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On the Tail Transition of First Arrival Position Channels: From Cauchy to Exponential Decay

Yen-Chi Lee

TL;DR

This work characterizes how the First Arrival Position FAP channel transitions from a heavy-tailed Cauchy noise model in zero drift to an exponential tail under nonzero drift. A universal critical length scale $n_c = \sigma^2/v$ demarcates diffusion-dominated and drift-dominated regions, yielding a Truncated Cauchy channel and finite moments beyond $n_c$. Capacity analyses reveal that Gaussian approximations misestimate performance at low drift, while the zero-drift Cauchy baseline provides a robust lower bound; as drift grows, the channel behavior shifts toward Gaussian with optimal inputs transitioning from heavy-tailed to discrete. These insights guide the design of dense Molecular MIMO systems by quantifying tail interference and informing input shaping under drift-diffusion dynamics.

Abstract

While the zero-drift First Arrival Position (FAP) channel is rigorously known to be Cauchy-distributed, practical molecular communication systems typically operate with non-zero drift. This letter characterizes the transition from heavy-tailed Cauchy behavior to light-tailed exponential decay. Through asymptotic analysis, we identify a critical spatial scale $n_c=σ^2/v$ separating diffusion- and drift-dominated regimes, revealing that the channel effectively behaves as a ``Truncated Cauchy'' model. Numerical results show that Gaussian approximations severely underestimate capacity at low drift, while the zero-drift case provides the appropriate performance lower bound for systems where drift assists particle transport.

On the Tail Transition of First Arrival Position Channels: From Cauchy to Exponential Decay

TL;DR

This work characterizes how the First Arrival Position FAP channel transitions from a heavy-tailed Cauchy noise model in zero drift to an exponential tail under nonzero drift. A universal critical length scale demarcates diffusion-dominated and drift-dominated regions, yielding a Truncated Cauchy channel and finite moments beyond . Capacity analyses reveal that Gaussian approximations misestimate performance at low drift, while the zero-drift Cauchy baseline provides a robust lower bound; as drift grows, the channel behavior shifts toward Gaussian with optimal inputs transitioning from heavy-tailed to discrete. These insights guide the design of dense Molecular MIMO systems by quantifying tail interference and informing input shaping under drift-diffusion dynamics.

Abstract

While the zero-drift First Arrival Position (FAP) channel is rigorously known to be Cauchy-distributed, practical molecular communication systems typically operate with non-zero drift. This letter characterizes the transition from heavy-tailed Cauchy behavior to light-tailed exponential decay. Through asymptotic analysis, we identify a critical spatial scale separating diffusion- and drift-dominated regimes, revealing that the channel effectively behaves as a ``Truncated Cauchy'' model. Numerical results show that Gaussian approximations severely underestimate capacity at low drift, while the zero-drift case provides the appropriate performance lower bound for systems where drift assists particle transport.

Paper Structure

This paper contains 17 sections, 10 equations, 3 figures.

Figures (3)

  • Figure 1: Abstract FAP channel model featuring hyperplane-shaped transmitters (Tx) and receivers (Rx). The particle undergoes Brownian motion with diffusion coefficient $D$ and drift velocity $\mathbf{v}$ over a transmission distance $\lambda$. The Rx registers the arrival point on the transverse plane.
  • Figure 2: Capacity transition of the FAP channel from the Cauchy regime to the Gaussian regime. The significant gap at low drift velocities highlights the failure of standard variance-based Gaussian approximations.
  • Figure 3: Spatial interference probability versus separation distance $r$. The zero-drift baseline is computed analytically via the Cauchy CDF, while non-zero drift curves are obtained by numerically integrating the exact Bessel-based PDF. For the high-drift case (blue dashed), the exponential truncation begins visibly after the critical scale $n_c \approx 40\,\mu\text{m}$.