A smooth surface metric with no local isometric immersion in ℝ3

Some smooth rules for measuring length cannot be built as a surface in space, even near one point.

1 paper September 24, 2026 Explained by AI

A metric is a rule for measuring lengths on a flat region. The question is whether a small curved surface in space can carry those exact lengths. The paper proves that for some smooth metric, no such surface exists near the center, however small. The paper also claims the metric can match flat lengths to every order at the center. A Lean proof of the main statement is listed.

First step
1971
A. V. Pogorelov, a less smooth metric with no local surface
Significance
Major
If the proof holds, it answers a smooth local problem that Ghomi's 2019 survey lists as open.
Trust
Formal proof listed
Field
Differential geometry
1 paper

The explanation

Picture the saddle surface z = xy, shaped like a riding saddle. An ant living on it can measure distances along the surface. From distances alone, it can compute the Gaussian curvature [a number saying how the surface bends near a point]. Negative means saddle-shaped, positive means dome-shaped, and zero means flat like paper. On this saddle the curvature is −1 at the center. Above the point (1, 1) it is −1/9. Above (2, 0) it is −1/25.

Now run the question backwards. Start with only a metric [a rule giving the length of every short path in a flat region]. Can you always build a surface in ordinary three-dimensional space with exactly those lengths? Ask only for a small piece around one point. Such a piece is a local isometric immersion [a smooth map into space that keeps every length]. An immersion may cross itself, but near a single point it cannot. So allowing or forbidding self-crossings gives the same local question.

Much was known. Take analytic metrics [ones given by convergent power series]. Janet and Cartan showed in 1926 and 1927 that the answer is yes. For smooth metrics [ones with derivatives of every order], the answer is yes where curvature is not zero. Trouble starts where the curvature hits zero. There the governing equation can change character. On one side it behaves like a stretched membrane, on the other like waves. Nakamura and Maeda in 1989 handled a clean sign change, where curvature crosses zero at a nonzero slope.

Smoothness matters at both ends. Nash and Kuiper showed that with only one derivative required, a local surface always exists. In 1971 Pogorelov built a metric with limited smoothness and no local surface with two derivatives. Nadirashvili and Yuan published a refinement in 2008 with curvature never negative. The fully smooth question stayed open. Yau discussed it, and Ghomi's 2019 survey lists it as a problem. A 2002 preprint by Nadirashvili and Yuan claimed a stronger counterexample, but their later paper calls the question open. This paper leaves that discrepancy unresolved and does not use the preprint's claim.

The paper proves the answer is no. It builds a smooth metric on the open square from −1 to 1 in both directions. No neighborhood of the center, however small, has a smooth surface with those lengths. The paper also claims the metric can match the flat metric to every order at the center. A flat plane realizes the flat metric. So the metric's derivatives at that one point cannot decide the question.

One subtle point is that smoothness must hold on a single fixed piece. Having a solution with any finite number of derivatives is not enough. Those solutions may live on pieces that shrink as the number grows. The paper must rule out every smooth candidate on every neighborhood at once.

The construction places a chain of tiny disks marching toward the center. Disk number j is centered at distance 1/2^j, with radius 1/2^(j+4). Disk 1 sits at 0.5 with radius 1/32, about 0.031. Disk 10 sits at about 0.00098 with radius about 0.000061. Each radius is 1/16 of its distance from the center. Inside each disk the curvature is negative, and on its rim it is zero. Any surface built near the center would contain one whole disk. A short argument from the 2002 preprint, re-proved here, then forces a special one-direction bending somewhere on that rim.

Just outside each disk, the paper places tiny square patches that crowd toward every rim point, tilted at many angles. Each patch gets a carefully perturbed metric. A height function records how far the surface rises in one fixed direction. On each patch, no height of the kind that bending produces can solve an equation every such surface obeys. So the surface cannot exist. The paper gets suitable patch metrics from Baire category, a general existence argument. It writes no formula for them. Its curvature also takes both signs. So it does not settle the smooth question when curvature must be never negative, or never positive.

How sure is this? A computer proof checker called Lean has checked a formal version of the main statement. It says no neighborhood of the center has a smooth surface with these lengths. The Lean scope note does not mention the flat-matching refinement, so that part sits outside the check. No specialist review has been published.

What it doesn't show. This does not settle metrics whose curvature is never negative, or never positive. The example uses both signs.

