Abstract

The trigonometric monomial cos⁡(⟨k,x⟩)\cos(\left\langle k, x \right\rangle) on Td\mathbb{T}^d, a harmonic polynomial p:Sd−1→Rp: \mathbb{S}^{d-1} \rightarrow \mathbb{R} of degree kk and a Laplacian eigenfunction −Δf=k2f-Δf = k^2 f have root in each ball of radius ∼∥k∥−1\sim \|k\|^{-1} or ∼k−1\sim k^{-1}, respectively. We extend this to linear combinations and show that for any trigonometric polynomials on Td\mathbb{T}^d, any polynomial p∈R[x1,…,xd]p \in \mathbb{R}[x_1, \dots, x_d] restricted to Sd−1\mathbb{S}^{d-1} and any linear combination of global Laplacian eigenfunctions on Rd \mathbb{R}^d with d∈{2,3}d \in \left\{2,3\right\} the same property holds for any ball whose radius is given by the sum of the inverse constituent frequencies. We also refine the fact that an eigenfunction −Δϕ=λϕ- Δϕ= λϕ in Ω⊂RnΩ\subset \mathbb{R}^n has a root in each B(x,αnλ−1/2)B(x, α_n λ^{-1/2}) ball: the positive and negative mass in each B(x,βnλ−1/2)B(x,β_n λ^{-1/2}) ball cancel when integrated against ∥x−y∥2−n\|x-y\|^{2-n}.

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