MRH: Markov Relevancy Horizon

Theoretical Framework

The Markov Relevancy Horizon (MRH) is a term proposed by Dennis Palatov, inspired by Markov blankets — a concept from probabilistic graphical models where a node's Markov blanket is the minimal set of other nodes that makes it conditionally independent of everything else. The blanket is the boundary: everything inside it is relevant to the node, everything outside is statistically screened off.

MRH extends this idea from a static graph property to a dynamical, scale-dependent boundary. Where a Markov blanket asks “what nodes shield this node?”, the MRH asks “at what horizon do correlations between systems decay below the noise floor?” — making the boundary itself a function of scale, density, and context.

The minimal set of interacting degrees of freedom whose state transitions materially influence the coherence evolution of a defined system.

Operational Criteria

An MRH is not just a vague boundary — it must satisfy two testable conditions:

Predictive Sufficiency

Removing any element inside the MRH degrades coherence prediction. Everything inside is load-bearing.

Predictive Closure

Adding elements outside the MRH does not materially improve prediction. Everything outside is irrelevant. If it does improve prediction, the MRH was incorrectly specified.

MRH and Presence

Presence (ρ) — the compatible structural elements that drive coherence — is defined relative to an MRH. Change the MRH boundary, and presence changes. This means coherence is always context-dependent: what counts as “present” depends on which system you're examining and at what scale.

See: Coherence Function for how presence feeds into C(ρ).

How It Works

Every system maintains correlations with nearby systems. As distance (spatial or temporal) increases, these correlations weaken. The MRH is where they become negligible.

MRH and Quantum Measurement

This is Synchronism's most provocative claim about quantum mechanics:

Wave function “collapse” = crossing the MRH.

When a quantum system interacts with a macroscopic apparatus, the correlations between the system and its environment rapidly exceed the MRH. What we call “measurement” is this boundary crossing. No observer needed. No consciousness required. Just decoherence at the relevancy horizon.

6 Testable Protocols

Full treatment: Measurement Without Observers →

MRH at Cosmic Scales

The same concept applies to cosmology. Cosmic horizons (particle horizon, event horizon) can be reinterpreted as MRH boundaries at cosmological scales. Beyond the MRH, correlations from the early universe have decayed. What we call the “observable universe” is the region within our MRH.

Cosmic Horizons as MRH Phenomena →

MRH in Statistical Mechanics

In statistical mechanics, the correlation length ξ measures how far correlations extend. At a phase transition, ξ diverges. The MRH is the dynamical version of this: where correlations become irrelevant not just in space but in the full phase space of the system.

What's Untested

The MRH as a replacement for “wave function collapse” is the central untested prediction. Six experimental protocols have been designed (Sessions #368-370) but none have been run. The theory predicts specific decoherence patterns at the MRH boundary that should be measurable.

Next: Measurement Without Observers →See the 6 Protocols

Prerequisites

Understanding these concepts first will help:

The Coherence FunctionC(ρ) = tanh(γ log(ρ/ρ_crit + 1))

Related Concepts

Measurement Without ObserversMRH crossing replaces wave function collapseCosmic HorizonsInflation, dark energy as MRH phenomenaDecoherence at the MRHWhy classical emerges from quantum