Encyclopedia Holography Holography Record Monotonicity
ARTICLE 5 claims 5 theorems
Holography Record Monotonicity
In a discrete model of a holographic universe, the boundary record of a cell cannot shrink without a compensating heat debit, and this bookkeeping rule alone forces a weak form of complementarity.
Record monotonicity
Holography record monotonicity is a property of a discrete model of a holographic universe, one where a small three-dimensional cell carries a boundary record of six bits, one per face. The property says that the record's weight, the number of 1 bits, cannot decrease for free. In the model, a decrease in record weight is always exported as negative boundary heat, a debit, and a step with zero heat leaves the weight exactly unchanged. This is the no free erasure condition: posted information cannot be silently destroyed.
The model is built by the Recognition Science framework, which treats reality as a ledger, a discrete record of events. The framework's library, a machine-checked collection of formal theorems, proves the balance law: along any trajectory, the total heat equals the change in record weight. This is a theorem, not an assumption, for the posting rule that defines heat as the flux of record bits across the six faces. The theorem is called books_balance in the library.
The key structural result concerns gauge equivalence. Two configurations are gauge-related when they carry the same boundary record. The library proves that this relation is exactly the coset structure of a 16-element kernel: the only ways to change a configuration without changing its record are the 16 global parity moves. The theorem is gauge_iff_kernel. Also, no protocol built from record-compatible steps, steps that never create a boundary distinction without a posted source, can separate a gauge pair. The theorem gauge_never_separated shows this.
Quotienting the cell by gauge equivalence yields the central result: the record readout becomes an injection from physical states into the boundary record space. The theorem weak_complementarity proves this. There are 16 physical states, 16 posted records, and 4 posted bits against a 6-bit boundary capacity. This is weak complementarity: bulk physical states embed in the boundary record space. Operationally, if any physical distinguishing experiment factors through posting-compatible protocols, then record-equal states are physically indistinguishable. The theorem weak_complementarity_of_gsl states this conditional result.
The module replaces a monolithic complementarity premise with two weaker inputs: the posting rule already carried by the Clausius selector, and the no-free-record condition on dynamics. The erasure half of the generalized second law is discharged as a theorem; only the creation half remains a physical premise. The named falsifier for the remaining hypothesis is a physical process that separates two record-equal configurations with no posted source.
THEOREM stepHeatCell_eq_potential · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- One bulk step posts exactly the change of the record potential: `δQ = ΔΦ`. -/
theorem stepHeatCell_eq_potential (c c' : CellCfg) :
stepHeatCell c c' = cellPotential c' - cellPotential c :=
recordFlux_eq_weight_sub _ _ (by rw [faceRecord_length, faceRecord_length])
THEOREM gauge_iff_kernel · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **Gauge classes = kernel cosets.** Two configurations are gauge-related iff their
difference lies in the 16-element record kernel of `CellInjection`. The entire candidate
failure of complementarity is the coset structure of one named finite group. -/
theorem gauge_iff_kernel (c c' : CellCfg) :
gaugeRel c c' ↔ xorCfg c c' ∈ recordKernel := by
rw [mem_recordKernel_iff]
exact gauge_iff_kernel_record c c'
THEOREM gauge_never_separated · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **Gauge pairs are operationally inseparable** by posting-compatible protocols. -/
theorem gauge_never_separated (c c' : CellCfg) (h : gaugeRel c c') : ¬ Separated c c' := by
rintro ⟨Us, hUs, hne⟩
exact hne (no_protocol_separates Us hUs c c' h)
THEOREM weak_complementarity · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **WEAK COMPLEMENTARITY (quotient form, THEOREM).** The boundary record readout is
injective on physical states: distinct physical states of the bulk carry distinct
boundary records. This is the injection `bulk_phys(B) ↪ records(∂B)` the holography
manuscript assumes; here it is a theorem of the gauge quotient. -/
theorem weak_complementarity : Function.Injective physRecord := by
intro a b
refine Quotient.inductionOn₂ a b ?_
intro c c' h
exact Quotient.sound h
THEOREM weak_complementarity_of_gsl · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **WEAK COMPLEMENTARITY FROM THE GSL (the step-3 headline).** For any physical
distinguishability witnessed by posting-compatible protocols, record-equal bulk states
are physically indistinguishable: the manuscript's complementarity injection holds with
the monolithic premise replaced by the no-free-record discipline. -/
theorem weak_complementarity_of_gsl (dist : CellCfg → CellCfg → Prop)
(hG : KernelIsGauge dist) (c c' : CellCfg) (h : gaugeRel c c') : ¬ dist c c' :=
fun hd => gauge_never_separated c c' h (hG c c' hd)
What this page does not claim
No free erasure is proved only for the posting rule, not for all possible dynamics. The injection weak_complementarity is proved on the quotient, not for every individual configuration. The physical premise that every distinguishing experiment factors through posting-compatible protocols is a hypothesis, not a theorem.
