phenomenon

triplet superconductivity

A form of superconductivity where electron pairs have parallel spins, allowing supercurrents to flow through magnetic materials.
62 related articles

Description

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.

History

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.

How it works

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.

In practice

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.

Fun fact

In some triplet superconductors, the supercurrent can flow through a ferromagnetic barrier, a phenomenon impossible in conventional superconductors.

Concept graph →

Related articles · 62

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