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Math-281 · mathematics · Pde

Sharp Upper Bound in Yau's Conjecture on Nodal Sets of Laplace Eigenfunctions

Status OpenLLM status Open unverified

Statement

Definitions and mathematical statement

For the usual connected-manifold formulation, let $\phi\ne0$ satisfy $-\Delta_g\phi=\lambda\phi$ on a smooth closed Riemannian $n$-manifold, $n\ge2$, and define its nodal set $Z(\phi)=\{x:\phi(x)=0\}$. The target upper estimate is \[ \mathcal H^{n-1}(Z(\phi))\le C(M,g)\sqrt\lambda \] for every positive eigenvalue and eigenfunction. Hausdorff measure measures the hypersurface-size of the zeros, and the constant is independent of the eigenfunction and eigenvalue. Scope qualification: connectedness is implicit in the standard statement but absent from the catalogue wording. On a disconnected manifold an eigenfunction can vanish identically on an entire component, making the literal bound false; use connected $M$ or explicitly restrict to components where the eigenfunction is nonzero. No analyticity of $g$ is assumed.

Formulation and concept references: [S1].

Short English statement

On a smooth connected closed manifold, is every eigenfunction's nodal hypersurface measure bounded by a constant times the square root of its eigenvalue?

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Statement licence: CC-BY-4.0 · Source file

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Math-281-A2 · Literature report · LLM-generated · unknown ·

OpenAI claim summary for Math-281

Power-law failure of nodal upper bounds: One fixed smooth connected closed metric and eigenfunctions of unbounded positive eigenvalue have unbounded nodal-measure-to-square-root-eigenvalue ratio. This directly negates the universal metric-dependent-constant assertion in our definition.

Nodal upper length on surfaces: The sharp nodal upper bound holds for all smooth closed connected surfaces, while the recorded target ranges over all smooth closed dimensions n at least two.

Nodal upper-bound failures in dimensions three and four: One fixed smooth connected closed metric and eigenfunctions of unbounded positive eigenvalue have unbounded nodal-measure-to-square-root-eigenvalue ratio. This directly negates the universal metric-dependent-constant assertion in our definition.

The claimed counterexample lies within the question’s hypotheses and contradicts its universal conclusion.

Sharp Upper Bound in Yau's Conjecture on Nodal Sets of Laplace Eigenfunctions

OpenAI's claim

Power-law failure of nodal upper bounds: The manuscript claims a fixed smooth metric on $S^4\times S^1$ with eigenfunctions whose nodal four-volume exceeds the square-root scale by a fixed positive power of the eigenvalue; this rules out even an arbitrary-small-power-loss version of the proposed general upper bound.

Nodal upper length on surfaces: The paper claims nodal length at most $C\sqrt\lambda$ for every real nonzero Laplace eigenfunction on a fixed smooth closed surface; combined with the established lower estimate, this settles the two-dimensional smooth setting.

Nodal upper-bound failures in dimensions three and four: The companion claims fixed smooth metrics on $S^3$ and $S^2\times\mathbb T^2$ with unbounded nodal-measure-to-$\sqrt\lambda$ ratios along exact eigenfunction sequences; the three-sphere metric may be chosen as close to round as prescribed in the smooth topology.

Mathematical statement of the claimed result

Mathematical claim 1.
On one fixed smooth metric $g$ on $S^4\times S^1$, the claim gives $\epsilon_0>0$ and nonzero real smooth eigenfunctions $u_j$ with \[-\Delta_gu_j=\lambda_ju_j,\qquad\lambda_j\to\infty,\qquad\frac{\mathcal H_g^4(\{u_j=0\})}{\lambda_j^{1/2+\epsilon_0}}\to\infty.\] Thus even a fixed positive power beyond the square-root nodal upper scale is exceeded along this sequence.
Mathematical claim 2.
Fix a smooth metric $g$ on a closed connected surface $M$. One finite $C(M,g)$ is asserted to work simultaneously for all nonzero real eigenfunctions solving $-\Delta_gu=\lambda u$, $\lambda>0$, satisfies \[\mathcal H_g^1(\{u=0\})\le C(M,g)\sqrt\lambda.\] The constant is shared by all eigenfunctions in all positive eigenspaces; the assertion is specific to surfaces.
Mathematical claim 3.
Every $C^\infty$ neighborhood of the round metric on $S^3$ is claimed to contain a smooth metric $g_\infty$ and real eigenfunctions $u_j$ with \[-\Delta_{g_\infty}u_j=\lambda_ju_j,\quad\lambda_j\to\infty,\quad\mathcal H_{g_\infty}^2(\{u_j=0\})/\sqrt{\lambda_j}\to\infty.\] The metric is fixed for the sequence. Taking its product with a fixed circle and extending $u_j$ constantly along that factor gives the stated corresponding four-dimensional failure.

