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 thermodynamicarguments.
This theory is sometimes called phenomenological as it describes some of the phenomena of superconductivity without explaining the underlying microscopic mechanism.
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 "Fn" is the free energy in the normal phase, "α" and "β" are phenomenological parameters, "m" is an effective mass, A is the electromagnetic
vector potential, and B=curlA is the magnetic induction. 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 density and "Re" the "real part". 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.
Consider a homogeneous superconductor in absence of external magnetic field. Then there is no superconducting current and the equation for ψ simplifies to:
This equation has a trivial solution ψ = 0. This corresponds to normal state of the superconductor, that is for temperatures "T" above the superconducting transition temperature "T""c".
Below superconducting transition temperature the above equation is expected to have a non-trivial solution (that is ψ ǂ 0). Under this assumption the equation above can be rearranged into:
When the right hand side of this equation is positive, there is a non zero solution for ψ (remember that the magnitude of a complex number can be positive or zero). This can be achieved by assuming the following temperature dependence of α: α("T") = α0 ("T" - "T""c") with α0 / β > 0:
*Above superconducting transition temperature, "T" > "T""c", the expression α("T") / β is positive and the right hand side of the equation above is negative. Magnitude of a complex number must be non-zero number, so only ψ = 0 solves the Ginzburg–Landau equation.
*Below superconducting transition temperature, "T" < "T""c", the right hand side of the equation above is positive and there is a non-trivial solution for ψ. Furthermore
that is ψ approaches zero as "T" gets closer to "T""c" from below. Such a behaviour is typical for a second order phase transition.
Coherence Length and Penetration Depth
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 "ψ0" 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 Isuperconductors are those with "κ" < 1/√2, and Type IIsuperconductors those with "κ" > 1/√2. For Type II superconductors, the phase transitionfrom the normal state is of second order, for Type I superconductors it is of first order. This is provedby deriving a " dual Ginzburg–Landau theory" for the superconductor (see Chapter 13 of the third textbook below).
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 limitof the XY model.The importance of the theory is also enhanced by a certain similarity with the Higgs mechanismin high-energy physics.
* V.L. Ginzburg and L.D. Landau, "Zh. Eksp. Teor. Fiz." 20, 1064 (1950) ... Original paper of Ginzburg and Landau
* A.A. Abrikosov, "Zh. Eksp. Teor. Fiz." 32, 1442 (1957) (English translation: "Sov. Phys. JETP" 5 1174 (1957)] .) ... Abrikosov's original paper on vortex structure of
Type IIsuperconductors derived as a solution of G–L equations for κ > 1/√2
* L.P. Gor'kov, "Sov. Phys. JETP" 36, 1364 (1959)
* A.A. Abrikosov's 2003 Nobel lecture: [http://nobelprize.org/nobel_prizes/physics/laureates/2003/abrikosov-lecture.pdf pdf file] or [http://nobelprize.org/nobel_prizes/physics/laureates/2003/abrikosov-lecture.html video]
* V.L. Ginzburg's 2003 Nobel Lecture: [http://nobelprize.org/nobel_prizes/physics/laureates/2003/ginzburg-lecture.pdf pdf file] or [http://nobelprize.org/nobel_prizes/physics/laureates/2003/ginzburg-lecture.html video]
* D. Saint-James, G. Sarma and E. J. Thomas, "Type II Superconductivity" Pergamon (Oxford 1969)
* M. Tinkham, "Introduction to Superconductivity", McGraw-Hill (New York 1996)
* de Gennes, P.G., "Superconductivity of Metals and Alloys", Perseus Books, 2nd Revised Edition (1995), ISBN 0-201-40842-2 (this book is heavily based on G–L theory)
Hagen Kleinert, "Gauge Fields in Condensed Matter", Vol. I [http://www.worldscibooks.com/physics/0356.htm World Scientific (Singapore, 1989)] ; Paperback ISBN 9971-5-0210-0 ("also available online [http://www.physik.fu-berlin.de/~kleinert/kleiner_reb1/contents1.html here] ")
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