Cooper pair breaking refers to the phenomenon in superconductors where the bound pairs of electrons, known as Cooper pairs, are disrupted due to thermal or external influences. In a superconductor, these pairs form at low temperatures, allowing for zero electrical resistance. However, when the temperature rises or when an external magnetic field is applied, the energy can become sufficient to break these pairs apart.
This process can be quantitatively described using the concept of the Bardeen-Cooper-Schrieffer (BCS) theory, which explains superconductivity in terms of these pairs. The breaking of Cooper pairs results in a finite resistance in the material, transitioning it from a superconducting state to a normal conducting state. Additionally, the energy required to break a Cooper pair can be expressed as a critical temperature above which superconductivity ceases.
In summary, Cooper pair breaking is a key factor in understanding the limits of superconductivity and the conditions under which superconductors can operate effectively.
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