Finite-subsystem QFI edge topology

Determine, by evaluating the exact quantum Fisher information expression for the particle number in a finite subextensive subsystem of the quenched two-dimensional p+ip superfluid, whether the sign of the QFI spectrum immediately inside the phase-II continuum edges carries topological information when the large-subsystem condition is not satisfied.

Background

The paper derives the phase-II QFI spectrum primarily within the large-subsystem approximation, LAks1L_A\gg k_s^{-1}, where the two momenta entering the exact QFI expression can be treated as approximately equal. In that regime, when μ<mΔ2\mu_\infty<m\Delta_\infty^2, the QFI spectrum vanishes at the continuum edges and its sign immediately inside the edges directly reveals the pre-quench pseudospin winding number QQ.

For finite subsystems with LAks1L_A\lesssim k_s^{-1}, the exact QFI involves pairs of distinct momenta. Although the spectrum still vanishes at the relevant edges, its sign depends on the pseudospin texture over a finite momentum window rather than solely on the zero-momentum pseudospin. The paper therefore leaves unresolved whether this finite-subsystem edge behavior retains any reliable information about the topology of the pre-quench state.

References

A more complete analysis of $\sgn \tilde{F}_Q(\pm2(E_0+0+))$, and whether it carries any topological information, outside the regime $L_A \gg k_s{-1}$, requires evaluating the exact expression in Eq.~\ref{eq:FQA2} and is left for future study.

Quantum Fisher information in a quenched $p + ip$ superfluid  (2608.21164 - Varrone et al., 21 Aug 2026) in Section 'Beyond the large-$L_A$ approximation' (Section 3.4), paragraph discussing phase-II continuum-edge behavior