Superconducting coherence length explained

In superconductivity, the superconducting coherence length, usually denoted as

\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]

\xi=\sqrt{

\hbar2
2m|\alpha(T)|
}

where

\alpha(T)

is a parameter in the Ginzburg–Landau equation for

\psi

with the form

\alpha0(T-Tc)

, where

\alpha0

is a constant.

In Landau mean-field theory, at temperatures

T

near the superconducting critical temperature

Tc

,

\xi(T)\propto

-1
2
(1-T/T
c)
. Up to a factor of

\sqrt{2}

, it is equivalent to the 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]

\xiBCS=

\hbarvf
\pi\Delta

where

\hbar

is the reduced Planck constant,

m

is the mass of a Cooper pair (twice the electron mass),

vf

is the Fermi velocity, and

\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

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

3 x 10-6

cm, the lattice distance being of order

10-8

cm. For a very authoritative explanation based on physical intuition see the CERN article by V.F. Weisskopf.[3]

The ratio

\kappa=λ/\xi

, where

λ

is the London penetration depth, is known as the Ginzburg–Landau parameter. Type-I superconductors are those with

0<\kappa<1/\sqrt{2}

, and type-II superconductors are those with

\kappa>1/\sqrt{2}

.

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

Notes and References

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