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Tensions in Practice: A small observable state in tension with a sufficient predictive state

A deterministic cycle observed through three labels

The actual cycle repeats A, B, A, C. Start at a uniformly chosen position in that four-step cycle. Seeing A alone gives equal one-step chances of B and C. But A after B must be followed by C, while A after C must be followed by B. A three-label summary is enough for that restricted one-step marginal question; splitting A into its two phases retains the history needed for correct multi-step predictions.

Keep a compact one-step summary

Track only the three visible labels.

Predict valid sequences

Retain enough phase information to determine the next step.

Why these aims pull against each other

Merging the two A phases saves state but loses a predictive distinction. Recovering it requires a richer state and access to the phase, not merely labeling the coarse process memoryless.

Compare the arrangements

Keep the visible label

Use the stationary one-step frequencies for A, B and C under the uniform starting phase.

What it protects
Only the visible three-label state is needed for that limited conditional forecast.
What it costs
The summary cannot be iterated as a Markov transition model: it would allow B, A, B, which this cycle never produces.
When it fits
Fits one-step questions when only the current label is retained and the declared phase mixture applies.

Illustration note: This is a valid marginal summary, explicitly not a Markov representation of the full observed sequence.

Split the two A phases

Track A-after-C and A-after-B separately, alongside B and C.

What it protects
Every displayed transition reproduces the actual cycle, including multi-step paths.
What it costs
Four states and reliable phase tracking are required; seeing A in isolation does not identify its phase.
When it fits
Fits sequence prediction when the previous label or another phase signal is available.

Illustration note: The enriched process is deterministic and Markov. This does not make arbitrary systems observable or easy to predict.

What this illustration does—and does not—establish

The source supplies the structural tension; the invented example makes one relation inspectable. Costs and conditions are part of each arrangement, not exceptions to a universal recommendation.

  • The four-step cycle and uniform starting phase are invented and exact. They are not an estimated transition model.
  • The coarse arrows are one-step conditional frequencies; the fine arrows are deterministic state transitions. Their scopes are explicitly different.
  • No claim is made that adding any variable always restores the Markov property; this selected phase variable does so in this finite example.

Source entries

Markov Process

Prime · Source of the tension

The canonical tension motivates this comparison. The setting, finite values and arrangements are declared editorial illustrations, not measured findings.

Enriching the state to restore the Markov property trades memory for dimensionality

The practitioner must navigate between a state too thin to be Markov and a state so fat that the memorylessness buys no tractability.

Read the source section

The source operation

A Markov process embodies the *memorylessness* (Markov) property: the future evolution of a system is conditionally independent of its entire past history given its present state, an idea first made rigorous by Markov (1906) in his study of dependent sequences of random variables. The current state "screens off" the past, so that once you know where the system is now, knowing how it got there adds nothing to your prediction of where it goes next. The structural claim is sharp and almost paradoxically strong: a single, sufficiently-rich present state is a *complete summary* of all history relevant to the future, so prediction requires only the state now and a transition rule, not the trajectory that produced it.

Read the source section