Outline of the argument

Power-law failure of nodal upper bounds: A logarithmic envelope on the four-sphere is corrugated through a number of generations proportional to the logarithm of frequency, producing a power gain in its gradient integral. Complex phase and transport jets create highly accurate localized waves beneath that envelope. Exact metric and spectral corrections then realize genuine eigenfunctions while preserving the growing nodal score on one limiting metric.

Nodal upper length on surfaces: Subharmonic profile limits control local growth under affine subdivision. High-growth excursions along grid paths produce witness regions on which growth persists to terminal scale. A packing argument pays for witness regions outside their entry squares using summable collars, bounding the terminal average growth and hence nodal length.

Nodal upper-bound failures in dimensions three and four: Each construction starts with explicit high-frequency background modes and an untouched region that anchors spectral control. Corrugated logarithmic envelopes and finite complex-wave jets create quasimodes with a stable lower score from opposite-sign tests. Metric corrections make the waves exact, and a persistence argument passes to one fixed smooth metric without losing the score.

Formal verification

Family 350 describes Lean coverage for the surface upper bound and the three- and four-dimensional fixed-metric violations; the five-dimensional power-law refinement is separate.

Power-law failure of nodal upper bounds: The manuscript links NodalLength.lean, SmoothYau.lean (declaration OAI.YauCounterexamples.sphere_three), SmoothYau.lean (declaration OAI.YauCounterexamples.sphere_two_torus_two), YauCounterexample.lean (declaration OAI.Yau.Target.yau_nodal_set_upper_bound_counterexample).

The documented selection does not cover the entire manuscript assertion relevant here.

Nodal upper length on surfaces: The manuscript links NodalLength.lean, SmoothYau.lean (declaration OAI.YauCounterexamples.sphere_three), SmoothYau.lean (declaration OAI.YauCounterexamples.sphere_two_torus_two), YauCounterexample.lean (declaration OAI.Yau.Target.yau_nodal_set_upper_bound_counterexample).

The documented selection includes this manuscript’s main assertion; that assertion retains the restrictions stated above.

Nodal upper-bound failures in dimensions three and four: The manuscript links NodalLength.lean, SmoothYau.lean (declaration OAI.YauCounterexamples.sphere_three), SmoothYau.lean (declaration OAI.YauCounterexamples.sphere_two_torus_two), YauCounterexample.lean (declaration OAI.Yau.Target.yau_nodal_set_upper_bound_counterexample).

The documented selection includes this manuscript’s main assertion; that assertion retains the restrictions stated above.

This site has not run the Lean development. These links describe OpenAI’s selected formal statements and should be read with their stated scope.

Status caveat

OpenAI reports that an internal model produced the manuscripts. Their arguments have not been independently verified as proofs by this site. Any portion outside the documented formal scope may contain mistakes, and the catalogue label reports the announced mathematical claim.

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Math-281-A1 · Exploration · LLM-generated · gpt 6 astra ultra ·

gpt 6 astra ultra attempt on Math-281

Sharp Upper Bound in Yau's Conjecture on Nodal Sets of Laplace Eigenfunctions

Definitions and mathematical statement

For the usual connected-manifold formulation, let $\phi\ne0$ satisfy $-\Delta_g\phi=\lambda\phi$ on a smooth closed Riemannian $n$-manifold, $n\ge2$, and define its nodal set $Z(\phi)=\{x:\phi(x)=0\}$. The target upper estimate is \[ \mathcal H^{n-1}(Z(\phi))\le C(M,g)\sqrt\lambda \] for every positive eigenvalue and eigenfunction. Hausdorff measure measures the hypersurface-size of the zeros, and the constant is independent of the eigenfunction and eigenvalue. Scope qualification: connectedness is implicit in the standard statement but absent from the catalogue wording. On a disconnected manifold an eigenfunction can vanish identically on an entire component, making the literal bound false; use connected $M$ or explicitly restrict to components where the eigenfunction is nonzero. No analyticity of $g$ is assumed.

Formulation and concept references: [S1].

Short English statement

On a smooth connected closed manifold, is every eigenfunction's nodal hypersurface measure bounded by a constant times the square root of its eigenvalue?

