The line counting function $f(x) = \sum_{L \in \mathcal{L}} \mathbf{1}_L(x)$, counting how many lines from $\mathcal{L}$ pass through the point $x \in \mathbb{F}_p^2$.
Instances For
Exact inner product of the mean-zero indicator residues of two lines $L_1, L_2$ (each of size $p$): $\sum_x (\mathbf{1}_{L_1}(x) - p^{-1})(\mathbf{1}_{L_2}(x) - p^{-1}) = |L_1 \cap L_2| - 1$.
If two distinct lines $L_1, L_2$ in $\mathbb{F}_p^2$ intersect in at most one point then the cross-term inner product of their mean-zero indicator residues is $\leq 0$.
$L^2$ bound on the high-frequency part: if every pair of distinct lines in $\mathcal{L}$ meets in at most one point, then $\sum_{x \in \mathbb{F}_p^2} f_h(x)^2 \leq |\mathcal{L}| \cdot p$.
Main Lemma 2F (finite field Fourier line decomposition). For a collection $\mathcal{L}$ of lines in $\mathbb{F}_p^2$ (each of size $p$, pairwise intersecting in at most one point), the line-counting function $f = \sum_{L \in \mathcal{L}} \mathbf{1}_L$ admits a decomposition $f = f_0 + f_h$ into a constant part $f_0 = |\mathcal{L}|/p$ and a mean-zero high-frequency part $f_h$ with: (i) orthogonality $\sum_x f_0 f_h = 0$, (ii) $\sum_x f_0^2 = |\mathcal{L}|^2$, and (iii) the $L^2$ bound $\sum_x f_h^2 \leq |\mathcal{L}| \cdot p$.