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Compactly supported real scalar potentials realizing the Hardy uncertainty endpoint for Schrödinger evolutions

Xiao-Ming Fu, Tianyang Sun

math.AP Jul 25, 2026 · v1
The proof of the main theorem (Theorem 1.1) was formally verified in Lean, with the formalization released in a project repository.
At the critical Hardy Gaussian weight for the Schrödinger equation in one space dimension on $[0,1]$, the known nonzero scalar example in the weighted $L^2$ class carries a complex-valued potential. Cassano and Fanelli observed that the existence of a real-valued scalar endpoint example was open, and produced examples with real electric and magnetic potentials only after introducing a magnetic potential. We construct a nonzero smooth solution of $i\partial_t u+\partial_x^2 u=Vu$ on $\mathbb{R}\times[0,1]$ such that $e^{x^2/4}u(\cdot,0),e^{x^2/4}u(\cdot,1)\in L^2(\mathbb{R})$ and the potential is bounded, smooth, real-valued, and purely scalar and is supported in one fixed compact spatial interval for all times. This compact-support endpoint example is the main result. We also record the explicit rational-tail realization underlying the construction. The main results of this paper were obtained by the multi-agent system Eureka and have subsequently been verified by the authors.

At the critical Hardy Gaussian weight for the 1D Schrödinger equation on [0,1], the only known nonzero endpoint examples used either a complex-valued potential or an added magnetic potential. Whether a real-valued, purely scalar endpoint example exists was an open problem.

The authors use a transported ansatz with a Gaussian width y(t) satisfying y”=16/y^3 and a pseudoconformal phase b=y'/(4y). This choice makes the continuity equation hold identically, which forces the potential to be real. A rational-tail profile, refined into a compactly supported profile built from parabolic cylinder functions, keeps the weighted L^2 endpoint condition satisfied while the potential stays bounded. The results were obtained by the multi-agent system Eureka, checked by the authors, and the main theorem was formally verified in Lean.

They construct a nonzero smooth solution with e^{x^2/4}u at times 0 and 1 in L^2. The potential is bounded, smooth, real-valued and purely scalar, and is supported in a fixed compact spatial interval for all times. The mechanism extends to all dimensions and to general time intervals.