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Exact value of the L2-equicontinuity mass threshold M* for the focusing continuum Calogero–Moser model

Determine the exact value of the sharp mass threshold M*, defined for the focusing continuum Calogero–Moser model iu_t + u_{xx} - 2 i u Π^+ ∂_x(|u|^2) = 0, with the property that whenever a bounded family U ⊂ H^∞_+ of initial data is L2-equicontinuous (i.e., uniformly translation-continuous in L2 or, equivalently, with uniformly vanishing high-frequency tails) and satisfies sup_{u0∈U} M(u0) < M*, then the associated set of partial orbits U_T^* = {u(t) : u solves the model with u(0) ∈ U, t ∈ [0, T)} is L2-equicontinuous for all T > 0.

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Background

Laurens, Killip, and Vișan introduced the notion of L2-equicontinuity for families of initial data in H∞_+ and defined a sharp mass threshold M* ensuring that if sup mass is below M*, then the entire set of partial orbits remains L2-equicontinuous for all times. They proved M* ≥ 2π and global well-posedness below M* for all Hs_+, s ≥ 0.

The present paper proves that for any mass just above 2π there exist initial data whose maximal orbit fails to be L2-equicontinuous, showing that global-in-time L2-equicontinuity fails in general for mass > 2π. Despite this, the precise value of M* is not determined in the paper and remains explicitly unidentified.

References

They showed that M* \geq 2\pi and that CM-DNLS is globally well-posed in Hs_+ for all s \geq 0 below the mass M*. The exact value of M* is currently unknown, but Theorem~\ref{main result} shows that global-in-time $L2$-equicontinuity fails in general for mass greater than $2\pi$.

Turbulent Threshold for Continuum Calogero-Moser Models (2401.16609 - Hogan et al., 29 Jan 2024) in Introduction, paragraph following Definition (L2 Equicontinuity) and discussion of M*, referencing Theorem \ref{main result}