AI Proved What?

Episode 372, October 2026

Feel the inside from the surface?

An AI preprint claims global uniqueness for the smooth isotropic elasticity inverse problem in three dimensions

Covers result 372 in OpenAI’s catalog: its one paper. See its connections to other results and the work it cites.

3:56. English captions available. The video loads from YouTube when you press play.

Chapters

  1. 0:00The question
  2. 1:17The claim
  3. 2:19How the proof goes
  4. 3:23Where it stands

The claim, in plain words

Push on the surface of a solid body and measure how hard it pushes back. Do those measurements, taken all over the surface, tell you how stiff the material is everywhere inside? For an isotropic material, stiffness at each point is two numbers, the Lamé moduli lambda and mu, and the physical conditions are that mu and three lambda plus two mu are positive: resistance to shearing and to squeezing. Lambda itself can be negative; our computer finds that an auxetic foam has negative lambda and still qualifies. In a one-dimensional bar the data reveal only an average stiffness, but in a layered toy our computer finds that sideways variation tells a soft top from a stiff top.

In 1994 Nakamura and Uhlmann claimed global uniqueness in three dimensions; their 2003 erratum reduced the claim to materials whose mu varies slowly, matching a result of Eskin and Ralston. Since then the general case has been called open: in 2013, a significant unsolved problem; in 2022, an open problem. In two dimensions, Imanuvilov and Yamamoto settled it, and analytic or piecewise constant materials in three dimensions were handled by 2022.

Result 372 is one OpenAI paper, 24 pages, dated September 24 and made public October 6, 2026. It claims that on every bounded connected smooth domain in three dimensions, for smooth moduli with mu and three lambda plus two mu positive, if two materials give the same full static map from surface displacements to surface forces, then both moduli agree everywhere. No analyticity, no closeness to constants and no knowledge near the surface is assumed.

What it doesn’t claim

Not claimed: a way to reconstruct the moduli, a stability estimate, data on only part of the surface, or materials that are not isotropic. Four days after the release, Diao and Durdiev posted a 78-page proof of the same theorem, independent by their account, with a preliminary draft saved, by their records, two days before the release; they used ChatGPT for exploratory discussions, and they cite the OpenAI paper.

Where it stands

Posted as a preprint
OpenAI, 24 pages, dated September 24, 2026
Peer reviewed
Not yet; no specialist verdict
Formalized in Lean
The theorem, re-proving the cited boundary and Carleman inputs (scope notes)

Last checked October 19, 2026. The paper is unrefereed and unchanged since release, though it cites lecture notes dated October 2. The theorem has a Lean proof, about 32,000 lines, not run by us, which re-proves the boundary and Carleman inputs the paper cites. We found no specialist verdict. OSVerify has not reviewed it.

How the proof goes

  1. Glue, then probe with lopsided waves. Known results give the moduli and all their derivatives at the surface, so the two materials can be extended to agree outside, and solutions in one body can be glued to solutions in the other. A Carleman estimate then produces exact solutions that oscillate in one direction and grow exponentially in another, built from complex directions whose square is zero. As tau grows they become wildly lopsided: our computer finds a ratio of about half a billion between two points two units apart, at tau equal to ten.
  2. Forcing the comparison to be trivial. Comparing these solutions between the two bodies, and taking limits, gives a comparison matrix that is the identity outside and depends holomorphically on the complex direction. Geometry of those null directions forces the matrix to be the identity everywhere. That first recovers the ratio lambda plus mu over lambda plus two mu, which our computer confirms is a function of Poisson’s ratio alone; an ordinary differential equation argument then recovers mu, and with it lambda.

The numbers in the video

  • Ours: an auxetic foam has negative λ but positive μ and 3λ + 2μ, so it is inside the theorem's class.
  • Ours: in a layered toy, static data at k = 0 cannot tell a soft top from a stiff top, but with sideways variation the push-back per unit k tends to 2 versus 6.
  • Ours: (λ+μ)/(λ+2μ) = 1/(2(1−ν)), so the first quantity the proof recovers is Poisson's ratio.
  • Lean: 42 files and 31,645 lines in the import closure of the comparator's solution (counted by us; not run by us).

Read the source

The paper

OpenAI groups related papers into one result; this one has a single paper.

Transcript

Read the full script

0:00The question

Push on the surface of a solid body and measure how hard it pushes back. Do those measurements, taken all over the surface, tell you how stiff the material is everywhere inside? For an isotropic material, stiffness at each point is two numbers, the Lamé moduli lambda and mu, and the physical conditions are that mu and three lambda plus two mu are positive: resistance to shearing and to squeezing. Lambda itself can be negative; our computer finds that an auxetic foam has negative lambda and still qualifies. In a one-dimensional bar the data reveal only an average stiffness, but in a layered toy our computer finds that sideways variation tells a soft top from a stiff top. In 1994 Nakamura and Uhlmann claimed global uniqueness in three dimensions; their 2003 erratum reduced the claim to materials whose mu varies slowly, matching a result of Eskin and Ralston. Since then the general case has been called open: in 2013, a significant unsolved problem; in 2022, an open problem. In two dimensions, Imanuvilov and Yamamoto settled it, and analytic or piecewise constant materials in three dimensions were handled by 2022.

1:17The claim

Result 372 is one OpenAI paper, 24 pages, dated September 24 and made public October 6, 2026. It claims that on every bounded connected smooth domain in three dimensions, for smooth moduli with mu and three lambda plus two mu positive, if two materials give the same full static map from surface displacements to surface forces, then both moduli agree everywhere. No analyticity, no closeness to constants and no knowledge near the surface is assumed. Not claimed: a way to reconstruct the moduli, a stability estimate, data on only part of the surface, or materials that are not isotropic. Four days after the release, Diao and Durdiev posted a 78-page proof of the same theorem, independent by their account, with a preliminary draft saved, by their records, two days before the release; they used ChatGPT for exploratory discussions, and they cite the OpenAI paper.

2:19How the proof goes

Known results give the moduli and all their derivatives at the surface, so the two materials can be extended to agree outside, and solutions in one body can be glued to solutions in the other. A Carleman estimate then produces exact solutions that oscillate in one direction and grow exponentially in another, built from complex directions whose square is zero. As tau grows they become wildly lopsided: our computer finds a ratio of about half a billion between two points two units apart, at tau equal to ten. Comparing these solutions between the two bodies, and taking limits, gives a comparison matrix that is the identity outside and depends holomorphically on the complex direction. Geometry of those null directions forces the matrix to be the identity everywhere. That first recovers the ratio lambda plus mu over lambda plus two mu, which our computer confirms is a function of Poisson’s ratio alone; an ordinary differential equation argument then recovers mu, and with it lambda.

3:23Where it stands

The paper is unrefereed and unchanged since release, though it cites lecture notes dated October 2. The theorem has a Lean proof, about 32,000 lines, not run by us, which re-proves the boundary and Carleman inputs the paper cites. We found no specialist verdict. If it holds, complete static measurements on the surface of a smooth isotropic elastic body determine its stiffness everywhere inside, in three dimensions.

Spot a mistake?

This episode simplifies on purpose, but it shouldn’t be wrong. If something is, open an issue on GitHub or leave a comment on YouTube. Corrections are noted here with a date.