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Helium-3 for Quantum Computing

Helium-3 as a Fermi Liquid

Liquid helium-3 is a textbook Fermi liquid: its atoms are fermions whose collective behavior is described by quasiparticles with an enhanced effective mass.

Fermions in a liquid

A helium-3 atom has an odd number of nucleons and one unpaired nuclear spin, making the atom a fermion. Liquid helium-3 is therefore a dense collection of interacting fermions, and at low temperature it behaves according to Landau's theory of Fermi liquids, one of the foundational frameworks of condensed-matter physics.

Quasiparticles and effective mass

Kronos motion — quantum verdict

In a Fermi liquid the strongly interacting particles are described as weakly interacting quasiparticles: each real particle dressed by the disturbance it creates in its neighbors. The quasiparticles obey Fermi-Dirac statistics and fill states up to a Fermi surface. Interactions renormalize their properties, so a helium-3 quasiparticle has an effective mass several times the bare atomic mass, and quantities like heat capacity and compressibility follow Fermi-liquid predictions with this enhanced mass.

Consequences for cryogenics

This physics matters directly for dilution refrigeration. In the dilute phase of a helium-3 / helium-4 mixture, the helium-3 behaves as a dilute Fermi gas of quasiparticles moving through the superfluid background. Its heat capacity and enthalpy, which set the cooling power of the mixing chamber, follow from this Fermi-liquid description. The finite solubility and the enthalpy difference across the phase boundary are both consequences of helium-3 being a Fermi system.

Superfluid helium-3

At far lower temperatures, around two millikelvin, liquid helium-3 itself becomes superfluid, but by a different mechanism than helium-4. The fermionic atoms form pairs, analogous to Cooper pairs in a superconductor but with the pairs carrying spin and orbital angular momentum, producing a rich set of superfluid phases. This is well below the operating range of a dilution refrigerator but is a landmark result in the physics of the isotope.