Sharp 3-energy bound for Katz–Tao sets on the parabolic cylinder
Establish that every δ-separated (δ, d)-Katz–Tao set S contained in the truncated parabolic cylinder Y = {(x, x², z) : x ∈ [0, 1], z ∈ [0, 1]} ⊂ R³, with 1 < d ≤ 2, satisfies E₃,δ(S) ≲ε δ⁻ε max{δ⁻(3d+2), δ⁻(5d−1)} for every ε > 0.
References
The analogous conjecture we make for a (δ, d)-KT set S ⊂ Y, 1 < d ≤ 2, is E3,δ(S) ≲ε δ−ε max{δ−(3d+2), δ−(5d−1)}.
— Sharp $L^6$ Fourier moments and (3,$δ$)-energy estimates for fractal measures on the truncated cone in $\R^3$
(2610.23679 - Demeter, 16 Oct 2026) in Section 1.2, equation (9), p. 3