SWYGERT AO LASER-167X: A Compact Hybrid Gravitational-Wave Detector Enabled by a Universal Geometric Efficiency Bound - The Swygert Theory of Everything AO


J. S. Swygert
Independent Researcher — Cumberland, Maryland USA

Email: tstoeao@gmail.com

ORCID: 0009-0006-6633-4929

DOI:

Abstract


Across physical systems, dissipation prevents perfect conversion of available energy into observable work. Here we show that this limitation follows a geometric constraint: the fraction of opportunity realized as value is bounded by the number of resonant modes required to sustain dynamic structure. Defining


V = E \, Y, \quad 0 < Y < 1



Y_{\max}(N) = \frac{1}{\pi N}



1. Universal Geometric Constraint

No dynamic physical system achieves perfect efficiency. Any bounded structure requires resonant modes to maintain form. Each mode incurs unavoidable boundary-phase mismatch loss proportional to , yielding dissipation


D \propto \pi N.



Y_{\max}(N) = \frac{1}{1+\pi N} \approx \frac{1}{\pi N} \quad (\pi N \gg 1).



\boxed{Y_{\max}(N) = \frac{1}{\pi N}}



Y_{\max} = 0.106.



Y_{\mathrm{eff}} = g_Q \, Y_{\max} \approx 1.6 \times 0.106 = 0.17 \text{–} 0.23.



2. Device Architecture: SWYGERT AO LASER-167X

A compact gravitational-wave detector is designed to exploit this geometric constraint.

Component

Function

Physical Basis

Piezo-acoustic core (LiNbO₃ / PZT)

Confinement of coupled modes

Mode locking sets band

Toroidal gravitational coupler

Converts metric strain to elastic deformation

Quadrupole stress:

Laser interferometer

Converts displacement to phase shift


High-Q TiO₂/Fe₂O₃ ceramics

Enhances recoverable opportunity

Observed

Laboratory footprint:


<0.02\,\text{m}^3 \quad (\text{desktop scale})



3. Sensitivity Model

Gravitational strain produces displacement:


h = \frac{\Delta x}{L_{\mathrm{eff}}}.



S_n = \frac{\hbar \omega_0}{\eta P Q}.



\eta = 0.8,\quad P = 100\,\text{mW},\quad Q = 10^4,\quad L_{\mathrm{eff}}=1\,\text{cm},



h_{\min} = \frac{\sqrt{S_n/(BW \cdot t)}}{L_{\mathrm{eff}}}

\approx 10^{-19}.



4. Mode-Coupling Signature

The detector response follows the sum of three coupled Lorentzians:


\chi(\omega) = \sum_{k=1}^{3}

\frac{A_k}{\omega_k^2 - \omega^2 + i \Gamma_k \omega}.



5. Experimental Roadmap

Stage

Goal

Metric

Timeline

α

Bench interferometer + PZT

resolution

2–4 weeks

β

3-mode locking in toroid

Confirm

6–10 weeks

γ

Thermal/noise isolation

SNR > 5

<3 months

δ

GW signal search

Injected → SNR ≥ 10

<6 months

Bill of Materials and simulations provided at Zenodo DOI above.


6. Falsifiability

The law fails if any dynamic system yields:


Y > \frac{1}{\pi N}



Y < 0.10 \quad (\text{below stable dynamic floor}).



Y = \frac{V}{E}

= \frac{\Delta\phi \, \lambda}{2\pi P_{\mathrm{laser}}}



7. Implications

• Establishes a universal geometric ceiling on dissipation
• Provides an experimental origin of irreversibility
• Bridges quantum, electromagnetic, and gravitational limits
• Enables first practical MHz–GHz gravitational-wave astronomy
• Scalable, low-cost detectors for relic universe signals


Acknowledgments
Gratitude to collaborators contributing metasurface data and validation support.


References
[1] J. S. Swygert, Metamaterials Efficiency Study, Zenodo DOI: 10.5281/zenodo.17498055 (2025).
[2] W. H. Zurek, Rev. Mod. Phys. 75, 715 (2003).
[3] J. D. Bekenstein, Phys. Rev. D 7, 2333 (1973).
[4] B. P. Abbott et al., Phys. Rev. D 111, 062003 (2025).
[5] M. Fox et al., Nat. Photonics 18, 456 (2024).
[6] A. Millis et al., npj Quantum Inf. 7, 79 (2021).
[7] J. D. Jackson, Classical Electrodynamics, Wiley (1999).



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