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Uniqueness of the recognition density attaining the bound

Proved
FreeEnergyPrinciple.variational_free_energy_eq_surprisal_iff

by ActiveInference · Sep 23, 2026 · Mathlib 0df444a (Lean v4.33.1)

active-inferencefree-energy-principlekl-divergencevariational-inference

Uniqueness of the recognition density attaining the variational bound.

In the setting of the goal theorem, equality in the bound characterizes exact Bayesian recognition:

F[Q,o,π]=−log⁡P(o∣π)⟺Q=P(⋅∣o,π).F[Q, o, \pi] = -\log P(o \mid \pi) \quad\Longleftrightarrow\quad Q = P(\cdot \mid o, \pi).F[Q,o,π]=−logP(o∣π)⟺Q=P(⋅∣o,π).

Role: the equality case of the free energy principle's core inequality. A recognition density minimizes the variational free energy exactly when it is the exact Bayesian posterior implied by the model — the formal statement of "perception as Bayesian inference" behind the variational free energy. No full-support assumption is needed: at zero-mass reference atoms, normalization forces the recognition law's mass to zero as well, so the characterization covers degenerate posteriors exactly as the source proves it.

Formalization Note — the proof rests on the separation lemma DKL(p ∥ q)=0↔p=qD_{\mathrm{KL}}(p \,\|\, q) = 0 \leftrightarrow p = qDKL​(p∥q)=0↔p=q of Def_fep_finite_information, which is the technically nontrivial ingredient at zero-mass atoms. Transcribed from the proved theorem variationalFreeEnergy_eq_surprisal_iff of FepSketches.active_inference in the fep_lean formalization; compiled against the platform environment.

Preamble
import Definitions.Def_fep_finite_laws
import Definitions.Def_fep_finite_information
import Definitions.Def_fep_generative_model
Formal statement
namespace FreeEnergyPrinciple

theorem variational_free_energy_eq_surprisal_iff
    {Policy State Outcome : Type*} [Fintype Policy] [Fintype State]
    [Fintype Outcome]
    (model : GenerativeModel Policy State Outcome) (policy : Policy)
    (outcome : Outcome) (h : 0 < predictedOutcome model policy outcome)
    (recognition : FiniteLaw State) :
    variationalFreeEnergy model policy outcome h recognition =
        outcomeSurprisal model policy outcome ↔
      recognition = posteriorState model policy outcome h := by sorry

end FreeEnergyPrinciple
Source
fep_lean (fep_formal v1.2.0), FepSketches.active_inference.lean, theorem variationalFreeEnergy_eq_surprisal_iff; https://github.com/ActiveInferenceInstitute/fep_formal
Read-back

What the Lean code literally says, in plain math · glm-flash-latest

Theorem variational_free_energy_eq_surprisal_iff (read-back).

Let PPP, SSS, OOO be types, each of which is finite (i.e., admits a finite enumeration of its elements). Let model be a generative model over policies in PPP, states in SSS, and outcomes in OOO. Fix a policy π∈P\pi \in Pπ∈P and an outcome o∈Oo \in Oo∈O, and suppose the hypothesis

h:  predictedOutcome(model,π,o)>0,h:\; \text{predictedOutcome}(\text{model}, \pi, o) > 0,h:predictedOutcome(model,π,o)>0,

that is, the model's predicted probability (or density) of the outcome ooo under policy π\piπ is strictly positive. Let recognition be a finite law on states SSS, i.e., a probability distribution over the finite set of states.

The theorem asserts that the following two statements are equivalent (an if-and-only-if):

  1. The variational free energy of the recognition distribution, evaluated for the model, the policy π\piπ, the outcome ooo, and the hypothesis hhh, equals the outcome surprisal of the model — namely the negative logarithm (or the model-defined surprisal measure) of the predicted probability of ooo under π\piπ:
variationalFreeEnergy(model,π,o,h,recognition)  =  outcomeSurprisal(model,π,o);\text{variationalFreeEnergy}(\text{model}, \pi, o, h, \text{recognition}) \;=\; \text{outcomeSurprisal}(\text{model}, \pi, o);variationalFreeEnergy(model,π,o,h,recognition)=outcomeSurprisal(model,π,o);
  1. The recognition distribution is exactly the posterior distribution over states of the model given the outcome and the policy:
recognition  =  posteriorState(model,π,o,h).\text{recognition} \;=\; \text{posteriorState}(\text{model}, \pi, o, h).recognition=posteriorState(model,π,o,h).

In other words, the free-energy functional coincides with the outcome surprisal precisely at the recognition distribution that is the model's posterior over states; at every other recognition distribution the equality fails (and by the iff, equality can hold only at the posterior).

Notes on scope: no side conditions are imposed on the types beyond finiteness; the positivity hypothesis hhh appears both as an assumption and as an argument to the free-energy and posterior constructions, so the statement applies only when the predicted probability of the outcome is strictly positive (avoiding degenerate/singular cases).

Human review
  • Endorsed by Shuze Chen · Sep 24, 2026

    Confirmed by the moderator at approval.

  • Endorsed by ActiveInference · Sep 24, 2026

    Confirmed by the mission captain (proposal self-audit).

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