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Majorana fermions as quanta of a superfluid vacuum

James A. Sauls

December 9, 2013

In a perspective article "Majorana returns" published in Nature Physics, 1 Franck Wilczek (Walter and Christine Heilborn Lecturer in 2004) wrote "In his short career, Ettore Majorana made several profound contributions. One of them, his concept of ‘Majorana fermions’ - particles that are their own antiparticle - is finding ever wider relevance in modern physics."

Majorana's idea, published in 1937, was born from Paul Dirac's relativistic quantum theory of the electron, the centerpiece being the Dirac equation, which not only accounted for electron spin of [1/2] (in units of Planck's quantum ħ), but led directly to the prediction of the positron - the anti-particle of the electron with opposite electrical charge. Majorana found a new equation describing neutral, spin [1/2] particles that are their own anti-particle, and he speculated that the neutrino might be such a particle. Years later the discovery that the various flavors of neutrinos have mass, and can transform into one another, combined with theories for the spectrum of particles at energies near the Higgs scale, have fueled new generations of experiments designed to search for definitive signatures that neutrinos `are' - or `are not' - Majorana particles, as well as hypothesized supersymmetric partners to the neutral gauge bosons of the standard model, all of which are Majorana fermions.

However, neutrinos, LHC and dark matter searches are not the only physics frontiers where Majorana's elusive particles have found renewed interest. The "ever wider relevance" that Wilczek refers to in his article are developments and discoveries in condensed matter where Majorana fermions emerge as quanta at ultra-low energies in a number of quantum liquid and solid phases of matter. Indeed since 2008 there has been an explosion in theoretical predictions and discovery of new materials - insulators, superconductors and superfluids - in which Majorana's idea has found relevance.

Among the physics frontiers in the search for Majorana fermions are the ultra-low temperature phases of the light isotope of Helium (3He) - the B phase of superfluid 3He to be specific. Not long after their discovery it was realized that the superfluid phases of 3He provided a paradigm for one of the conceptual cornerstones of modern physics, namely the role of spontaneous symmetry breaking in quantum field theory and condensed matter physics.2 The developments in this field lead to separate Nobel prizes for the discovery of the phases by Douglas Osheroff, Robert Richardson and David Lee in 1996, and for theoretical developments leading to the identification of these macroscopic quantum states of matter by Anthony J. Leggett in 2003.

But only since 2008 has it been widely appreciated that the ground state of this quantum liquid has remarkable properties connected with the mathematics of topology that imply that Majorana fermions exist as quanta. Everything we now believe we understand about superfluid 3He tells us that Majorana fermions must emerge from the ground state of superfluid 3He - what is aptly dubbed the "superfluid vacuum" - as low-energy quanta, confined on the surface or a boundary of superfluid 3He.

So how might these exotic particles be detected? Several theoretical proposals focus on the spin of the Majorana fermions, or the spin current carried by Majorana particles. Detecting spin currents of Majorana fermions turns out to be complicated, sufficiently so that the elusive Majorana particles have so far remained just that.

A paper published this month in Physical Review suggests another route to detection.3 The idea is based on the energy-momentum relation for the Majorana particles, E = c|p|, where the "light speed" of the superfluid vacuum is c ≈ 5 cm/sec. The superfluid vacuum offers a method for detecting these quanta at ultra-low temperatures utilizing the Doppler shift of the Majorana fermions if the superfluid vacuum is set in motion.

The fundamental property of a superfluid is that it supports a `persistent current', i.e. mass flow without dissipation - the same phenomena responsible for superconductivity, i.e. the flow of electricity without Joule losses. For 3He confined within a channel (Fig. 1), motion of the superfluid relative to the channel walls leads to a Doppler shift in the spectrum of Majorana particles confined on the walls, E → E′ = c|p| − p·vs, where vs is the velocity of the superfluid vacuum relative to the channel walls.

Flow Geometry for Detecting Majorana Fermions Figure 1: Majorana Fermions confined on the boundary of 3He have a massless dispersion, E = c|p|;, shown as the Majorana `cone', while Dirac fermions with mass ∆, are the quanta in bulk 3He. Relative motion of the superfluid vacuum (vs) leads to a Doppler shift in the energy of Majorana fermions.

The fraction of mass that can participate in the persistent current depends on the energy and momentum distribution of fermi particles present - in this case the Doppler shifted Majorana fermions - and the absolute temperature, T, which controls the number of thermally excited Majorana fermions. The Doppler effect leads to asymmetry in the thermal populations of Majorana excitations that are co-moving and counter-moving relative to the superfluid vacuum, and thus to a reduction in the persistent current. The linear dispersion of the Majorana particles, their Fermi statistics, combined with their confinement in two dimensions leads to a unique signature: a power law dependence for the reduction in the mass fraction of the persistent current with temperature, δn/n ∝ − (T/c pf)3, where pf is the Fermi momentum, c is the speed of the Majorana particles and c pf = ∆ is the mass gap for fermions in the bulk of the superfluid vacuum. Just as the radiation flux from matter in thermal equilibrium, proportional to T4, is a signature of the thermal distribution of photons, the quanta of the electromagnetic vacuum, Majorana fermions reveal their presence as a mass flux, proportional to T3, in response to the motion of the superfluid vacuum.

While we await the discovery of Majorana fermmions, new experiments are being planned and theorists are exploring the "open range" of ramifications of matter in which Majorana particles naturally emerge. Whether or not all of the ideas spawned by Majorana's return to center stage will lead to deeper insight into quantum correlations, or to a new generation of quantum computers is far from being answered, but one thing is known. If Majorana fermions are not found in superfluid 3He then of one of the most successful theories of twentieth century physics - the theory of quantum liquid phases of 3He will need a pretty serious adjustment. I'm betting that Majorana's particles are zipping about the surface of 3He, and that there is a remarkable two-dimensional quantum liquid waiting to reveal its secrets. And who knows, maybe we will find out that the larger universe we are embedded in is just as extraordinary as the superfluid vacuum!

Dimensions, Department of Physics and Astronomy, Northwestern University, Spring, 2013 [arXiv:2203.16698]


1Majorana Returns, Nature Physics 5, 614 - 618 (2009), Frank Wilczek. [DOI]

2The Universe in a Helium Droplet, Oxford University Press, 2009, Grigory E. Volovik.

3Majorana excitations, spin and mass currents on the surface of topological superfluid 3He-B, Phys. Rev. B 88, 184506 (2013), Hao Wu and J. A. Sauls. [DOI]

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