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Unconditional Density Bounds for Quadratic Norm-Form Energies via Lorentzian Spectral Weights

Published 27 Feb 2026 in math.NT | (2603.00301v1)

Abstract: For a real quadratic field Q(d)\mathbb{Q}(\sqrt{d}), we study the norm-form energy N=Sζ<sup>2</sup>dSL<sup>2N = S_ζ<sup>2</sup> - d \cdot S_L<sup>2, where SζS_ζ and SLS_L are Lorentzian-weighted zero sums with w(ρ)=2/(1/4+γ<sup>2)w(ρ) = 2/(1/4 + γ<sup>2). We prove three main results. (1) Spacelike spectral data: $N &lt; 0$ unconditionally for all squarefree $d &gt; 1$, as a consequence of a low-lying zero dominance theorem proved via explicit zero-counting. (2) Effective density bound: at each verified truncation level MM, $\mathrm{dens}{N &gt; 0} \leq 2|f_{S_L<sup>{(M)}}|_\infty</sup> \cdot (W_1(ζ)/\sqrt{d} + ε<em>M)$, established unconditionally via Jacobi--Anger resonance analysis. (3) Exact asymptotic: under the computationally verified hypothesis that the infinite resonance lattice Λ</em>Λ</em>\infty has finite rank (verified for M20M \leq 20, where rank =0= 0), the sharp asymptotic $\mathrm{dens}{N &gt; 0} = C(d)/\sqrt{d} + o(1/\sqrt{d})$ holds. For d=5d = 5, C(5)=2fSL(0)E[Sζ]=0.1191C(5) = 2\,f_{S_L}(0)\cdot\mathbb{E}[|S_ζ|] = 0.1191; the constant depends on dd through the zeros of L(s,χd)L(s,χ_d), and C(d)=O(1/logd)C(d) = O(1/\log d) as dd \to \infty.

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