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)

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