What question did this study set out to answer?

The main aim is to demonstrate the limitations of the point spectrum in first-order perturbations and resolve it using the Schrödinger operator.

February 13, 2026Open Access

Beyond First Order: Gauge Obstruction and Schrödinger Resolution in the Idele Class Spectral Framework

Puntos clave

The main aim is to demonstrate the limitations of the point spectrum in first-order perturbations and resolve it using the Schrödinger operator.
Constructed the Harmonic Equilibrium Operator and analyzed its gauge equivalence to the free Stone generator.
Examined self-adjointness through the Kato–Rellich theorem.
Investigated the properties and non-triviality of the modified Birman–Schwinger operator.
Formulated conjectures and a computational protocol for evaluating the operator.
Point spectrum is trivial under first-order perturbations, indicating limitations in the spectral identification hypothesis.
Established new Schrödinger operator showing unconditional self-adjointness and absence of gauge trivialization.
Demonstrated a non-trivially entire Fredholm determinant for the modified Birman–Schwinger operator.

Resumen

Title: Beyond First Order: Gauge Obstruction and Schrödinger Resolution in the Idele Class Spectral Framework Author: Frédéric David Blum (Independent Researcher, AI-Assisted Research Collaboration) Abstract We prove that the Harmonic Equilibrium Operator Hε=D+VεHε=D+Vε constructed on L2(CQ)L2(CQ) in the Harmonic Ontology program toward the Riemann Hypothesis is unitarily equivalent to the free Stone generator D=−i d/dtD=−id/dt via an explicit gauge transformation (Uvf)(t)=ei∫0tvf(t).(Uvf)(t)=ei∫0tvf(t). This trivializes the spectral data: Specpp(Hε)=∅Specpp(Hε)=∅, the Birman–Schwinger determinant is identically one, and the scattering phase shift is constant. Consequently, the Spectral Identification Hypothesis—that the point spectrum encodes zeta zero ordinates—is untenable for any first-order perturbation D+VD+V with V∈L∞∩L1V∈L∞∩L1. We resolve this obstruction by replacing HεHε with the Schrödinger Harmonic Operator Hε=D2+VεHε=D2+Vε. For this operator we prove: (i) Unconditional self-adjointness on Dom(D2)Dom(D2) via the Kato–Rellich theorem;(ii) Absence of gauge trivialization: no unitary multiplication operator conjugates HεHε to D2D2;(iii) The modified Birman–Schwinger operator is Hilbert–Schmidt and non-Volterra, yielding a non-trivially entire Fredholm determinant;(iv) The scattering phase shift δχ(k)δχ(k) depends non-trivially on kk. Via the Birman–Krein formula, the trace difference Trf(Hε,χ)−f(D2)Trf(Hε,χ)−f(D2) equals a phase-shift integral. Under a new Jost–Zeta Correspondence Conjecture, this reduces to the Weil explicit formula—providing a natural mechanism for the Harmonic Trace Identity. The Riemann Hypothesis is reformulated as the statement that Hε,χ0Hε,χ0 has no bound states—a non-binding condition for a one-dimensional Schrödinger operator, accessible via Bargmann bounds and Lieb–Thirring inequalities. We formulate precise conjectures, describe a three-level computational protocol (Birman–Schwinger determinant, Jost function via Numerov, modified HTI test), and prove that the full architectural framework of the Harmonic Ontology—local-global decomposition, multi-resolution detection, Connes bridge—transfers rigorously to the Schrödinger setting. MSC 2020: 11M26, 47A10, 47A40, 81U05, 46L87, 58B34 Keywords: Riemann Hypothesis, gauge equivalence, Schrödinger operators, Jost function, scattering phase shift, idele class group, Birman–Krein formula, Weil explicit formula, inverse scattering, spectral theory

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