Exotic quantum statistics and thermodynamics from a number-conserving theory of Majorana fermions

TL;DR

This paper develops a number-conserving quantum statistical theory for Majorana fermions, revealing a distribution with a sharp Fermi surface and residual entropy, differing from traditional models but aligning with experimental observations.

Contribution

It introduces a novel, exactly solvable, number-conserving model for Majorana fermions, providing new insights into their thermodynamics and statistical behavior.

Findings

Derived a number-conserving Majorana distribution function

Identified a sharply-defined Fermi surface at finite temperatures

Found nearly identical thermodynamics to a free Fermi gas with residual entropy

Abstract

We propose a closed form for the statistical distribution of non-interacting Majorana fermions at low temperature. Majorana particles often appear in the contemporary many-body literature in the Kitaev, Fu-Kane, or Sachdev-Ye-Kitaev models, where the Majorana condition of self-conjugacy immediately results in nonconserved particle number, non-trivial braiding statistics, and the absence of a noninteracting limit. We deviate from this description and instead consider a gas of noninteracting, spin-1/2 Majorana fermions that obey the spin-statistics theorem via imposing a condensed matter analog of momentum conservation. This allows us to build a quantum statistical theory of the Majorana system in the low temperature, low density limit without the need to account for strong fluctuations in the particle number. A combinatorial analysis leads to a configurational entropy which deviates from the fermionic result with an increasing number of available microstates. A number-conserving Majorana distribution function is derived which shows signatures of a sharply-defined Fermi surface at finite temperatures. Such a distribution is then re-derived from a microscopic model in the form of a modified Kitaev chain with a bosonic pair interaction. The thermodynamics of this free Majorana system is found to be nearly identical to that of a free Fermi gas, except now distinguished by a two-fold ground state degeneracy and, subsequently, a residual entropy at zero temperature. Despite clear differences with the anyonic or Sachdev-Ye-Kitaev models, we nevertheless find surprising agreement between our theory and experimental signatures of Majorana excitations in several materials. Experimental realization of our exactly solvable model is also discussed in the realm of astrophysical and high-energy phenomena.