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Cooper pairs

Definition/Summary
A bound state of two electrons having equal and opposite momentum and spin. These states can form in a normal metal due to: 1) an attractive phonon-mediated interaction, and 2) the presence of the Fermi surface. The formation of Cooper pairs in a normal metal will occur if the temperature is low enough and will cause the metal to become a superconductor.

Equations
Click to see the LaTeX code for this image
where the first factor is the spin-singlet part of the wave function, and the next factor is the symmetric real-space part of the wave function.

In the above equation Click to see the LaTeX code for this image and Click to see the LaTeX code for this image is the energy of the Cooper pair, given in the weak coupling approximation by Click to see the LaTeX code for this image, where Click to see the LaTeX code for this image is the Fermi energy, Click to see the LaTeX code for this image is the reduced Planck constant, Click to see the LaTeX code for this image is an effective cutoff energy specifying over what interval the effective attraction is non-zero and equal to Click to see the LaTeX code for this image, and Click to see the LaTeX code for this image is the density of states at the Fermi energy.

Scientists
Leon N Cooper (1930-)

Recent forum threads on Cooper pairs
 
Breakdown
Physics
> Condensed Matter
>> Superconductivity

See Also
Introduction to Superco

Images

Extended explanation
One of the obvious problems with the idea of a bound state of two electrons is that the electrons have the same charge. Thus, in addition to an attractive phonon-mediated force there is a repulsive Coulomb force. The way around this problem is the effect of screening. In a metal there are many mobile electrons in addition to the two electrons making up the Cooper pair. It is possible that these "other" electrons screen the Coulomb repulsion enough that the phonon-mediated attraction is dominant.

But, even if the net force is attractive between electrons, this does not necessitate the existence of a bound state. Only in two or fewer dimensions will an arbitrarily weak attraction lead to a bound state. The way out of this dilemma is the existence of a Fermi surface. The fact that the two electrons making up a Cooper pair are above the filled "Fermi Sea" of the normal metal make the density of states appear two dimensional and allows for the existence of a bound state.

Commentary

tiny-tim @ 07:07 AM Nov16-09
Thankyou PhaseShifter, it's being looked into.
Title changed from "Cooper pair" to "Cooper pairs" since forum searches show that that links to 70% more threads.

PhaseShifter @ 05:53 AM Sep23-09
Could you clarify the "equal and opposite momentum" part?

It seems to me that if they always had wqual and opposite momentum then the pair wouldn't contribute to current at all.

_PJ_ @ 12:11 PM Aug30-09
Are these factors known? Might it be that suffiently lower temperatures are required?

f95toli @ 06:13 PM Aug24-09
Note that not all metals become superconducting at low temperatures. Good conductors such as gold, silver and copper never become superconducting, regardless of temperature. Hence, whether or not a Cooper pair can form depends depends on several factors, temperature is just one.


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