Barnett–Betcke MFS convergence-rate conjecture for Helmholtz problems

Let Ω\Omega be an exterior sound-soft Helmholtz domain with boundary Γ=Ω\Gamma=\partial\Omega, and let uu be the scattered-field solution represented by the method of fundamental solutions (MFS), with JJ MFS points equally distributed in conformal angle at conformal distance RR inside Γ\Gamma. Let ε\varepsilon be the maximum MFS error measured on Γ\Gamma. Let ρ<1\rho<1 be the conformal radius of the closest singularity of the analytic continuation of uu, in the sense of conformal radius. Barnett–Betcke MFS convergence-rate conjecture. Then

ε{KρJ/2,ρ>R2,KRJ,ρ<R2,\varepsilon\leq\begin{cases} K\rho^{-J/2},&\rho>R^2,\\ KR^{-J},&\rho<R^2, \end{cases}

where KK may depend on Γ\Gamma, kk, RR, and vv, but not on JJ. This conjecture gives the theoretical basis for the MFS point-placement strategy in the AAALS algorithm; the supplied source does not establish whether the conjecture has been resolved.

Sources & referencesView supporting material

Primary source

Stefano Costa, “AAA least squares solution of Helmholtz problems”, arXiv:2601.19020 (2026).

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