Research attempt

Scope and source check.
This unresolved attempt by GPT-6 Astra Ultra was prepared on 27 September 2026 using Fourier calculations, explicit spherical harmonics and the primary review [S1]. The connectedness qualification in the statement is retained. The smooth-metric upper problem is distinct from the known sharp analytic-metric case and from the sharp lower estimate. Results for Euclidean Dirichlet domains or bi-Laplace equations also have different hypotheses and are not substituted for this closed-manifold problem. The attempt proves the sharp order on the standard flat torus and tests the tempting strategy of a uniform bound in every wavelength ball.

It is enough to discuss real eigenfunctions. If a complex eigenfunction is allowed, one of its real and imaginary parts is a nonzero real eigenfunction with the same eigenvalue, and the complex zero set is contained in that real zero set. An upper bound for the latter suffices. All examples and nodal hypersurface calculations below are real-valued.

A complete flat-torus estimate by one-dimensional zero counting.
Work on $\mathbb T^n=(\mathbb R/2\pi\mathbb Z)^n$ with its standard flat metric. Fourier expansion of $-\Delta\phi=\lambda\phi$ gives \[ \phi(x)=\sum_{|k|^2=\lambda}a_ke^{ik\cdot x}. \] There are finitely many such lattice vectors. Set $R=\lfloor\sqrt\lambda\rfloor$. On a coordinate circle, keeping all but $x_i$ fixed, the restriction is a trigonometric polynomial of degree at most $R$. Unless it vanishes identically on that circle, it has at most $2R$ distinct zeros: multiply its expression by $e^{iRx_i}$ and regard it as a polynomial of degree at most $2R$ in $e^{ix_i}$.

For each coordinate direction, the exceptional parameter values giving an identically zero restriction have $(n-1)$-dimensional measure zero. Indeed all the coefficient trigonometric polynomials in the other variables would have to vanish there, and at least one of those coefficients is nonzero because $\phi\ne0$. The zero set of a nonzero trigonometric polynomial has measure zero. That last fact can be proved inductively by the same one-variable zero count and Fubini, treating identically zero slices in the next lower dimension.

We use the standard nodal-structure fact for nonzero analytic Laplace eigenfunctions, reviewed in [S1]: the regular nodal hypersurface is smooth, and its singular part has zero $(n-1)$-dimensional Hausdorff measure. Let $\nu$ be a unit normal on its regular part. The coarea formula for projection omitting coordinate $i$ gives \[ \int_{Z_{\rm reg}}|\nu_i|\,d\mathcal H^{n-1} =\int_{\mathbb T^{n-1}}\#\left(Z_{\rm reg}\cap \text{the corresponding coordinate circle}\right) \,dx_{\widehat i} \le2R(2\pi)^{n-1}. \] Exceptional slices do not contribute to this integral. Since a unit vector satisfies $\sum_i|\nu_i|\ge1$, summing the inequalities yields \begin{equation}\label{wsref-0-61-32-37-37-3a-74-6f-72-75-73} \mathcal H^{n-1}(Z(\phi)) \le2n(2\pi)^{n-1}\sqrt\lambda. \end{equation} Thus the conjectured exponent is proved for every eigenfunction on this flat torus, including arbitrary linear combinations within a high-multiplicity eigenspace. No claim that such combinations have only the zeros of their individual Fourier modes is made.

Exact examples check the scale and constants.
For $\phi(x)=\sin(mx_1)$, there are $2m$ parallel nodal subtori, each of measure $(2\pi)^{n-1}$, and $\lambda=m^2$. Hence \[ \mathcal H^{n-1}(Z(\phi))=2(2\pi)^{n-1}\sqrt\lambda. \] The square-root order cannot be improved even within this family. For another check on the two-dimensional torus, $\phi(x,y)=\sin(mx)\sin(\ell y)$ has eigenvalue $m^2+\ell^2$. Its nodal set is a union of $2m$ vertical and $2\ell$ horizontal circles. Their finitely many intersections have zero length, so \[ \mathcal H^1(Z)=4\pi(m+\ell) \le4\pi\sqrt2\sqrt{m^2+\ell^2}. \] This confirms that adding crossing families changes the constant but not the exponent. Counting each grid intersection as another curve segment would double-count a measure-zero part.

The normalization matters. Using period one instead of $2\pi$ changes both the eigenvalue formula and the geometric measure. The estimate above fixes both conventions before counting zeros, so no frequency factor $2\pi$ is lost when comparing with $\sqrt\lambda$.

A proposed wavelength-ball shortcut fails on the sphere.
Suppose one could cover a general manifold by $O(r^{-n})$ balls of radius $r=\lambda^{-1/2}$ and bound nodal measure in every such ball by $Cr^{n-1}$, with $C$ depending only on the metric. Summation would immediately give $C/r=C\sqrt\lambda$. Unfortunately the proposed local bound is false, including on the analytic round sphere where the desired global bound is true.

