English

The Collision Spectrum

General Mathematics 2026-04-02 v1

Abstract

For a prime base bb and primitive odd Dirichlet character χ\chi modulo b2b^2, the collision transform coefficient S^(χ)\hat{S}^{\circ}(\chi) admits an exact factorization: S^(χ)=B1,χSG(χ)ϕ(b2), \hat{S}^{\circ}(\chi) = -\frac{B_{1,\overline{\chi}} \cdot \overline{S_G(\chi)}}{\phi(b^2)}, where B1,χB_{1,\overline{\chi}} is the generalized first Bernoulli number and SG(χ)S_G(\chi) is the diagonal character sum. By the standard Bernoulli--LL-value formula, B1=(b/π)L(1,χ)|B_1| = (b/\pi)\, |L(1, \chi)|, so the collision invariant's Fourier spectrum encodes LL-function special values. A Parseval identity gives an exact formula for the weighted second moment L(1,χ)2SG(χ)2\sum |L(1, \chi)|^2 \cdot |S_G(\chi)|^2 in terms of the collision invariant's values on the finite group. The digit function computes this LL-value moment exactly. Under a conditional zero-free hypothesis, the triangle inequality yields a separate bound connecting L(1)L(1) to L(s)L(s) for ss in the critical strip. At base~55, the factorization gives S^L(1)2|\hat{S}^{\circ}| \propto |L(1)|^2 exactly. For quadratic characters in the family, the decomposition specializes to class-number data.

Keywords

Cite

@article{arxiv.2604.00054,
  title  = {The Collision Spectrum},
  author = {Alexander S. Petty},
  journal= {arXiv preprint arXiv:2604.00054},
  year   = {2026}
}

Comments

6 pages

R2 v1 2026-07-01T11:46:55.372Z