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Global well-posedness of one-dimensional cubic fractional nonlinear Schr\"odinger equations in negative Sobolev spaces

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arxiv 2311.13370 v1 pith:UGOPLJEZ submitted 2023-11-22 math.AP

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keywords cubicfnlsnegativesobolevspaceswell-posednesscircleequation
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We study the Cauchy problem for the cubic fractional nonlinear Schr\"odinger equation (fNLS) on the real line and on the circle. In particular, we prove global well-posedness of the cubic fNLS with all orders of dispersion higher than the usual Schr\"odinger equation in negative Sobolev spaces. On the real line, our well-posedness result is sharp in the sense that a contraction argument does not work below the threshold regularity. On the circle, due to ill-posedness of the cubic fNLS in negative Sobolev spaces, we study the renormalized cubic fNLS. In order to overcome the failure of local uniform continuity of the solution map in negative Sobolev spaces, by applying a gauge transform and partially iterating the Duhamel formulation, we study the resulting equation with a cubic-quintic nonlinearity. In proving uniqueness, we present full details justifying the use of the normal form reduction for rough solutions, which seem to be missing from the existing literature. Our well-posedness result on the circle extends those in Miyaji-Tsutsumi (2018) and Oh-Wang (2018) to the endpoint regularity.

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Cited by 2 Pith papers

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  1. On Balancing Sparsity with Reliable Connectivity in Distributed Network Design with Random K-out Graphs

    cs.SI 2025-08 conditional novelty 8.0 of 10

    Derivative fractional nonlinear Schrödinger equations on the torus are well-posed in Sobolev spaces exactly when a certain integral of the nonlinearity vanishes; otherwise solutions do not exist.

  2. Well- and Ill-posedness of the Cauchy problem for derivative fractional nonlinear Schr\"odinger equations on the torus

    math.AP 2025-08 conditional novelty 7.0 of 10

    For derivative fractional NLS on the torus with α>2, well-posedness holds in H^s for s > max(α/2+1, 5/2) exactly when the resonant integral of F_ω vanishes.

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