The process by which electrons form pairs, enabling superconductivity without resistance.Electron pairing is the quantum phenomenon where two electrons, which normally repel each other due to their negative charges, form a bound state that behaves as a single particle. This pairing is the foundation of conventional superconductivity, where a material conducts electricity with zero resistance below a critical temperature. The pairs, known as Cooper pairs, have integer spin and thus behave as bosons, allowing them to condense into a single quantum state that can carry current without scattering. Electron pairing also plays a role in other phenomena, such as superfluidity in certain fermionic systems and the formation of polarons in solids.
The concept was introduced by Leon Cooper in 1956, and it was immediately incorporated into the BCS theory of superconductivity by Bardeen, Cooper, and Schrieffer in 1957, which earned them the Nobel Prize in Physics in 1972.
In a conventional superconductor, an electron moving through a crystal lattice attracts the positively charged ions, creating a slight distortion. A second electron is then drawn to this region of positive charge, effectively forming a pair mediated by lattice vibrations (phonons). The pairing is strongest when the electrons have opposite momenta and spins, as this minimizes the energy cost. Once paired, the electrons are no longer subject to the same scattering processes that cause resistance, because the collective condensate is rigid against perturbations. The energy gap between the paired state and unpaired electrons protects the superconducting state.
Electron pairing is exploited in superconducting magnets for MRI machines and particle accelerators, in quantum computing qubits, and in sensitive magnetic field detectors like SQUIDs.
In some exotic materials, electrons can form not just pairs but quartets, as observed in certain iron-based superconductors, challenging the standard BCS picture.












