R&D Report: 64P1S5G Resonator at 28 GHz — Simulation Shows 2.23×10¹²× Energy Density Amplification at Hologram Center
Official American Aires Inc. R&D Department computational report (2020). MEMS-based simulation of the 64P1S5G microprocessor — used in Lifetune Room and Lifetune Personal — interacting with 28 GHz 5G-band electromagnetic radiation. The simulation demonstrates coherent holographic field transformation.
Microprocessor Specifications
| Parameter | 64P1S5G Value |
|---|---|
| Product | Lifetune Room, Lifetune Personal (2020 model) |
| Radiation frequency modeled | 28 GHz (5G millimeter-wave band) |
| Fractalization axes | 64 |
| Levels of fractalization | 1 level + prototype |
| Number of ring resonators | 4,161 |
| Slit dimensions (width × depth) | 0.2 μm × 0.8 μm |
| Substrate | Type-n monocrystalline silicon, crystallographic plane 100 (Miller index) |
| Resonator dimensions | 19.6 mm × 19.6 mm × 0.5 mm |
| Gain coefficient (Kl) in slits | 2–8× (low density to high density zones) |
| Scientific consultants | Prof. A.V. Kopyltsov (LETI), Prof. A. Jukna (VGTU) |
Why a Custom Simulation Was Required
Standard electromagnetic simulation software (FDTD, FEM packages) treats resonator-EMF interaction using classical physics principles. The Aires resonator exhibits a class of behavior not modeled by these tools: counter-wave interaction on the resonator surface producing derivative resonances. Specifically:
- The primary slit topology generates a diffraction response (first-order field superposition)
- The superposition itself becomes a secondary diffraction grating, generating a second-order response
- This cascade continues to a fourth derivative, where the result is Fourier-like transformation of the incident wave
Custom MEMS-based software was developed for the C16S (2018) and extended for the 64P1S5G (2020) to model these multi-order derivative interactions. Calculations required 120 machine-hours of compute time per simulation run.
Mathematical Model: Field Gain in Slits
The simulation models two distinct wave propagation paths at each resonator slit:
- Path l1 (over the slit): l1 = b = 0.2 μm
- Path l2 (along the slit): l2 = b + 2×glu = 9b = 1.8 μm
Diffraction intensity at angle θ is modeled using the standard single-slit diffraction formula, with the total electric field vector decomposed as: E = E_reflected + E_diffracted.
The result is computed as a 4-dimensional matrix (3D spatial + time) of field strength E and intensity I values across the receiver space above the resonator surface.
Key Computational Results
The Singularity at the Center
The circuit’s counter-resonance geometry — paired radial axes arranged strictly along diameters — causes a unique phenomenon at the center point. Counter-flows of potential from opposite sides of the ring multiply rather than cancel. The result is a point of singularity: energy density is maximized, while electric field amplitude approaches zero. This is mathematically consistent with quantum singularity concepts and with formula (1) in the original report (the harmonic convergence principle). The potential at this focal point:
Conclusion
The simulation confirms that the 64P1S5G resonator does not merely scatter or reflect 28 GHz radiation. It transforms the incident radiation into a highly coherent, symmetric, self-affine superposition — a hologram — whose structure mirrors the fractal topology of the resonator itself. The annular slits act as waveguides; ring intersections phase-match counter-flows to generate a stationary standing wave. The cascade of derivative responses produces a system with characteristics far beyond what classical reflection or diffraction alone would predict.
This report, alongside the C16S/C28S/C32S reports (2018), provides the theoretical physics foundation for how Aires microprocessors interact with and transform electromagnetic radiation in the 2.4–28 GHz range.
Researchers: K. Korshunov, I. Soltovskaya, T. Shamko | Project manager: I. Serov | Year: 2020