Abstract

For a set E⊂FqdE\subset \mathbb F_q^d, we define the kk-resultant magnitude set as Δk(E)={∥x1+⋯+xk∥∈Fq:x1,…,xk∈E}, Δ_k(E) =\{\|\textbf{x}_1 + \dots + \textbf{x}_k\|\in \mathbb F_q: \textbf{x}_1, \dots, \textbf{x}_k \in E\}, where ∥v∥=v12+⋯+vd2\|\textbf{v}\|=v_1^2+\cdots+ v_d^2 for v=(v1,…,vd)∈Fqd.\textbf{v}=(v_1, \ldots, v_d) \in \mathbb F_q^d. In this paper we find a connection between a lower bound of the cardinality of the kk-resultant magnitude set and the restriction theorem for spheres in finite fields. As a consequence, it is shown that if E⊂FqdE\subset \mathbb F_q^d with ∣E∣≥Cqd+12−16d+2,|E|\geq C q^{\frac{d+1}{2}-\frac{1}{6d+2}}, then ∣Δ3(E)∣≥cq|Δ_3(E)|\geq c q for d=4d = 4 or d=6d = 6, and ∣Δ4(E)∣≥cq|Δ_4(E)| \geq cq for even dimensions d≥8.d \geq 8. In addition, we prove that if d≥8d\geq 8 is even, and ∣E∣≥Cε qd+12−19d−18+ε|E|\geq C_\varepsilon ~q^{\frac{d+1}{2} - \frac{1}{9d -18} + \varepsilon} for ε>0\varepsilon >0, then ∣Δ3(E)∣≥cq.|Δ_3(E)|\geq c q.

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