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High-sensitivity optical communication systems, quantum key distribution (QKD) receivers, light-detection, ranging (LiDAR) front-ends, and advanced astronomical instrumentation—including photon-counting optical arrays, adaptive optics wavefront sensors, high-time-resolution pulsar timing detectors, and fast optical transient follow-up receivers—rely on Avalanche Photodiodes (APDs) to achieve internal signal amplification via impact ionization. However, ultimate receiver sensitivity, signal-to-noise ratio (SNR), and timing jitter are fundamentally constrained by excess noise multiplication factors (), spatial dead-space effects, and high-field space-charge instability. In this work, we extend our first-principles inter-site fluctuation mechanics framework to the high-field impact ionization regime of APD multiplication regions. We formulate a stochastic master equation coupling primary carrier injection with non-local impact ionization rates, dead-space boundary conditions, and trap-assisted avalanche initiation. We derive the exact excess noise factor and its convolution with distributed inter-site generation-recombination noise, establishing how microscopic defect kinetics in the multiplication region generate excess noise spikes and micro-plasma instabilities. Finally, we outline a comprehensive MATLAB simulation architecture to validate multiplication noise spectra, excess noise scaling, and total noise equivalent power across varying operational gains and ionization ratios.
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James Glenn-Anderson (2026) studied this question.
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