A form of superconductivity where electron pairs have parallel spins, allowing supercurrents to flow through magnetic materials.Triplet superconductivity is a rare and exotic form of superconductivity in which the paired electrons—known as Cooper pairs—have parallel spins, unlike the conventional singlet state where spins are antiparallel. This spin-aligned pairing gives the supercurrent unusual properties, most notably the ability to flow through magnetic materials without being destroyed. In ordinary superconductors, even a weak magnetic field or magnetic impurity breaks the antiparallel pairs, but triplet pairs are largely immune because their spin state is symmetric under exchange, matching the symmetry of a magnetic environment.
The theoretical possibility was proposed in the 1960s, but the first convincing experimental evidence emerged in the early 2000s with the discovery of triplet superconductivity in the heavy-fermion compound UTe2 and in certain ruthenates. The field remains active, with ongoing debates about the exact pairing symmetry.
In a conventional superconductor, electrons pair through lattice vibrations (phonons) into a spin-singlet state with total spin zero. Triplet pairing requires a different glue—often magnetic fluctuations or spin excitations—that favors parallel spins, yielding a total spin of one. This triplet state can be odd in momentum space (p-wave or f-wave), meaning the pairing amplitude changes sign under spatial inversion. The parallel spins allow the supercurrent to coexist with ferromagnetic order, and the order parameter can even be chiral, breaking time-reversal symmetry.
Triplet superconductors are studied for potential use in spintronics, where the spin-polarized supercurrent could transfer spin information without energy loss, and in quantum computing as a platform for topologically protected qubits.
In some triplet superconductors, the supercurrent can flow through a ferromagnetic barrier, a phenomenon impossible in conventional superconductors.






















