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Real and complex analysis

The exact Sobolev endpoint for Schrödinger convergence

OpenAI research collection · 2 manuscripts · Source checked 2026-10-19

OpenAI's result summary

Proves almost-everywhere convergence e^{it\Delta}f→ f as t\downarrow0 for every f∈ H^{n/(2(n+1))}(\mathbb R^n) and every dimension n ≥ 2. This attains the sharp Sobolev equality case of Carleson's Schrödinger convergence problem, including the planar endpoint H^(1/3).

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Short excerpts below come from OpenAI's abstracts. The full abstract and original PDF preserve the paper's precise scope.

MANUSCRIPT 01

Endpoint convergence for the planar Schrodinger equation

We resolve the planar Sobolev endpoint of Carleson's convergence problem: for initial data in H^{1/3}(\mathbb R^2), the Schrödinger evolution converges almost everywhere to the initial data as t\downarrow0. The evolution is defined by taking the Gaussian regularization limit first; on one full-measure spatial set, this limit…

Full source abstract

We resolve the planar Sobolev endpoint of Carleson's convergence problem: for initial data in H^{1/3}(\mathbb R^2), the Schrödinger evolution converges almost everywhere to the initial data as t\downarrow0. The evolution is defined by taking the Gaussian regularization limit first; on one full-measure spatial set, this limit exists for every 0< t< 1, and the resulting evolution is continuous at t = 0.

This exact PDF is not listed in the imported formalization catalogue. Family scope notes may contain further information.

MANUSCRIPT 02

Endpoint pointwise convergence for the Schrodinger equation in higher dimensions

We resolve the Sobolev endpoint of Carleson's pointwise convergence problem in every dimension n ≥ 3. For initial data in H^{n/(2(n+1))}(\mathbb R^n), the free Schrödinger evolution converges almost everywhere to the initial data as t\downarrow0. The evolution is defined by removing Gaussian regularization on one full-measure…

Full source abstract

We resolve the Sobolev endpoint of Carleson's pointwise convergence problem in every dimension n ≥ 3. For initial data in H^{n/(2(n+1))}(\mathbb R^n), the free Schrödinger evolution converges almost everywhere to the initial data as t\downarrow0. The evolution is defined by removing Gaussian regularization on one full-measure spatial set, uniformly over the interval 0< t< 1.

This exact PDF is not listed in the imported formalization catalogue. Family scope notes may contain further information.

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