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Research PaperResearchia:202604.06032

From Gaussian Fading to Gilbert-Elliott: Bridging Physical and Link-Layer Channel Models in Closed Form

Bhaskar Krishnamachari

Abstract

Dynamic fading channels are modeled at two fundamentally different levels of abstraction. At the physical layer, the standard representation is a correlated Gaussian process, such as the dB-domain signal power in log-normal shadow fading. At the link layer, the dominant abstraction is the Gilbert-Elliott (GE) two-state Markov chain, which compresses the channel into a binary decodable or not'' sequence with temporal memory. Both models are ubiquitous, yet practitioners who need GE parameters fro...

Submitted: April 6, 2026Subjects: Engineering; Chemical Engineering

Description / Details

Dynamic fading channels are modeled at two fundamentally different levels of abstraction. At the physical layer, the standard representation is a correlated Gaussian process, such as the dB-domain signal power in log-normal shadow fading. At the link layer, the dominant abstraction is the Gilbert-Elliott (GE) two-state Markov chain, which compresses the channel into a binary ``decodable or not'' sequence with temporal memory. Both models are ubiquitous, yet practitioners who need GE parameters from an underlying Gaussian fading model must typically simulate the mapping or invoke continuous-time level-crossing approximations that do not yield discrete-slot transition probabilities in closed form. This paper provides an exact, closed-form bridge. By thresholding the Gaussian process at discrete slot boundaries, we derive the GE transition probabilities via Owen's TT-function for any threshold, reducing to an elementary arcsine identity when the threshold equals the mean. The formulas depend on the covariance kernel only through the one-step correlation coefficient ρ=K(D)/K(0)ρ= K(D)/K(0), making them applicable to any stationary Gaussian fading model. The bridge reveals how kernel smoothness governs the resulting link-layer dynamics: the GE persistence time grows linearly in the correlation length TcT_c for a smooth (squared-exponential) kernel but only as Tc\sqrt{T_c} for a rough (exponential/Ornstein--Uhlenbeck) kernel. We further quantify when the first-order GE chain is a faithful approximation of the full binary process and when it is not, reconciling two diagnostics, the one-step Markov gap and the run-length total-variation distance, that can trend in opposite directions. Monte Carlo simulations validate all theoretical predictions.


Source: arXiv:2604.03160v1 - http://arxiv.org/abs/2604.03160v1 PDF: https://arxiv.org/pdf/2604.03160v1 Original Link: http://arxiv.org/abs/2604.03160v1

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Date:
Apr 6, 2026
Topic:
Chemical Engineering
Area:
Engineering
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