)^−1/2. Up to a factor of ${\displaystyle {\sqrt {2}}}$, it is equivalent characteristic exponent describing a recovery of the order parameter away from a perturbation in the theory of the second order phase transitions.

In some special limiting cases, for example in the weak-coupling BCS theory of isotropic s-wave superconductor it is related to characteristic Cooper pair size:[2]

${\displaystyle \xi _{BCS}={\frac {\hbar v_{f}}{\pi \Delta }}}$

where ${\displaystyle \hbar }$ is the reduced Planck constant, ${\displaystyle m}$ is the mass of a Cooper pair (twice the electron mass), ${\displaystyle v_{f}}$ is the Fermi velocity, and ${\displaystyle \Delta }$ is the superconducting energy gap. The superconducting coherence length is a measure of the size of a Cooper pair (distance between the two electrons) and is of the order of ${\displaystyle 10^{-4}}$ cm. The electron near or at the Fermi surface moving through the lattice of a metal produces behind itself an attractive potential of range of the order of ${\displaystyle 3\times 10^{-6}}$ cm, the lattice distance being of order ${\displaystyle 10^{-8}}$ cm. For a very authoritative explanation based on physical intuition see the CERN article by V.F. Weisskopf.[3]

The ratio ${\displaystyle \kappa =\lambda /\xi }$, where ${\displaystyle \lambda }$ is the London penetration depth, is known as the Ginzburg–Landau parameter. Type-I superconductors are those with ${\displaystyle 0<\kappa <1/{\sqrt {2}}}$, and type-II superconductors are those with ${\displaystyle \kappa >1/{\sqrt {2}}}$.

In strong-coupling, anisotropic and multi-component theories these expressions are modified.[4]

See also

• Ginzburg–Landau theory of superconductivity
• BCS theory of superconductivity
• London penetration depth

References

1. Tinkham, M. (1996). Introduction to Superconductivity, Second Edition. New York, NY: McGraw-Hill. ISBN 0486435032.
2. Annett, James (2004). Superconductivity, Superfluids and Condensates. New York: Oxford university press. p. 62. ISBN 978-0-19-850756-7.
3. Victor F. Weisskopf (1979). The Formation of Cooper Pairs and the Nature of Superconducting Currents, CERN 79-12 (Yellow Report), December 1979
4. "Superfluid States of Matter". CRC Press. Retrieved 2019-04-02.