[theory] formation of cooper pairs

In summary, cooper pairs in low temperature superconductors are formed through a quantum mechanical effect, where a small attractive interaction between electrons creates a binding energy and opens a gap in the energy spectrum. This results in a decrease in electrical resistance to zero at low temperatures. To fully understand this phenomenon, one must study the BCS theory or the field theory approach.
  • #1
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Homework Statement


I'm interested to know how cooper pairs are formed in low temperature superconductors.

The Attempt at a Solution


My basic understanding is that electrons will repel other electrons and attract the positive ions which make up the lattice of the metal. The attraction between the +ve ions and the electrons is enough to distort the ions and hence attract other electrons. The attraction due to the displaced ions can then overcome the repulsion between electrons causing them to form cooper pairs. Does this general case apply for low temperature superconductors?
 
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  • #2
IIRC that picture, though convenient to make a mental image, is only approximately right. The Cooper pairing between electrons is a purely quantum mechanical effect and one needs the full BCS theory to describe it. The field theoretical description looks quite elegant.

Basically, what happens, is that a small attractive interaction between the electrons takes place (for example in the way you explained in your post, in the case of a crystal lattice). Two electrons can be bound together in a single quantum state (note however, that they can be physically separated by a "large" distance) which has a certain "binding energy". This , as condensed matter people say, opens a gap in the energy spectrum: it takes a certain amount of energy to break this pair. If the temperature is low enough so that thermal fluctuations cannot bridge this gap, the system will form as much of this lower-energy pairs as possible, whence - among other things - the electrical resistance (~ "number of collisions due to thermal fluctuations") drops to zero.

But again, to understand it fully, you should dive into BCS theory (and if you know anything about field theory, I can recommend the field theory approach).
 

What is the theory behind the formation of cooper pairs?

The theory of cooper pair formation was first proposed by physicist Leon Cooper in 1956. It suggests that in certain materials, such as superconductors, electrons can pair up and move through the material without resistance. This phenomenon is known as superconductivity.

How do cooper pairs form in a material?

According to the BCS theory (named after its creators Bardeen, Cooper, and Schrieffer), cooper pairs form due to an interaction between electrons and the lattice vibrations (phonons) in a material. This interaction acts as a binding force between the electrons, allowing them to pair up and move freely.

Why are cooper pairs important in superconductivity?

Cooper pairs are crucial for the phenomenon of superconductivity because they allow for the flow of electrical current without any resistance. This means that superconductors can conduct electricity with 100% efficiency, making them useful for a variety of applications in fields such as transportation, medical imaging, and energy storage.

Can cooper pairs exist at any temperature?

In order for cooper pairs to form, certain conditions must be met, including low temperatures. This is because at higher temperatures, the thermal energy is too strong and can break apart the pairs. However, some materials called high-temperature superconductors can exhibit superconductivity at relatively higher temperatures.

What evidence supports the theory of cooper pair formation?

There is a significant amount of experimental evidence that supports the theory of cooper pair formation. For example, the Meissner effect, which is the expulsion of magnetic field lines from a superconductor, can only be explained by the presence of cooper pairs. Additionally, the BCS theory accurately predicts the critical temperature at which superconductivity occurs in various materials.

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