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Classification of quasiperiodic isodispersive phases

Characterize all quasiperiodic isodispersive phases for reflectionless potentials of the Lax operator L in the classical integrable system defined by the Lax pair (L, M) and evolution equations (iu_t = 2(q^* ξ_x − q ξ^*_x), iv_t = 2(ξ ξ_x^* − ξ^* ξ_x)_x, i ξ_t = −2 v ξ + q_x, i q_t = −2 v q − 2 ξ u_x − 4 ξ_x u + 4 ξ (|ξ|^2)_x − ξ_{xxx}) by determining the conserved densities ρ_n^{R,I} required to classify such phases beyond the uniform-phase invariants ρ_1^I = u − 2|ξ|^2 and (ρ_3^I)_{uniform} = |q|^2 + (u^2 + v^2)/2 + 2 u |ξ|^2 − 2 |ξ|^4.

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Background

The paper introduces isodispersive phases to describe backgrounds at x → ±∞ that share the same dispersion relation λ(k) for the Lax operator L. While uniform isodispersive phases can be classified by low-order conserved densities, the tsunami-soliton dynamics produce oscillatory and quasiperiodic backgrounds whose classification is nontrivial.

The authors suggest that a complete classification of these quasiperiodic isodispersive phases may require higher-order conserved densities ρ_n{R,I}, but this requirement and the full classification framework remain unresolved.

References

While the uniform phases are classified by values $\rho_1{\text{I}=u-2|\xi|2 $ and $ (\rho_3{\text{I})_{\text{uniform}=|q|2+\frac{u2+v2}{2}+2u|\xi|2-2|\xi|4$, characterizing all quasiperiodic isodispersive phases might require higher-order $\rho_n{\text{R,I}$'s, remaining to be an open problem.

Tsunami Solitons Emerging from Superconducting Gap (2508.18311 - Takahashi, 23 Aug 2025) in Penultimate paragraph, beginning "Finally, we introduce the concept of isodispersive phases…"