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

Recently it was discovered that the ground state orbital angular momentum in two-dimensional chiral superfluids with pairing symmetry $(p_x+ip_y)^ν$ depends on the winding number $ν$ in a striking manner. The ground state value for the $ν=1$ case is $L_z=\hbar N/2$ as expected by counting the Cooper pairs, while a dramatic cancellation takes place for $ν>1$. 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 $ν=1$ under all studied circumstances. We study how angular momentum depends on the gap size $Δ/E_F$ and obtain the result $L_z=\frac{\hbarν}{2} N(1-\fracμ{E_F})$ for $ν=2,3$. Thus, the gap-dependence of $L_z$ for $ν<4$ enters at most through the chemical potential while $ν\geq4$ 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.

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