R&D Computational Reports: Aires C16S, C28S, C32S Resonators at 2.4 GHz (Wi-Fi) — MEMS Simulation of Self-Affine Diffraction Grating Interaction (2018)

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R&D Computational Reports: Aires C16S, C28S, C32S Resonators at 2.4 GHz (Wi-Fi) — MEMS Simulation of Self-Affine Diffraction Grating Interaction (2018)

R&D Reports (2018): C16S, C28S & C32S Resonators at 2.4 GHz — MEMS Simulation of Wi-Fi Interaction via Custom Diffraction Model

Three companion computational reports characterizing the interaction of 2.4 GHz (Wi-Fi) electromagnetic radiation with the C16S (Aires Shield Pro), C28S (Aires Defender Pro), and C32S (Aires Guardian) microprocessors using a custom MEMS-based diffraction simulation that accounts for counter-wave interactions standard packages miss.

Computational physicsMEMS simulation2.4 GHz Wi-FiC16S / C28S / C32SSelf-affine diffractionAires Shield ProAires Defender ProAires Guardian2018

Three Microprocessors, One Architecture

The C16S, C28S, and C32S microprocessors all share the same fundamental self-affine circular diffraction grating architecture — a 4-level fractal structure etched onto a silicon wafer. The key difference is the number of fractalization axes, which determines the density of the ring resonator network and the complexity of the counter-resonance interactions.

C16S — Aires Shield Pro (2018)

• Fractalization axes: 16
• Fractal levels: 4
• Ring resonators: 83,521
• Slit dimensions: 0.4 μm × 0.8 μm
• Dimensions: 7.5mm × 7.5mm × 0.5mm
• Basic module D: 1.625 mm; Circuit D: 6.5 mm

C28S — Aires Defender Pro (2018)

• Fractalization axes: 28
• Fractal levels: 4
• Ring resonators: 707,281
• Slit dimensions: 0.4 μm × 0.8 μm
• Basic module D: 4.6 mm; Circuit D: 18.4 mm

C32S — Aires Guardian (2018)

• Fractalization axes: 32
• Fractal levels: 4
• Ring resonators: 1,185,921
• Slit dimensions: 0.4 μm × 0.8 μm
• Basic module D: 4.6 mm; Circuit D: 18.4 mm

Why Standard Simulation Packages Are Insufficient

Commercial electromagnetic simulation software (FDTD, FEM-based packages) models interaction in the context of classical physics — meaning they treat reflections and absorptions from flat/smooth surface features. The Aires resonator exhibits two phenomena these tools do not account for:

  1. Counter-wave interaction on the resonator surface: Because the fractalization axes are arranged in pairs strictly along ring diameters, counter-propagating surface waves interact at each diameter crossing. This is not a classical reflection scenario.
  2. Derivative resonances: The field superposition generated by the primary slit topology itself becomes a secondary diffraction grating, generating further superpositions in a cascade. This multi-order derivative response is physically distinct from single-pass diffraction.

Custom MEMS-based physical models, algorithms, and computer programs were developed to simulate these effects. Scientific consultants: Prof. Dr. A.V. Kopyltsov (Professor of Technical Sciences) and Prof. A. Jukna (Professor, Physics Department).

Physical Model

For all three processors, the simulation used an identical physical model:

  • Incident radiation: 2.4 GHz (Wi-Fi), field strength E₀ = 10 V/m, distance from source: 10 m
  • Slit behavior: slits absorb incident radiation; the smooth resonator surface reflects (angle of incidence = angle of reflection)
  • Receiver space: cubic matrix above the resonator, divided into cubic cells with increment h = 28 μm
  • Simulation duration: 1 second of electromagnetic interaction; computational time: 120 machine-hours per run

Mathematical Model: Slit Gain Factor

The key gain mechanism is the path-length difference between radiation traveling over vs. into a slit. For the C16S/C28S/C32S (slit width 0.4 μm, depth 0.8 μm):

l1 = b = 0.4 μm (over slit)   •   l2 = b + 2×glu = 5b = 2.0 μm (into slit)
Δl = l2 - l1 = 4b = 1.6 μm   →   Max field gain Kl = 4× in high-density zones

Field gain: Kl = 2× in low-density circuit regions, up to 4× in high-density zones. For comparison, the 64P1S5G (5G model, 0.2 μm slit width) achieves Kl up to 8× due to deeper slit-to-width ratio.

The diffraction contribution at angle θ is modeled via: E_total = E_reflected + E_diffracted, using the standard intensity formula I = I₀ × [sin(πb sinθ/λ) / (πb sinθ/λ)]².

Multi-Order Derivative Cascade

The simulation models four orders of field response:

  1. Derivative 1: Primary diffraction response of the C-series topology — computed as a symmetric cubic matrix, mirrored for symmetry
  2. Derivative 2: Derivative 1 matrix rotated 45° about X, Y, Z axes and summed — the superposition that begins acting as a secondary grating
  3. Derivative 3: Derivative 2 projected in 66 directions (67 total spheres summed) — producing deep interference including half-wave and quarter-wave resonant interconnections
  4. Derivative 4: Result of third-derivative interactions driving the incident wave flow toward harmonization with the structural eigenmodes — analogous to a direct and inverse Fourier transform
Core architectural principle: The self-affine topology of the C-series resonators transforms incident 2.4 GHz EMF not by blocking or absorbing it, but by initiating a cascade of derivative resonances that progressively harmonize the wave with the resonator’s fractal eigenmodes. The result is a coherent spatiotemporal superposition — a structured hologram — in the space above the resonator whose geometry mirrors the fractal structure of the circuit itself.

Annular Diffraction: From Ring to Fractal Hologram

A distinctive result from the basic ring analysis (C16S, shown in the report): the diffraction response of a single ring resonator at 2.4 GHz produces an annular spectrogram. Crucially, the ring’s curved surface focuses incident impulses toward its geometric center, where counter-propagating surface waves from opposite sides of the ring initiate counter-resonance. At gamma-radiation frequencies, this produces an internal fractal structure analogous to the pattern of a sunflower — a naturally self-similar biological structure. At 2.4 GHz Wi-Fi frequencies, the same topology produces a correspondingly scaled holographic response consistent with the fractal mathematical model.

Scaling: More Axes = More Coherent Response

Model Axes Rings Ring ratio vs. C16S
C16S (Aires Shield Pro) 16 83,521
C28S (Aires Defender Pro) 28 707,281 8.5×
C32S (Aires Guardian) 32 1,185,921 14.2×
64P1S5G (Lifetune Room/Personal) 64 4,161* *different geometry, 28 GHz optimized

*The 64P1S5G uses a different fractalization architecture (1 level + prototype) optimized for 28 GHz millimeter-wave interaction, rather than the 4-level 2.4 GHz architecture of the C-series.

Researchers: K. Korshunov, I. Soltovskaya, T. Shamko  |  Project manager: I. Serov  |  Scientific consultants: Prof. Kopyltsov, Prof. Jukna  |  Year: 2018

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