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Nonlinear stability of the constant solution in the focusing case for large periods

Prove the nonlinear stability of the nonzero constant solution u(x,t) ≡ 1 to the focusing nonlocal derivative NLS equation i u_t = u_{xx} − u (i + H) (|u|^2)_x with respect to periodic perturbations in H^1_per((0,L), C) for every spatial period L ∈ [π, ∞).

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Background

The authors prove nonlinear stability of the nonzero constant background in the defocusing case for all periods and, in the focusing case, for periods L ∈ (0, π), using a Lyapunov functional built from conserved quantities. They also identify a linear resonance and instability in the focusing case for the 2π-periodic setting, indicating challenges for larger periods.

Consequently, extending nonlinear stability to larger spatial periods in the focusing case is unresolved. The remark explicitly states that proving nonlinear stability for L ≥ π remains open, a regime that includes periods multiple of 2π where linear instability is present.

References

For L ∈ [π,∞), it is an open problem to prove the nonlinear stability of the constant solution u = 1 with respect to perturbations in H1_{ m per}((0,L),\mathbb{C}) in the focusing case σ = −1.

Traveling periodic waves and breathers in the nonlocal derivative NLS equation (2501.15625 - Chen et al., 26 Jan 2025) in Remark (end of Section 3: Stability of the nonzero constant background)