Minimal 3-Stack Kernel

Si Substrate Photonic-Core vs Ti3SiC2 Enhanced Architecture

Si 14 Xe 54 S 16 Ti 22 Ag 47

Kernel Visualization

IN L0
IN L1
OUT+
OUT-
GND
Xe Gap

Photon Propagation Speed Comparison

Material
Speed
Delay Ratio
Si Substrate
150,000 m/s
1x (baseline)
Ti3SiC2
2 m/s
1x slower

Control Panel

Material Selection

Input Controls

Environment Parameters

Pressure (Xe Gap) 1.0 atm
O1 Bias 0.0 V

Real-time Metrics

D (Displacement)
0.00nm
OUT Current
0.00mA
Delay Time
0.00μs
Throughput
0.00MOps

README.md - Technical Analysis

Why Ti3SiC2 Beats Si for Photonic-Core Logic

Traditional silicon photonics relies on Si substrate 3s2 3p2 with integrated lasers for optical signal generation. While Si enables photon propagation at ~150,000 m/s through the crystalline lattice, this high velocity limits control over signal timing and increases crosstalk in dense 3D stacks.

Ti3SiC2 MAX Phase Advantages

  • Extreme Slow-Light Effect: Ti3SiC2 exhibits photon propagation at ~2 m/s due to its layered hexagonal structure and metallic A-layer. This 75,000x reduction vs Si enables programmable optical delays critical for neuromorphic computing and signal synchronization.
  • Metallic-Like Conductivity: Unlike insulating Si, Ti3SiC2 combines ceramic stiffness with metallic electron transport. The Ag core with +/- terminals benefits from low-resistance Ti traces (left/right) for efficient charge injection.
  • Thermal Tolerance: S (sulfur) capping above Ag prevents oxidation at 600°C+ operating temps. Xe gas gap provides tunable dielectric (pressure-sensitive) for capacitive isolation without thermal expansion mismatch.
  • Anisotropic Properties: The 3s2 3p2 = 2 lasers Si configuration forces isotropic emission. Ti3SiC2 confines photons along basal planes, reducing leakage and enabling deterministic 6-connection routing: IN L0, IN L1, OUT+, OUT-, GND, Xe gap.

Architecture: Minimal 3-Stack

Layer 1 (Bottom): Si Substrate or Ti3SiC2 base with dual laser injection (L0/L1). GND plane.
Layer 2 (Mid): Ag Core with +/- terminals. Ti traces left/right for signal routing.
Layer 3 (Top): S passivation above Ag. Xe gas gap above for pressure-tunable optical coupling.

The 10kHz clock synchronizes optical pulses. O1 bias modulates S-Ag Schottky barrier height. Pressure controls Xe density, tuning the gap capacitance and photon tunneling probability. The dramatic delay difference makes Ti3SiC2 ideal for temporal logic gates where propagation time is a computational variable, not a bug.