On $S^2\subset\mathbb R^3$, take \[ \phi_m=\operatorname{Re}(x_1+ix_2)^m. \] The homogeneous polynomial is harmonic in $\mathbb R^3$, so its restriction has eigenvalue $m(m+1)$. Its zeros are $m$ distinct great circles through the north and south poles. Distinct circles intersect only at the poles, a length-zero set. Thus the total nodal length is $2\pi m$, of the desired global order.

But a geodesic ball of radius $r<\pi/2$ centered at the north pole contains two radial arcs of length $r$ from each circle. Its nodal length is exactly $2mr$. At wavelength radius $r=[m(m+1)]^{-1/2}$ this remains comparable to two, whereas the proposed uniform local bound $Cr$ tends to zero. The quotient of the actual local length by $r$ is $2m$, unbounded. High vanishing order at one point obstructs a uniform per-ball constant even though it does not violate the global conjecture.

This example also explains why a compactness argument over normalized wavelength-scale functions cannot assume bounded vanishing order. The metric is fixed throughout, while the eigenvalue and the local multiplicity increase. Normalizing an $L^2$ norm does not remove the many meridian sheets near the pole.

A more realistic conditional summation criterion.
Let $r=c\lambda^{-1/2}$ be below a fixed coordinate radius and choose a covering by $O(r^{-n})$ balls. Suppose one has numbers $N_j\ge1$ measuring local oscillation or doubling, together with two estimates \[ \mathcal H^{n-1}(Z\cap B_j)\le C N_j r^{n-1}, \qquad \sum_jN_j\le C' r^{-n}. \] Then summing proves $\mathcal H^{n-1}(Z)\le CC' r^{-1}=O(\sqrt\lambda)$. This deduction is exact. Neither displayed hypothesis is asserted here for all smooth metrics. The first is a linear local nodal estimate; the second is a bound on the average complexity across the cover, not a uniform bound on each $N_j$.

The spherical example is compatible with exceptional large $N_j$ near a small set of poles, but not with their uniform boundedness. A worst-case global frequency bound at each ball, multiplied by the full number of balls, loses precisely the distributional information needed for the sharp exponent. Known polynomial estimates in frequency do not turn into linear estimates by renaming their constants. A successful implementation must account quantitatively for how high-complexity balls are distributed.

Harmonic lifting is useful but does not supply that estimate.
Define on the product manifold $M\times\mathbb R$ \[ u(x,t)=e^{\sqrt\lambda t}\phi(x). \] For the product metric, $\Delta_{M\times\mathbb R}u=e^{\sqrt\lambda t} (\Delta_M\phi+\lambda\phi)=0$. Its zero set is $Z(\phi)\times\mathbb R$. Thus harmonic-function estimates can be applied to the lifted problem, with explicit exponential growth in the new direction. On a product interval of length $L$, the regular zero-set measure is $L\mathcal H^{n-1}(Z(\phi))$, with the singular part negligible in the standard nodal framework.

The lift does not make the metric analytic when $g$ is only smooth. Nor does it guarantee a linear relationship between a doubling index and nodal measure. It is a correct change of equation that transfers the central quantitative difficulty. The Fourier proof of (a277:torus) used a finite frequency band on every coordinate circle; restrictions of eigenfunctions to geodesics for a general smooth metric need not be trigonometric polynomials of bounded degree. Applying their one-dimensional polynomial zero count would therefore be unjustified.

Boundary cases and verification.
Connectedness prevents a nonzero eigenfunction from vanishing identically on an entire separate component, the literal obstruction already noted in the catalogue. Positive eigenvalues exclude the constant-function case. Finitely many low eigenvalues can be absorbed into a metric- dependent constant when using the wavelength cover; this does not address the high-frequency estimate. The proof and tests separately track hypersurface measure, isolated crossing points, eigenvalue normalization and singular nodal points.

Exact finite checks verify the torus grid formulas, the eigenvalue and local length of the spherical example, and the powers of $r$ in the conditional sum. The analytic nodal-structure and coarea inputs are stated explicitly. The strongest result is the all-eigenfunction flat- torus estimate, plus a concrete disproof of a tempting uniform local shortcut. The first remaining gap is a sharp quantitative local-to-global mechanism for arbitrary smooth metrics, such as the two-part summation package above. The catalogue's smooth upper-bound assertion remains UNRESOLVED.

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