Phase-error scaling and ranking of finite-window and partial-averaging schemes

Measure the phase-error scaling of the Koopman finite-window method at a resonance crossing and compare it with the $O(\epsilon^{4/7})$ phase-error scaling achieved by the optimally tuned partial-averaging switch, in order to rank the two schemes.

Background

The paper reports that the optimally tuned partial-averaging switch of Lynch et al. achieves a phase error of O(ϵ4/7)O(\epsilon^{4/7}). For the finite-window Koopman construction, the paper demonstrates boundedness of the generator and recovery of the leading resonant jump, but it does not quantify the corresponding phase-error scaling at a crossing.

Because the finite-window scaling has not been measured, the relative accuracy of the two approaches remains unresolved and the authors state that the schemes cannot yet be ranked.

References

The optimally tuned switch of Ref. attains a phase error of $O(\epsilon{4/7})$. The corresponding scaling for the finite window at a crossing has not been measured, so the two schemes cannot yet be ranked.

Resonance crossings as entire functions of the Koopman operator  (2608.21193 - Canizares, 21 Aug 2026) in Section 3, Subsection “Caveats and limitations,” item 3 (label sec:kerr-caveats)