Under reviewFluid dynamics3 min read

Navier–Stokes: a new proof claim, and a dispute over credit

A fluid singularity, a Lean certificate, and two accounts of the race.

OpenAI · Tristan Buckmaster · Levent Alpöge

Where this stands

A newly released mathematical claim with a public formal artifact. This page does not assert that Clay has accepted a solution or awarded a prize.

Start with the question

The problem

Can a three-dimensional incompressible viscous fluid that starts smoothly develop a singularity in finite time? Clay’s official formulation includes breakdown alternatives with smooth external forcing, as well as global-existence alternatives.

∂tu+(u⋅∇)u=−∇p+ν Δu+f∇⋅u=0\begin{gathered} \partial_t u + (u \cdot \nabla) u = -\nabla p + \nu\, \Delta u + f \\ \nabla \cdot u = 0 \end{gathered}

Before the news

Understand the mathematics

The established mathematics behind the story, step by step. What is new, and who claims it, follows below with sources.

Reading the equation

Here u(x,t)∈R3u(x, t) \in \mathbb{R}^3 is the velocity of the fluid at the point xx and time tt, pp is the pressure, ν>0\nu > 0 the viscosity and ff an external force. The left side is the acceleration of a fluid particle: ∂tu\partial_t u is the change at a fixed point, and (u⋅∇)u(u \cdot \nabla) u the change from being carried along by the flow. This term is quadratic in uu, and it is the source of all the difficulty.

The condition ∇⋅u=0\nabla \cdot u = 0 says the fluid is incompressible. The pressure is then not a separate unknown: taking the divergence of the equation gives

−Δp=∑i,j∂i∂j(uiuj)−∇⋅f.-\Delta p = \sum_{i,j} \partial_i \partial_j (u_i u_j) - \nabla \cdot f.
What is known: energy

For a smooth solution, multiplying the equation by uu and integrating over space gives the energy balance

12∥u(t)∥L22+ν∫0t∥∇u(s)∥L22 ds=12∥u0∥L22+∫0t ⁣ ⁣∫f⋅u dx ds.\begin{aligned} &\tfrac12 \|u(t)\|_{L^2}^2 + \nu \int_0^t \|\nabla u(s)\|_{L^2}^2 \, ds \\ &\quad = \tfrac12 \|u_0\|_{L^2}^2 + \int_0^t \!\! \int f \cdot u \, dx \, ds. \end{aligned}

Viscosity removes energy, and the force can add it. In 1934 Leray used this bound to construct weak solutions that exist for all time, but nobody knows whether they stay smooth or are unique.

Why three dimensions is hard

Without a force, if uu solves the equation then so does the rescaled flow

uλ(x,t)=λ u(λx,λ2t)for every λ>0.u_\lambda(x, t) = \lambda\, u(\lambda x, \lambda^2 t) \qquad \text{for every } \lambda > 0.

In three dimensions its energy is ∥uλ(t)∥L22=λ−1∥u(λ2t)∥L22\|u_\lambda(t)\|_{L^2}^2 = \lambda^{-1} \|u(\lambda^2 t)\|_{L^2}^2. Zooming in to small scales (large λ\lambda) makes the energy small, so the one quantity we control says almost nothing about the tiny scales where a singularity would form. This is called supercriticality. In two dimensions the energy does not change under this scaling, and smooth solutions are known to exist for all time.

The four ways to win the Clay prize

The official problem is solved by proving any one of four statements: (A) smooth solutions exist for all time on R3\mathbb{R}^3 for every smooth, rapidly decaying initial velocity, with f=0f = 0; (B) the same on the periodic box T3\mathbb{T}^3; (C) on R3\mathbb{R}^3 there are a smooth initial velocity and a smooth, decaying force ff for which no smooth solution with finite energy exists for all time; (D) the same breakdown on T3\mathbb{T}^3.

Alternatives C and D allow a force. That is why a construction with a smooth force can address the Millennium Problem while saying nothing about whether an unforced fluid can blow up.

01

Read the claim precisely

On 8 September, OpenAI announced a construction intended to establish alternatives C and D of the Millennium Problem. It involves a smooth applied force. This does not establish blowup for the unforced viscous equation. The distinction is part of the problem statement, rather than a technicality to leave out of the story. [1][3]

02

From Euler to viscosity

OpenAI reports that coordinating agents first found an unforced Euler construction, then used that progress to pursue Navier–Stokes. The company describes an 88-hour search followed by 17 hours of formalization. Those timings are its own account. The repository supplies separate Euler and Navier–Stokes developments and comparator challenges. [1][2]

03

Why the announcement became contentious

Buckmaster’s statement raised concerns about research priority, private Codex sessions, and proposed authorship arrangements. OpenAI says neither its researchers nor its agents saw the pair’s work before publication and denies looking up specific user data. Its statement leaves open whether de-identified usage data contributed to model improvement. These are conflicting public accounts, not an established finding of misconduct. [4][1]

Inspect the evidence

The Lean formalization

Lean artifact released; independent assessment ongoing

The repository states whole-space and periodic results for every positive viscosity, with smooth forcing, and supplies comparator instructions. Checking the formal statement against Clay’s hypotheses is essential. We reviewed the documentation, not a local rebuild of the proof.

Sources & further reading

Reviewed 9 Sept 2026. X permalinks were recovered from indexed posts and linked discussions; direct X pages were not consistently accessible. They document the conversation, not proof correctness.

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    Levent Alpöge’s response ↗X post

    Read alongside Buckmaster’s statement and OpenAI’s response. Allegations remain attributed to their authors.

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