# Ginzburg-Landau theory

In

physics,

**Ginzburg-Landau theory** is a mathematical theory used to model

superconductivity. It does not purport to explain the microscopic mechanisms giving rise to superconductivity. Instead, it examines the macroscopic properties of a superconductor with the aid of general

thermodynamic arguments.

Based on Landau's previously-established theory of second-order phase transitions, Landau and Ginzburg argued that the free energy *F* of a superconductor near the superconducting transition can be expressed in terms of a complex order parameter *ψ*, which describes how deep into the superconducting phase the system is. The free energy has the form

where

*F*_{n} is the free energy in the normal phase,

*α* and

*β* are phenomenological parameters,

**A** is the electromagnetic

vector potential, and

**H** is the magnetic field. By minimizing the free energy with respect to fluctuations in the order parameter and the vector potential, one arrives at the

**Ginzburg-Landau equations**

where

**J** denotes the electrical current. The first equation, which bears interesting similarities to the time-independent

Schrödinger equation, determines the order parameter

*ψ* based on the applied magnetic field. The second equation then provides the superconducting current.

The Ginzburg-Landau equations produce many interesting and valid results. Perhaps the most important of these is its prediction of the existence of two characteristic lengths in a superconductor. The first is a **coherence length** *ξ*, given by

which describes the size of thermodynamic fluctuations in the superconducting phase. The second is the

**penetration depth** *λ*, given by

where

*ψ*_{0} is the equilibrium value of the order parameter in the absence of an electromagnetic field. The penetration depth describes the depth to which an external magnetic field can penetrate the superconductor.

The ratio *κ* = *λ/ξ* is known as the **Ginzburg-Landau Parameter**. It has been shown that Type I superconductors are those with *κ* < 1/√2, and Type II superconductors those with *κ* > 1/√2.

The most important finding from Ginzburg-Landau theory was made by Alexei Abrikosov in 1957. In a type-II superconductor in a high magnetic field - the field penetrates in quantized tubes of flux, which are most commonly arranged in a hexagonal arrangement.

This theory arises as the scaling limit of the XY model.