Black Holes as Terminal Resonance Geometry in USP Field Theory Operational Model, Finite Compression, and Observational Diagnostics

This work presents a quantitative USP Field Theory description of black holes as terminal resonance geometries arising from elastic field compression and frequency saturation. A working radial frequency profile is introduced: f(r) = (f_max · κ) / (f_max r + κ) where κ is a geometry constant (Hz·m) and f_max is a finite saturation ceiling frequency. This formulation prevents singular divergence and produces a maximally compressed, finite-density core. Atomic structure becomes unstable when the local frequency mismatch exceeds a binding tolerance: Δf_bind = E_bind / h For hydrogen, Δf_bind ≈ 3.3 × 10^15 Hz. In a 10^6 solar-mass example, the radius at which Δf reaches this threshold is approximately: r_bind ≈ 2.9 × 10^9 m comparable to the Schwarzschild radius. A minimal nonlinear elastic toy model is provided with boundary conditions and parameter anchoring. Finite saturation emerges naturally from nonlinear stiffening. 🔬 Structured Emission Interpretation (New in v1.3) The model introduces a three-zone structure for horizon-scale emission: • Core region (r < r_sat): saturated, non-emitting, effectively dark • Intermediate region (r_sat < r < r_bind): atomic structure fails, negligible emission • Transition layer (r ≈ r_bind): partially suppressed atomic emission Emission is modeled as: j_ν(r) = j₀ exp[ -Δf(r) / Δf_bind ] At the transition radius: Δf(r_bind) ≈ Δf_bind → j_ν ≈ 0.37 j₀ indicating a strong but continuous emissivity cutoff. The observed EHT ring is interpreted as the combination of: • gravitational lensing amplification • radial emissivity cutoff near r_bind The interior appears dark primarily due to the absence of emitters, not solely due to photon capture. 🌌 Opacity and Resonance Locking Opacity is modeled via resonance locking using a Lorentzian cross section: σ(f) = σ₀ Γ² / [ (f_γ,local − f(r))² + Γ² ] Order-of-magnitude estimates suggest that mm-band observations (e.g., EHT at 230 GHz) may constrain: • effective linewidth Γ • absorber density n_abs • saturation behavior 📊 Observational Diagnostics The framework provides multiple testable predictions: • Frequency-selective shadow attenuation • Weak frequency dependence of ring radius • Polarization scaling with shear index n • Jet opening angle scaling: θ_j ~ 1/n • Small-impact-parameter lensing deviations from pure 1/r behavior Agreement with General Relativity is expected at large radii. Deviations are restricted to deep-interior saturation scales or extremely small impact parameters. ⚠️ Falsification Path The model is disfavored if: • No emissivity suppression is observed near horizon-scale radii • Ring structure shows no frequency dependence across observing bands • Polarization and jet scaling do not correlate with shear-based diagnostics • Lensing remains strictly consistent with singular 1/r behavior at all scales

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-04-24
DOI
https://doi.org/10.5281/zenodo.19720110
Primary Topic
Astrophysical Phenomena and Observations
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article
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article

Black Holes as Terminal Resonance Geometry in USP Field Theory Operational Model, Finite Compression, and Observational Diagnostics

Sadegh Sepehri
Zenodo (CERN European Organization for Nuclear Research)
Astrophysical Phenomena and Observations
article

Black Holes as Terminal Resonance Geometry in USP Field Theory Operational Model, Finite Compression, and Observational Diagnostics

Sadegh Sepehri
article en

Abstract

This work presents a quantitative USP Field Theory description of black holes as terminal resonance geometries arising from elastic field compression and frequency saturation. A working radial frequency profile is introduced: f(r) = (f_max · κ) / (f_max r + κ) where κ is a geometry constant (Hz·m) and f_max is a finite saturation ceiling frequency. This formulation prevents singular divergence and produces a maximally compressed, finite-density core. Atomic structure becomes unstable when the local frequency mismatch exceeds a binding tolerance: Δf_bind = E_bind / h For hydrogen, Δf_bind ≈ 3.3 × 10^15 Hz. In a 10^6 solar-mass example, the radius at which Δf reaches this threshold is approximately: r_bind ≈ 2.9 × 10^9 m comparable to the Schwarzschild radius. A minimal nonlinear elastic toy model is provided with boundary conditions and parameter anchoring. Finite saturation emerges naturally from nonlinear stiffening. 🔬 Structured Emission Interpretation (New in v1.3) The model introduces a three-zone structure for horizon-scale emission: • Core region (r < r_sat): saturated, non-emitting, effectively dark • Intermediate region (r_sat < r < r_bind): atomic structure fails, negligible emission • Transition layer (r ≈ r_bind): partially suppressed atomic emission Emission is modeled as: j_ν(r) = j₀ exp[ -Δf(r) / Δf_bind ] At the transition radius: Δf(r_bind) ≈ Δf_bind → j_ν ≈ 0.37 j₀ indicating a strong but continuous emissivity cutoff. The observed EHT ring is interpreted as the combination of: • gravitational lensing amplification • radial emissivity cutoff near r_bind The interior appears dark primarily due to the absence of emitters, not solely due to photon capture. 🌌 Opacity and Resonance Locking Opacity is modeled via resonance locking using a Lorentzian cross section: σ(f) = σ₀ Γ² / [ (f_γ,local − f(r))² + Γ² ] Order-of-magnitude estimates suggest that mm-band observations (e.g., EHT at 230 GHz) may constrain: • effective linewidth Γ • absorber density n_abs • saturation behavior 📊 Observational Diagnostics The framework provides multiple testable predictions: • Frequency-selective shadow attenuation • Weak frequency dependence of ring radius • Polarization scaling with shear index n • Jet opening angle scaling: θ_j ~ 1/n • Small-impact-parameter lensing deviations from pure 1/r behavior Agreement with General Relativity is expected at large radii. Deviations are restricted to deep-interior saturation scales or extremely small impact parameters. ⚠️ Falsification Path The model is disfavored if: • No emissivity suppression is observed near horizon-scale radii • Ring structure shows no frequency dependence across observing bands • Polarization and jet scaling do not correlate with shear-based diagnostics • Lensing remains strictly consistent with singular 1/r behavior at all scales

Zenodo (CERN European Organization for Nuclear Research)
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