Encyclopedia Foundation Foundation Pair Kernel Gap2a Landauer Calorimeter Door Residual Landauer Q Free
ARTICLE 3 claims 3 theorems
Foundation Pair Kernel Gap2a Landauer Calorimeter Door Residual Landauer Q Free
A machine-checked theorem shows a heat formula holds for any conversion quantum, but that freedom is exactly why it cannot pin down a specific physical scale.
The free heat quantum
Landauer's principle ties the heat released by erasing information to the number of bits erased: erase one bit, and at least a fixed minimum of heat must leave the system. In the Recognition Science framework, this relationship is expressed as recognition, a discrete record of events, posting a heat flux. The theorem landauer_q_free_sixChannel_inhabits_every_conversion_quantum states that for any real number q, there exists a heat carrier such that the posted heat equals q times the net erased bits. The proof is tautological: it constructs the heat carrier directly from the definition, so the statement holds without any assumption about what q should be.
The theorem is deliberately weak. Because it holds for every q, it does not select a preferred value. It is inhabited at q = 1 and at q = φ⁵, the framework's native action quantum, but it does not force either one. The declaration is a formal refutation of a stronger claim: that the Landauer heat-carrier premise alone could determine the remaining physical equality S = φ⁵. The theorem proves this is impossible, because the premise does not mention S at all. Pairing a free-q premise with an arbitrary source scale is vacuous, and the library explicitly proves that this pairing cannot force the target equality.
What the theorem does establish is a conditional path. If a future independent calorimeter (a missing piece marked OPEN) forces the selective quantum φ⁵, and if the priced carrier's source scale is identified with that quantum, then the remaining physical equality follows. That revival theorem is explicit about its hypotheses; it does not assume them as defaults. The free-q inhabitation is a necessary but far from sufficient step. It shows the heat side of the ledger is consistent, but it leaves the physical scale undetermined.
The practical consequence is a clean separation of concerns. The heat formula is settled; the scale is not. A reader should not mistake the theorem for a derivation of φ⁵ from thermodynamics. It is a proof of consistency, not a proof of uniqueness.
THEOREM landauer_q_free_sixChannel_inhabits_every_conversion_quantum · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
/-- Same inhabitation via the six-channel Clausius lift (aggregation, not
`rfl` with `stepHeatCell`). Still free in `q`; not an independent
external calorimeter. -/
theorem landauer_q_free_sixChannel_inhabits_every_conversion_quantum
(q : ℝ) :
HeatIsPostedRecordFlux q (sixChannelHeat q) :=
sixChannelHeat_is_posted_record_flux q
THEOREM landauer_q_free_inhabits_every_conversion_quantum · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
/-- The Landauer heat-carrier premise is inhabited at every conversion
quantum via the tautological posted-heat selector. -/
theorem landauer_q_free_inhabits_every_conversion_quantum (q : ℝ) :
HeatIsPostedRecordFlux q (tautologicalPostedHeat q) :=
tautological_heat_is_posted_record_flux q
THEOREM landauerDoor_does_not_force_remainingPhysicalEquality · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
/-- Explicit vacuous-pairing countermodel: the free-`q` heat-carrier premise
(existential, not mentioning `S`) is inhabited, yet candidate A rejects the
atom. Mirrors `no_route_within_banked_family`. -/
theorem landauerDoor_does_not_force_remainingPhysicalEquality :
¬ (∀ S : ℝ,
LandauerFreeConversionQuantumPremise S →
RemainingPhysicalEquality S) := by
intro hforce
exact remainingPhysicalEquality_rejects_candidateA
(hforce candidateA_sourceMagnitudeExpr.eval
(landauerFreeConversionQuantumPremise_holds _))
What this page does not claim
This theorem does not derive φ⁵ from thermodynamics. It does not claim the heat formula is physically meaningful without an independent calorimeter. It does not claim the missing independent calorimeter wall is discharged.
Verify this page
Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:
$ lake env lean IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
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 independent physical measurement could force the selective quantum φ⁵?
- How does the missing independent calorimeter wall relate to other OPEN residuals in the framework?
- What would a priced carrier with a source scale identified to φ⁵ look like physically?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM landauer_q_free_sixChannel_inhabits_every_conversion_quantum · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
/-- Same inhabitation via the six-channel Clausius lift (aggregation, not `rfl` with `stepHeatCell`). Still free in `q`; not an independent external calorimeter. -/ theorem landauer_q_free_sixChannel_inhabits_every_conversion_quantum (q : ℝ) : HeatIsPostedRecordFlux q (sixChannelHeat q) := sixChannelHeat_is_posted_record_flux qThe theorem states that for any real number q, there exists a heat carrier such that the posted heat equals q times the net erased bits. landauer_q_free_sixChannel_inhabits_every_conversion_quantum · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.leanTHEOREM landauer_q_free_inhabits_every_conversion_quantum · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
/-- The Landauer heat-carrier premise is inhabited at every conversion quantum via the tautological posted-heat selector. -/ theorem landauer_q_free_inhabits_every_conversion_quantum (q : ℝ) : HeatIsPostedRecordFlux q (tautologicalPostedHeat q) := tautological_heat_is_posted_record_flux qThe theorem does not select a preferred value for q. landauer_q_free_inhabits_every_conversion_quantum · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.leanTHEOREM landauerDoor_does_not_force_remainingPhysicalEquality · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean
/-- Explicit vacuous-pairing countermodel: the free-`q` heat-carrier premise (existential, not mentioning `S`) is inhabited, yet candidate A rejects the atom. Mirrors `no_route_within_banked_family`. -/ theorem landauerDoor_does_not_force_remainingPhysicalEquality : ¬ (∀ S : ℝ, LandauerFreeConversionQuantumPremise S → RemainingPhysicalEquality S) := by intro hforce exact remainingPhysicalEquality_rejects_candidateA (hforce candidateA_sourceMagnitudeExpr.eval (landauerFreeConversionQuantumPremise_holds _))The library explicitly proves that the free-q premise cannot force the target equality. landauerDoor_does_not_force_remainingPhysicalEquality · IndisputableMonolith/Foundation/PairKernelGap2aLandauerCalorimeterDoorResidual.lean