Factorization of the linearized nanopteron operator

Establish whether the linearization \(\mathcal B_{\epsilon}+\Sigma\) of the singularly perturbed Korteweg–de Vries traveling-wave equation at the solitary-wave profile \(\sigma\) can be treated through the proposed factorization-based approach involving the KdV linearization \(\mathcal K_0\) and the oscillator operator \(\epsilon^2\partial_z^2+(\epsilon\omega_\epsilon)^2\), and determine whether this approach yields an effective nanopteron construction.

Background

The paper observes that its two principal linear operators are the singularly perturbed oscillator operator ϵ2(z2+ωϵ2)\epsilon^2(\partial_z^2+\omega_\epsilon^2) and the invertible KdV linearization K0\mathcal K_0. A factorization of their combined operator would substantially simplify inversion and the subsequent nanopteron fixed-point argument.

The exact factorization proposed in the discussion does not hold. The authors nevertheless formulate a conjectural alternative based on rewriting the problem as a perturbed second-order oscillator equation after applying K01\mathcal K_0^{-1}. Whether this strategy can actually replace the paper’s operator framework remains unresolved.

References

Motivated by our reading of this perturbation, we conjecture that the following approach would also work for our treatment of the problem eqn: the problem.

eqn: the problem:

$\ep^2u^{(4)}+u''-u+u^2 = 0 $

Phase-Shifted Nanopteron Solutions to a Singularly Perturbed Korteweg--de Vries Equation  (2608.19097 - Faver, 19 Aug 2026) in Section 8, Subsection “Amick and Toland’s factorization”