Paraboloid L2L^2 extension range conjecture

Let q=Fqq=|\mathbb F_q|, and let PFqdP\subset \mathbb F_q^d be the paraboloid

P={ξFqd:ξd=ξ12++ξd12}.P=\{\xi\in \mathbb F_q^d:\xi_d=\xi_1^2+\cdots+\xi_{d-1}^2\}.

Write RP(pr)1R_P^*(p\to r)\lesssim 1 when the finite-field extension operator for PP is bounded from Lp(P)L^p(P) to Lr(Fqd)L^r(\mathbb F_q^d) uniformly in qq. The L2L^2 extension range conjecture. The following equivalences hold: if d2d\geq 2 is even, then RP(2r)1R_P^*(2\to r)\lesssim 1 if and only if 2d+4dr\frac{2d+4}{d}\leq r\leq\infty; if d=41d=4\ell-1 for N\ell\in\mathbb N and 1Fq-1\in\mathbb F_q is not a square, then RP(2r)1R_P^*(2\to r)\lesssim 1 if and only if 2d+6d+1r\frac{2d+6}{d+1}\leq r\leq\infty; if d=4+1d=4\ell+1 for N\ell\in\mathbb N, then RP(2r)1R_P^*(2\to r)\lesssim 1 if and only if 2d+2d1r\frac{2d+2}{d-1}\leq r\leq\infty; and if d3d\geq 3 is odd and 1Fq-1\in\mathbb F_q is a square, then RP(2r)1R_P^*(2\to r)\lesssim 1 if and only if 2d+2d1r\frac{2d+2}{d-1}\leq r\leq\infty. The reverse implications follow from the paper's necessary-condition lemma, while the forward implications are known in dimension two but remain open in higher even dimensions.

Sources & referencesView supporting material

Primary source

Doowon Koh, “Conjecture and improved extension theorems for paraboloids in the finite field setting”, arXiv:1603.06512 (2017).

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