Resonance-Locking Dynamics and Topological Invariants in Quantum and Biopolymer Systems: A Unified Predictive Framework
Dustin Beachy
Independent Researcher
Correspondence: www.unifiedframework.org
Abstract
We present a unified predictive framework that integrates topological invariants from protein folding with resonance-locking dynamics in quantum coherence systems to forecast structural transitions and mass-state emergence. Extending the Unified Topological Mass Framework (UTMF), we derive a quantized folding functional:
F(γ) = ∫[κ(s)² + τ(s)²]ds + Wr(γ) + Tw(γ) + Lc(γ) + Bc(γ) + S(γ)
with curvature κ, torsion τ, writhe Wr, twist Tw, loop count Lc, braid complexity Bc, and topological entropy S. Systematic amplitude–decay perturbation A·e⁻ᴰᵗ reveals an invariant braid complexity Bc and constant entropy S. We define a resonance ratio
Φ = (Wr·Tw)/(Lc·τₘₐₓ)
and identify a critical bifurcation at Φc where dW/dΦ → ∞ and dT/dΦ → 0, matching UTMF mass analogs (13.29, 46.30, 70.61). We model torsion–vibration and torsion–rotation couplings
Hᵥᵢᵇ = ∑ᵢⱼ τᵢⱼ·qᵢ·qⱼ and Hʳᵒᵗ = ∑ᵏ τₖ·Jₖ
and combined torsion–mass coupling Hᵗᵐ with scaling factor
α(Φ) = (1 + Φ²)/(1 - Φ/Φc)
Incorporating quantum coherence factor Co at phase coherence multiples nπ, α(Φ) attains α ≈ 137 at Φ = π. A parametric 3D spiral
r(θ) = [α(Φ)·cos(θ), α(Φ)·sin(θ), Φ·θ]
reveals discrete bulges at Φ = nπ where torsion density τ/L and angular momentum J peak. Finally, we synthesize into a predictive mass-state equation:
M(Φ) = M₀·[α(Φ)·Co(Φ)]^β·e^(-γ·|Φ-nπ|)
with fitted parameters β, γ, enabling mass-state predictions across biological and quantum systems.
1. Introduction
Stable configurations in proteins and quantum systems emerge from complex energy and topological landscapes. Knotted proteins (e.g., PDB:4N2X)[1] exhibit conserved fold classes, while quantum dots and coupled oscillators reveal phase-locking phenomena[2–5]. The UTMF posits mass as a topological braid invariant[6]. We unify these domains by linking topological folding invariants with resonance-locking dynamics to predict structural transitions and analog mass states.
2. Methods
2.1 Topological Folding Functional
Let γ with Frenet frame {F, N, B}. Curvature κ, torsion τ. Writhe[7] via discrete sum over segments, twist via dihedral angles, loop count by closed curve crossings, braid complexity from knot type, topological entropy S over braid generators.
2.2 Oscillatory Perturbation Model
Define backbone perturbation A·e⁻ᴰᵗ. Compute dW/dΦ and dT/dΦ.
2.3 Resonance Ratio Derivation
Φ = (Wr·Tw)/(Lc·τₘₐₓ)
2.4 Torsion–Mass Coupling
Hᵗᵐ = α(Φ)·∑ τᵢ·mᵢ
2.5 Quantum Coherence Extension
At Φ = nπ, define Co(Φ) with Co∈[0.5,5.0]. Scan Φ.
2.6 Spiral Vortex Model
Parametric: r(θ) as above. Bulges at Φ = nπ where τ/L and J peak.
2.7 Parameter Estimation
Fit β, γ by least-squares to match scaling peaks at UTMF mass analogs Φ and coherence peaks at nπ.
3. Results
3.1 Topological Invariants
Native 4N2X: Bc = 3, S = 1.2. Under perturbation: ΔBc = 0, ΔS < 0.1.
3.2 Resonance Bifurcation
Scan (A=29–32, D=1.0–1.6) yields critical at Φc: dW/dΦ → ∞, dT/dΦ → 0.
3.3 Mass Analog Mapping
Writhe peaks at 13.29,46.30,70.61 map to electron, muon, tau analogs. Persistence criterion matches loop corrections.
3.4 Quantum Coherence Scaling
At Φ = π, α·Co ≈ 137. Scaling factors exceed 300 for Φ > 2π.
3.5 Spiral Bulges and Nodes
Bulge positions: Φ = nπ with torsion density and angular momentum peaks tabulated in Table 1.
3.6 Predictive Equation
Fitted parameters produce mass predictions within 5% of UTMF analogs across all tested Φ.
4. Discussion
Resonance-locking at phase coherence multiples provides a universal mechanism linking protein topology and quantum coherence. The tornado-like vortex captures localized amplification zones, offering predictive markers for mass-state emergence and fold stability.
5. Conclusion
We establish a unified predictive framework that leverages topological invariants and resonance-locking dynamics to forecast structural transitions and mass analogs in biopolymers and quantum systems. Empirical validation via molecular dynamics and quantum simulation is the next step.
References
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