Encyclopedia Information Information Thermodynamics Ledger State
ARTICLE 4 claims 1 theorem 3 models
Information Thermodynamics Ledger State
A minimal mathematical structure for tracking the cost of information processing, with a proved lower bound on how much energy any such process must dissipate.
LedgerState and the cost of recognition
The LedgerState is a small data structure that represents a system's current information about its own parts. It consists of a finite set of active bonds, each with a positive real number called a bond multiplier. The multiplier measures how far that bond's current state is from perfect symmetry, where 1 would mean perfect balance. A bond with multiplier 2 is as imbalanced as a bond with multiplier 1/2, just in the opposite direction.
From this structure, the framework defines two quantities. The first is the recognition cost, which is the sum over all active bonds of the cost function J(x) = (x + 1/x)/2 - 1. This function is zero when x = 1 and grows as the bond moves away from balance. The second is the ledger entropy, defined as the sum of the absolute values of the natural logarithms of the bond multipliers. This measures the total amount of imbalance in the system, regardless of direction.
The central result is a proved theorem: the recognition cost of any state is at least half the sum of the squares of the logarithms of the bond multipliers. This gives a quadratic lower bound on the cost in terms of the entropy proxy. In plain terms, the more imbalanced a system's information is, the more it must cost to correct it. The theorem is proved in the machine-checked library of formal theorems, with no unproven assumptions beyond the standard logical axioms.
In Recognition Science, this structure models the Landauer limit, the principle that erasing one bit of information must dissipate at least kT ln 2 of energy. The framework's thermal cost function is exactly T times the natural logarithm of 2, matching the classical Landauer bound. The LedgerState provides the formal setting in which this bound becomes a theorem about recognition cost rather than a postulate about thermodynamics.
The framework also defines a recognition operator, which evolves a ledger state to a new state with no greater recognition cost. This is a formal model of dissipation: the operator can only decrease or preserve the cost, never increase it. The eight-tick dissipation limit theorem states that over one complete cycle, the cost after evolution is at most the cost before, which is simply a restatement of the operator's defining property.
What LedgerState does not claim is important. It does not claim that physical systems actually maintain such ledgers, nor that the recognition cost equals thermodynamic entropy in all cases. The entropy here is a proxy, a mathematical stand-in, not a proof of identity with physical entropy. The admissible predicate is defined as always true, meaning the framework does not yet restrict which states are physically possible. These are modeling choices, not empirical claims.
THEOREM total_dissipation_bound · IndisputableMonolith/Information/Thermodynamics.lean
/-- **Entropy Dissipation Theorem**
The total recognition cost of a state is bounded below by the quadratic
sum of the information mismatches. -/
theorem total_dissipation_bound (s : LedgerState) :
RecognitionCost s ≥ (1/2 : ℝ) * (s.active_bonds.sum (fun b => (Real.log (s.bond_multipliers b))^2)) := by
unfold RecognitionCost
rw [Finset.mul_sum]
apply Finset.sum_le_sum
intro b hb
have h := landauer_bound_holds s b hb
dsimp at h
linarith
MODEL thermal_cost · IndisputableMonolith/Information/Thermodynamics.lean
/-- **DEFINITION: Thermal Energy Scale**
The base thermal cost per tick. -/
noncomputable def thermal_cost (T : ℝ) : ℝ :=
T * Real.log 2
MODEL RecognitionOperator · IndisputableMonolith/Information/Thermodynamics.lean
/-- A local dissipative recognition operator for information thermodynamics. -/
structure RecognitionOperator where
evolve : LedgerState → LedgerState
minimizes_J : ∀ s, admissible s → RecognitionCost (evolve s) ≤ RecognitionCost s
MODEL admissible · IndisputableMonolith/Information/Thermodynamics.lean
/-- Admissibility predicate for the local information ledger. -/
def admissible (_s : LedgerState) : Prop := True
What this page does not claim
LedgerState does not claim that physical systems actually maintain such ledgers. The recognition cost is not claimed to equal thermodynamic entropy in all cases. The admissible predicate being always true means no physical restrictions are yet imposed.
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expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
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Derived articles
This page is generated by a question-recursion engine: the questions its answers raise become the next pages. The current agenda, with open targets marked red:
- What physical system, if any, maintains a ledger state that matches this mathematical structure?
- How does the recognition cost relate to thermodynamic entropy beyond the formal proxy used here?
- What restrictions on admissible states would make the framework physically meaningful?
- Can the quadratic lower bound be improved to a tighter inequality for specific bond distributions?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM total_dissipation_bound · IndisputableMonolith/Information/Thermodynamics.lean
/-- **Entropy Dissipation Theorem** The total recognition cost of a state is bounded below by the quadratic sum of the information mismatches. -/ theorem total_dissipation_bound (s : LedgerState) : RecognitionCost s ≥ (1/2 : ℝ) * (s.active_bonds.sum (fun b => (Real.log (s.bond_multipliers b))^2)) := by unfold RecognitionCost rw [Finset.mul_sum] apply Finset.sum_le_sum intro b hb have h := landauer_bound_holds s b hb dsimp at h linarithThe recognition cost of any state is at least half the sum of the squares of the logarithms of the bond multipliers. total_dissipation_bound · IndisputableMonolith/Information/Thermodynamics.leanMODEL thermal_cost · IndisputableMonolith/Information/Thermodynamics.lean
/-- **DEFINITION: Thermal Energy Scale** The base thermal cost per tick. -/ noncomputable def thermal_cost (T : ℝ) : ℝ := T * Real.log 2The framework's thermal cost function is exactly T times the natural logarithm of 2. thermal_cost · IndisputableMonolith/Information/Thermodynamics.leanMODEL RecognitionOperator · IndisputableMonolith/Information/Thermodynamics.lean
/-- A local dissipative recognition operator for information thermodynamics. -/ structure RecognitionOperator where evolve : LedgerState → LedgerState minimizes_J : ∀ s, admissible s → RecognitionCost (evolve s) ≤ RecognitionCost sA recognition operator evolves a ledger state to a new state with no greater recognition cost. RecognitionOperator · IndisputableMonolith/Information/Thermodynamics.leanMODEL admissible · IndisputableMonolith/Information/Thermodynamics.lean
/-- Admissibility predicate for the local information ledger. -/ def admissible (_s : LedgerState) : Prop := TrueThe admissible predicate is defined as always true. admissible · IndisputableMonolith/Information/Thermodynamics.lean