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/Holography/RecordMonotonicity.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)
A page whose claims cannot be reproduced this way does not ship. In production, every anchor links to the exact declaration in the public source release, and this block carries the build receipt for the page itself.
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 process could falsify the hypothesis that every distinguishing experiment factors through posting-compatible protocols?
- How does the 4-bit posted capacity relate to the 6-bit boundary capacity in a larger holographic model?
- What does the creation half of the generalized second law require beyond the no-free-record condition?
- How does this module's weak complementarity compare to the strong complementarity assumed in the full holography manuscript?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM stepHeatCell_eq_potential · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- One bulk step posts exactly the change of the record potential: `δQ = ΔΦ`. -/ theorem stepHeatCell_eq_potential (c c' : CellCfg) : stepHeatCell c c' = cellPotential c' - cellPotential c := recordFlux_eq_weight_sub _ _ (by rw [faceRecord_length, faceRecord_length])The library proves the balance law: along any trajectory, the total heat equals the change in record weight. stepHeatCell_eq_potential · IndisputableMonolith/Holography/RecordMonotonicity.leanTHEOREM gauge_iff_kernel · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **Gauge classes = kernel cosets.** Two configurations are gauge-related iff their difference lies in the 16-element record kernel of `CellInjection`. The entire candidate failure of complementarity is the coset structure of one named finite group. -/ theorem gauge_iff_kernel (c c' : CellCfg) : gaugeRel c c' ↔ xorCfg c c' ∈ recordKernel := by rw [mem_recordKernel_iff] exact gauge_iff_kernel_record c c'The theorem gauge_iff_kernel shows that gauge equivalence is exactly the coset structure of a 16-element kernel. gauge_iff_kernel · IndisputableMonolith/Holography/RecordMonotonicity.leanTHEOREM gauge_never_separated · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **Gauge pairs are operationally inseparable** by posting-compatible protocols. -/ theorem gauge_never_separated (c c' : CellCfg) (h : gaugeRel c c') : ¬ Separated c c' := by rintro ⟨Us, hUs, hne⟩ exact hne (no_protocol_separates Us hUs c c' h)The theorem gauge_never_separated shows that no protocol built from record-compatible steps can separate a gauge pair. gauge_never_separated · IndisputableMonolith/Holography/RecordMonotonicity.leanTHEOREM weak_complementarity · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **WEAK COMPLEMENTARITY (quotient form, THEOREM).** The boundary record readout is injective on physical states: distinct physical states of the bulk carry distinct boundary records. This is the injection `bulk_phys(B) ↪ records(∂B)` the holography manuscript assumes; here it is a theorem of the gauge quotient. -/ theorem weak_complementarity : Function.Injective physRecord := by intro a b refine Quotient.inductionOn₂ a b ?_ intro c c' h exact Quotient.sound hThe theorem weak_complementarity proves that the record readout is an injection from physical states into the boundary record space. weak_complementarity · IndisputableMonolith/Holography/RecordMonotonicity.leanTHEOREM weak_complementarity_of_gsl · IndisputableMonolith/Holography/RecordMonotonicity.lean
/-- **WEAK COMPLEMENTARITY FROM THE GSL (the step-3 headline).** For any physical distinguishability witnessed by posting-compatible protocols, record-equal bulk states are physically indistinguishable: the manuscript's complementarity injection holds with the monolithic premise replaced by the no-free-record discipline. -/ theorem weak_complementarity_of_gsl (dist : CellCfg → CellCfg → Prop) (hG : KernelIsGauge dist) (c c' : CellCfg) (h : gaugeRel c c') : ¬ dist c c' := fun hd => gauge_never_separated c c' h (hG c c' hd)The theorem weak_complementarity_of_gsl states that if any physical distinguishing experiment factors through posting-compatible protocols, then record-equal states are physically indistinguishable. weak_complementarity_of_gsl · IndisputableMonolith/Holography/RecordMonotonicity.lean