Encyclopedia Cosmology Cosmology Dark Energy Scale Affinity Derivation No Hidden Forces Canonical Kerne
ARTICLE 3 claims 3 theorems
Cosmology Dark Energy Scale Affinity Derivation No Hidden Forces Canonical Kerne
A single condition on how cosmic history is recorded forces the standard dark-energy equation of state, with no hidden forces required.
The canonical kernel
In physical cosmology, the equation of state of dark energy is the relation between its pressure and its energy density, usually written as a number w. The standard cosmological model, Lambda-CDM, takes w = -1 exactly, meaning dark energy behaves like a cosmological constant. A central question is whether any deeper principle forces that value, or whether it is simply a free parameter chosen to fit observations.
The Recognition Science framework addresses this question by starting from a discrete record of cosmic events, called the ledger, a bookkeeping device that assigns a value to each stage of cosmic expansion. The framework's library, a machine-checked collection of formal theorems, proves that if the ledger does not insert an extra preferred coordinate between the early universe and today, then the normalized fraction of the ledger's value must interpolate linearly between its endpoints. This condition, called no-hidden-scale-coordinate admissibility, forces the scale factor itself to be the ledger fraction.
From that single condition, the library derives the redshift history Z(z) = Z_today / (1 + z), where z is the cosmological redshift. The theorem named noHidden_forces_canonical_kernel then establishes the canonical equation of state: w(z) = -1 + δw0 / (1 + z), where δw0 is a constant deviation at the present day. This is the standard form used in phenomenological dark-energy models, and here it is not assumed but derived from the no-hidden-coordinate condition. The derivation is complete in the sense that the theorem is checked by the machine, with no unproved assumptions beyond the stated admissibility gate.
What the theorem does not do is explain why the no-hidden-coordinate condition itself must hold. That condition is stated as an admissibility gate, a premise of the derivation, not a consequence of a deeper principle. The framework's own documentation marks this as the remaining open problem: deriving the admissibility condition from the universal forcing layer. Nor does the theorem assert that the measured value of δw0 is zero; it only fixes the functional form of the deviation, leaving its magnitude to observation. The framework treats the comparison with measured values as an empirical check, not as part of the proof.
THEOREM noHidden_forces_canonical_kernel · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean
/-- The no-hidden-scale-coordinate condition forces the canonical equation of state. -/
theorem noHidden_forces_canonical_kernel (dw0 Zt : ℝ)
(H : NoHiddenScaleCoordinate) (z : ℝ)
(hZt : Zt ≠ 0) (hz : (1 : ℝ) + z ≠ 0) :
CosmicZHistory.bitKernel dw0 Zt
(CosmicZScaleLaw.ZfromScaleLaw Zt (noHidden_to_scaleAffine H)) z =
-1 + dw0 / (1 + z) :=
CosmicZScaleLaw.scaleAffine_forces_canonical_kernel
dw0 Zt (noHidden_to_scaleAffine H) z hZt hz
THEOREM noHidden_forces_identity · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean
/-- The no-hidden-scale-coordinate condition forces normalized Z-fraction to be the scale
factor itself. -/
theorem noHidden_forces_identity (H : NoHiddenScaleCoordinate) (a : ℝ) :
H.Zfrac a = a := by
exact CosmicZScaleLaw.scaleAffine_forces_identity (noHidden_to_scaleAffine H) a
THEOREM noHidden_forces_linearZ · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean
/-- The no-hidden-scale-coordinate condition forces the redshift history
`Z(z)=Z_today/(1+z)`. -/
theorem noHidden_forces_linearZ (Zt : ℝ) (H : NoHiddenScaleCoordinate) (z : ℝ) :
CosmicZScaleLaw.ZfromScaleLaw Zt (noHidden_to_scaleAffine H) z =
CosmicZHistory.linearZ Zt z :=
CosmicZScaleLaw.scaleAffine_forces_linearZ Zt (noHidden_to_scaleAffine H) z
What this page does not claim
The theorem does not derive the no-hidden-scale-coordinate condition from a deeper principle; it assumes that condition as an admissibility gate. The theorem does not fix the numerical value of the deviation δw0; it only fixes the functional form of the equation of state. The theorem does not prove that dark energy is a cosmological constant, since the deviation term is not forced to vanish.
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/Cosmology/DarkEnergyScaleAffinityDerivation.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:
- Can the no-hidden-scale-coordinate admissibility condition itself be derived from the universal forcing layer?
- What measured value of the dark-energy deviation δw0 does the framework predict, if any?
- How does the canonical equation of state compare with current observational constraints on w(z)?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM noHidden_forces_canonical_kernel · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean
/-- The no-hidden-scale-coordinate condition forces the canonical equation of state. -/ theorem noHidden_forces_canonical_kernel (dw0 Zt : ℝ) (H : NoHiddenScaleCoordinate) (z : ℝ) (hZt : Zt ≠ 0) (hz : (1 : ℝ) + z ≠ 0) : CosmicZHistory.bitKernel dw0 Zt (CosmicZScaleLaw.ZfromScaleLaw Zt (noHidden_to_scaleAffine H)) z = -1 + dw0 / (1 + z) := CosmicZScaleLaw.scaleAffine_forces_canonical_kernel dw0 Zt (noHidden_to_scaleAffine H) z hZt hzThe theorem named noHidden_forces_canonical_kernel then establishes the canonical equation of state: w(z) = -1 + δw0 / (1 + z), where δw0 is a constant deviation at the present day. noHidden_forces_canonical_kernel · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.leanTHEOREM noHidden_forces_identity · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean
/-- The no-hidden-scale-coordinate condition forces normalized Z-fraction to be the scale factor itself. -/ theorem noHidden_forces_identity (H : NoHiddenScaleCoordinate) (a : ℝ) : H.Zfrac a = a := by exact CosmicZScaleLaw.scaleAffine_forces_identity (noHidden_to_scaleAffine H) aThe framework's library, a machine-checked collection of formal theorems, proves that if the ledger does not insert an extra preferred coordinate between the early universe and today, then the normalized fraction of the ledger's value must interpolate linearly between its endpoints. noHidden_forces_identity · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.leanTHEOREM noHidden_forces_linearZ · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean
/-- The no-hidden-scale-coordinate condition forces the redshift history `Z(z)=Z_today/(1+z)`. -/ theorem noHidden_forces_linearZ (Zt : ℝ) (H : NoHiddenScaleCoordinate) (z : ℝ) : CosmicZScaleLaw.ZfromScaleLaw Zt (noHidden_to_scaleAffine H) z = CosmicZHistory.linearZ Zt z := CosmicZScaleLaw.scaleAffine_forces_linearZ Zt (noHidden_to_scaleAffine H) zFrom that single condition, the library derives the redshift history Z(z) = Z_today / (1 + z), where z is the cosmological redshift. noHidden_forces_linearZ · IndisputableMonolith/Cosmology/DarkEnergyScaleAffinityDerivation.lean