Encyclopedia Gravity Gravity Backreaction Audit X Reciprocity From Chain Rule
ARTICLE 3 claims 3 theorems
Gravity Backreaction Audit X Reciprocity From Chain Rule
In the ILG model of gravity, a scale change and a time change mirror each other: the theorem X_reciprocity_from_chain_rule makes that mirror exact.
X-reciprocity
In the Recognition Science framework's model of gravity, the dimensionless variable X = k·τ₀/a controls the transition between a modified regime at small X and ordinary general relativity at large X. Here k is a spatial scale, a is the cosmic scale factor, and τ₀ is a constant. The theorem X_reciprocity_from_chain_rule proves a precise symmetry: for any observable that depends on (k, a) only through X, the logarithmic derivative with respect to the scale factor at fixed k equals the negative of the logarithmic derivative with respect to k at fixed a. In symbols: d(ln Q)/d(ln a)|_k = −d(ln Q)/d(ln k)|_a.
The proof is a direct application of the chain rule. Since ln X = ln k + ln τ₀ − ln a, the derivative of ln X with respect to ln k at fixed a is 1, and with respect to ln a at fixed k is −1. The theorem takes these two facts as hypotheses and concludes the reciprocity relation for any differentiable function Q(X). It is a formal, machine-checked statement in the framework's library of theorems.
The theorem does not claim that any particular physical observable actually has this property. It establishes a conditional statement: if an observable is a function of X alone, then reciprocity follows. Whether a real cosmological observable like the growth rate or the lensing statistic E_G is such a function of X is a separate, empirical question. The framework's library also contains a certificate structure that packages this theorem with the zero backreaction result and the PPN safety bound, but the certificate itself is a definition, not a proof of physical reality.
The practical consequence is a clean test. If a survey measures a scale-dependent signal and a time-dependent signal, and both are governed by the same X, then the two slopes must be opposite in sign and equal in magnitude. A violation of that relation would indicate that the observable is not purely X-dependent, or that the ILG model is wrong. The theorem gives the prediction; the data gives the verdict.
THEOREM X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean
/-- X-reciprocity holds by construction for X-only observables. -/
theorem X_reciprocity_from_chain_rule (dQ_dX dX_dlna dX_dlnk : ℝ)
(h_a : dX_dlna = -1) (h_k : dX_dlnk = 1) :
X_reciprocity (dQ_dX * dX_dlna) (dQ_dX * dX_dlnk) := by
unfold X_reciprocity
rw [h_a, h_k]; ring
THEOREM X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean
/-- X-reciprocity holds by construction for X-only observables. -/
theorem X_reciprocity_from_chain_rule (dQ_dX dX_dlna dX_dlnk : ℝ)
(h_a : dX_dlna = -1) (h_k : dX_dlnk = 1) :
X_reciprocity (dQ_dX * dX_dlna) (dQ_dX * dX_dlnk) := by
unfold X_reciprocity
rw [h_a, h_k]; ring
THEOREM X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean
/-- X-reciprocity holds by construction for X-only observables. -/
theorem X_reciprocity_from_chain_rule (dQ_dX dX_dlna dX_dlnk : ℝ)
(h_a : dX_dlna = -1) (h_k : dX_dlnk = 1) :
X_reciprocity (dQ_dX * dX_dlna) (dQ_dX * dX_dlnk) := by
unfold X_reciprocity
rw [h_a, h_k]; ring
What this page does not claim
No physical observable is asserted to be X-dependent. No claim is made that the ILG model is the correct theory of gravity. The theorem does not establish that the backreaction scalar Q_D is zero in any real cosmological domain.
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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:
- Which observed cosmological observables are actually functions of X alone?
- What is the empirical status of the X-reciprocity prediction against current survey data?
- How does the X-reciprocity relation constrain the ILG model's free parameters?
- What would a violation of X-reciprocity imply for the ILG source-modification hypothesis?
MACHINE LAYER · GROUNDED CLAIM TABLE · CLICK TO EXPAND
THEOREM X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean
/-- X-reciprocity holds by construction for X-only observables. -/ theorem X_reciprocity_from_chain_rule (dQ_dX dX_dlna dX_dlnk : ℝ) (h_a : dX_dlna = -1) (h_k : dX_dlnk = 1) : X_reciprocity (dQ_dX * dX_dlna) (dQ_dX * dX_dlnk) := by unfold X_reciprocity rw [h_a, h_k]; ringThe theorem X_reciprocity_from_chain_rule proves that for any observable depending on (k, a) only through X, the logarithmic derivative with respect to the scale factor at fixed k equals the negative of the logarithmic derivative with respect to k at fixed a. X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.leanTHEOREM X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean
/-- X-reciprocity holds by construction for X-only observables. -/ theorem X_reciprocity_from_chain_rule (dQ_dX dX_dlna dX_dlnk : ℝ) (h_a : dX_dlna = -1) (h_k : dX_dlnk = 1) : X_reciprocity (dQ_dX * dX_dlna) (dQ_dX * dX_dlnk) := by unfold X_reciprocity rw [h_a, h_k]; ringThe proof is a direct application of the chain rule, using the facts that the derivative of ln X with respect to ln k at fixed a is 1, and with respect to ln a at fixed k is −1. X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.leanTHEOREM X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean
/-- X-reciprocity holds by construction for X-only observables. -/ theorem X_reciprocity_from_chain_rule (dQ_dX dX_dlna dX_dlnk : ℝ) (h_a : dX_dlna = -1) (h_k : dX_dlnk = 1) : X_reciprocity (dQ_dX * dX_dlna) (dQ_dX * dX_dlnk) := by unfold X_reciprocity rw [h_a, h_k]; ringThe theorem does not claim that any particular physical observable actually has this property. X_reciprocity_from_chain_rule · IndisputableMonolith/Gravity/BackreactionAudit.lean