Ground state angular momentum, spectral asymmetry, and topology in chiral superfluids and superconductors

TL;DR

This paper investigates how the ground state orbital angular momentum in two-dimensional chiral superfluids depends on pairing symmetry, topological edge states, and potential profiles, revealing robustness for certain cases and complex dependencies on system parameters.

Contribution

It provides a detailed analysis of the spectral asymmetry and angular momentum in chiral superfluids, extending understanding to total angular momentum in triplet superfluids with spin-orbit coupling.

Findings

Robustness of L_z=ħN/2 for ν=1 under various conditions

Derived L_z= (ħν/2) N(1 - μ/E_F) for ν=2,3

Total angular momentum behavior varies with Cooper pair angular momentum

Abstract

Recently it was discovered that the ground state orbital angular momentum in two-dimensional chiral superfluids with pairing symmetry $(p_x+ip_y)^\nu$ depends on the winding number $\nu$ in a striking manner. The ground state value for the $\nu=1$ case is $L_z=\hbar N/2$ as expected by counting the Cooper pairs, while a dramatic cancellation takes place for $\nu>1$. The origin of the cancellation is associated with the topological edge states that appear in a finite geometry and give rise to a spectral asymmetry. Here we study the reduction of orbital angular momentum for different potential profiles and pairing strengths, showing that the result $L_z=\hbar N/2$ is robust for $\nu=1$ under all studied circumstances. We study how angular momentum depends on the gap size $\Delta/E_F$ and obtain the result $L_z=\frac{\hbar\nu}{2} N(1-\frac{\mu}{E_F})$ for $\nu=2,3$. Thus, the gap-dependence of $L_z$ for $\nu<4$ enters at most through the chemical potential while $\nu\geq4$ is qualitatively different. In addition, we generalize the spectral asymmetry arguments to \emph{total} angular momentum in the ground state of triplet superfluids where due to a spin-orbit coupling $L_z$ is not a good quantum number. We find that the ground state total angular momentum also behaves very differently depending on total angular momentum of the Cooper pairs.