English

Reciprocity and the Maslov Phase

Number Theory 2026-04-29 v1 Representation Theory

Abstract

We give a metaplectic proof of Hilbert reciprocity, and hence of quadratic reciprocity, in which the local phase is the Kashiwara--Maslov phase of a triple of Lagrangians. In rank two the phase of the ordered triple (L,La,L0)(L_\infty,L_a,L_0) is the one-dimensional Weil index γv(a)\gamma_v(a). The local Hilbert symbol appears as the defect of strict multiplicativity of these phases: (a,b)v=γv(a)γv(b)γv(1)γv(ab). (a,b)_v = \frac{\gamma_v(a)\gamma_v(b)}{\gamma_v(1)\gamma_v(ab)}. The global step compares the local and adelic realizations of a single Bruhat word for the diagonal torus elements m(a)SL2(Q)m(a)\in \operatorname{SL}_2(\mathbb Q). Locally the raw Bruhat-word lift carries the normalization factor determined by the chosen quadratic convention. These operators form a projective representation of the diagonal torus with defect μv(a,b)=γv(a)γv(b)γv(1)γv(ab). \mu_v(a,b) = \frac{\gamma_v(a)\gamma_v(b)}{\gamma_v(1)\gamma_v(ab)}. For rational adelic data, the normalized Bruhat word is multiplicative. The reciprocity law states that the total defect vμv(a,b)\prod_v\mu_v(a,b) is 11. Combined with the local bridge above, this yields Hilbert reciprocity, while quadratic reciprocity is then the specialization to the pair of odd primes (p,q)(p,q).

Cite

@article{arxiv.2604.25288,
  title  = {Reciprocity and the Maslov Phase},
  author = {Jonathan Holland},
  journal= {arXiv preprint arXiv:2604.25288},
  year   = {2026}
}

Comments

20 pages

R2 v1 2026-07-01T12:38:36.750Z