geometry-topology / Spectral geometry; nodal sets of Laplace eigenfunctions

Yau's nodal-set conjecture for smooth metrics: is nodal measure comparable to sqrt(lambda)?

Dimensions three and four (Theorems 1.1, 1.2 of the principal manuscript): a smooth metric arbitrarily close to the round metric on S3S^3, and one on S2×T2S^2\times T^2, with exact eigenfunctions whose nodal measure divided by λ\sqrt\lambda is unbounded. Dimension five and up (companion): a metric on S4×S1S^4\times S^1 with nodal measure ≫λ1/2+ϵ0\gg\lambda^{1/2+\epsilon_0} for a fixed ϵ0>0\epsilon_0>0, and products give every dimension above five. Surfaces (companion): H1(Zu)≤C(M,g)λ\mathcal H^1(Z_u)\le C(M,g)\sqrt\lambda, so with Bruning's lower bound Yau's conjecture holds in dimension two. So the upper bound is true for surfaces and false for smooth metrics in every dimension ≥3\ge3; the lower bound (Logunov) is untouched, and real-analytic metrics are unaffected. No power excess is claimed in dimensions 3 and 4.

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geometry-topologySep 23, 2026Significance 58/100Registry: lean checked

Yau's nodal-set conjecture for smooth metrics: is nodal measure comparable to sqrt(lambda)?

Prior state unknown→disproved

Dimensions three and four (Theorems 1.1, 1.2 of the principal manuscript): a smooth metric arbitrarily close to the round metric on S3S^3, and one on S2×T2S^2\times T^2, with exact eigenfunctions whose nodal measure divided by λ\sqrt\lambda is unbounded. Dimension five and up (companion): a metric on S4×S1S^4\times S^1 with nodal measure ≫λ1/2+ϵ0\gg\lambda^{1/2+\epsilon_0} for a fixed ϵ0>0\epsilon_0>0, and products give every di…

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Dimensions three and four (Theorems 1.1, 1.2 of the principal manuscript): a smooth metric arbitrarily close to the round metric on S3S^3, and one on S2×T2S^2\times T^2, with exact eigenfunctions whose nodal measure divided by λ\sqrt\lambda is unbounded. Dimension five and up (companion): a metric on S4×S1S^4\times S^1 with nodal measure ≫λ1/2+ϵ0\gg\lambda^{1/2+\epsilon_0} for a fixed ϵ0>0\epsilon_0>0, and products give every dimension above five. Surfaces (companion): H1(Zu)≤C(M,g)λ\mathcal H^1(Z_u)\le C(M,g)\sqrt\lambda, so with Bruning's lower bound Yau's conjecture holds in dimension two. So the upper bound is true for surfaces and false for smooth metrics in every dimension ≥3\ge3; the lower bound (Logunov) is untouched, and real-analytic metrics are unaffected. No power excess is claimed in dimensions 3 and 4.

Dimensions three and four (Theorems 1.1, 1.2 of the principal manuscript): a smooth metric arbitrarily close to the round metric on S3S^3, and one on S2×T2S^2\times T^2, with exact eigenfunctions whose nodal measure divided by λ\sqrt\lambda is unbounded. Dimension five and up (companion): a metric on S4×S1S^4\times S^1 with nodal measure ≫λ1/2+ϵ0\gg\lambda^{1/2+\epsilon_0} for a fixed ϵ0>0\epsilon_0>0, and products give every dimension above five. Surfaces (companion): H1(Zu)≤C(M,g)λ\mathcal H^1(Z_u)\le C(M,g)\sqrt\lambda, so with Bruning's lower bound Yau's conjecture holds in dimension two. So the upper bound is true for surfaces and false for smooth metrics in every dimension ≥3\ge3; the lower bound (Logunov) is untouched, and real-analytic metrics are unaffected. No power excess is claimed in dimensions 3 and 4.

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