Where it came from

This result comes from an unreleased OpenAI model, published in the openai/math release on 6 October 2026.

Hype check

Major if the proof holds. A Lean proof of the main statement is listed, but the flat-matching refinement is outside the scope note. The example uses curvature of both signs, so the one-sign cases remain open. No specialist review has been published.

Words used

Metric
A rule that gives the length of every short path in a region.
Gaussian curvature
A number at each point saying how a surface bends: negative for a saddle, positive for a dome, zero for flat.
Isometric immersion
A smooth map of a region into space that keeps every length unchanged.
Smooth
Having derivatives of every order.
Analytic
Given near each point by a convergent power series, which is stricter than smooth.
Neighborhood
Any small open region around a point.
Taylor jet
The full list of derivatives of every order at a single point.

The original paper

All quoted lines (13)

  1. We leave this discrepancy unresolved.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  2. We do not use the preprint's nonsolvability assertion; the construction below supplies its own analytic obstruction.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  3. There is a C∞C^\infty positive definite Riemannian metric gg on (−1,1)2(-1,1)^2 such that no open neighborhood UU of the origin admits a C∞C^\infty isometric immersion F:(U,g)⟶R3.F:(U,g)\longrightarrow\R^3.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  4. No completeness or topological assumption is involved in Theorem A. The metric can moreover be chosen to have the same full Taylor jet at the origin as the Euclidean metric; see ….
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  5. Thus smooth local realizability is not determined by that jet.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  6. Existence at every finite differentiability order, on neighborhoods allowed to shrink with that order, does not by itself give one smooth map on a fixed neighborhood.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  7. Let Dj\mathcal D_j, j≥1j\ge1, be the round disks with centers (2−j,0)(2^{-j},0) and radii 2−j−42^{-j-4}.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  8. For each orientation in a fixed finite net, place shrinking obstructed patches approaching every boundary point of a disk with negative curvature inside and zero curvature on its boundary.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  9. The geometric construction uses the boundary-saddle argument of Nadirashvili and Yuan: a negatively curved disk cannot be a graph whose second fundamental form vanishes along its entire boundary.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  10. For each orientation in a fixed finite net, place shrinking obstructed patches approaching every boundary point of a disk with negative curvature inside and zero curvature on its boundary.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  11. In particular, for every C∞C^\infty neighborhood of g0g_0 in U\mathcal U, there is a metric in that neighborhood with no admissible height.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  12. In Theorem A, positive definiteness refers to the metric, not its curvature: the construction uses both signs of curvature.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text
  13. It does not settle the smooth local-realizability problem under either sign restriction K≥0K\ge0 or K≤0K\le0.
    A Smooth Metric with No Local Isometric Immersion into Three-Space Back to text

Other sources

  1. M. Janet, “Sur la possibilité de plonger un espace riemannien donné dans un espace euclidien”, Ann. Soc. Polon. Math. 5 (1926), 38–43
  2. G. Nakamura and Y. Maeda, “Local smooth isometric embeddings of low-dimensional Riemannian manifolds into Euclidean spaces”, Trans. AMS 313 (1989), 1–51
  3. J. Nash, “C¹ isometric imbeddings”, Annals of Mathematics 60 (1954), 383–396
  4. A. V. Pogorelov, “An example of a two-dimensional Riemannian metric admitting no local realization in E³”, Doklady Akad. Nauk SSSR 198 (1971), 42–43
  5. N. Nadirashvili and Y. Yuan, “Improving Pogorelov's isometric embedding counterexample”, Calc. Var. PDE 32 (2008), 319–323
  6. N. Nadirashvili and Y. Yuan, “Counterexamples for Local Isometric Embedding”, arXiv:math/0208127 (2002)
  7. M. Ghomi, “Open problems in geometry of curves and surfaces” (2019), Section 1.5, Problem 1.9
  8. S.-T. Yau, “Review of geometry and analysis”, Asian Journal of Mathematics 4 (2000), 235–278
  9. openai/math, “A Smooth Metric with No Local Isometric Immersion into Three-Space” and Lean scope note (2026) We give a negative answer to this local three-dimensional problem.
  10. É. Cartan, “Sur la possibilité de plonger un espace riemannien donné dans un espace euclidien”, Ann. Soc. Polon. Math. 6 (1927), 1–7