Leydold's conjecture on maximal nodal domains of spherical harmonics

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Let Hℓ\cal H_\ell be the eigenspace of spherical harmonics of degree ℓ\ell on the sphere, and let μ(u)\mu(u) denote the number of nodal domains of a spherical harmonic uu. Leydold's conjecture.

max⁡u∈Hℓμ(u)={12(ℓ+1)2if ℓ is odd,12ℓ(ℓ+2)if ℓ is even.\max_{u\in \mathcal H_\ell}\mu(u)=\left\{\begin{array}{ll}\frac{1}{2}(\ell+1)^2 & \text{if }\ell\text{ is odd},\\[4pt]\frac{1}{2}\ell(\ell+2) & \text{if }\ell\text{ is even.}\end{array}\right.

The right-hand side is attained by decomposed spherical harmonics in spherical coordinates. The conjecture was proved for ℓ≤6\ell\leq 6, but remains open in general; it would determine all possible maximal nodal-domain counts and has consequences for Courant-sharp eigenvalues and Pleijel-type bounds.

References

Primary source

Pierre Bérard and Bernard Helffer, “A. Stern's analysis of the nodal sets of some families of spherical harmonics revisited”, arXiv:1407.5564 (2015).

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