SigmaLayer/ConstraintDynamics: deterministic, measure-preserving ontic dynamics #
Category: 7-SigmaLayer (the projective-sector layer (Paper C)).
ConstraintDynamics Sigma is the canonical SigmaLayer core (postulates P2, P3, P4): a finite Liouville
reference measure muL on the ontic state space, together with a deterministic real-parameter flow
that forms a one-parameter group and preserves muL. This is the group-law refinement of the existing
LF1.OnticSetup (single map, no group law) and LF4.KahlerOnticSetup (time flow, no group law); the
adapters into those live in SigmaLayer/IsolationPreparation.lean and SigmaLayer/ProjectiveSector.lean.
Anti-circularity #
ConstraintDynamics carries NO Born weight, NO frequency claim, NO Fubini-Study equality, NO unitary
projected dynamics, NO Schrödinger equation. It is deterministic dynamics and a reference measure only.
The projective sector pi is a separate structure (ProjectiveSector); all quantum content is a theorem
target or a named bridge assumption, never a field here.
Deterministic, measure-preserving ontic dynamics (postulates P2, P3, P4). A finite Liouville
reference measure muL, a deterministic flow forming a one-parameter group (flow_zero, flow_add),
each time-t map measurable and preserving muL. No quantum content.
- muL : MeasureTheory.FiniteMeasure Sigma
P2: the finite Liouville reference measure.
- flow : OnticTime → Sigma → Sigma
P3: the deterministic ontic flow.
- measurable_flow (t : OnticTime) : Measurable (self.flow t)
Each time-
tmap is measurable. The flow at time
0is the identity (one-parameter group identity).The flow composes additively in time (one-parameter group law).
- flow_preserves (t : OnticTime) : MeasureTheory.MeasurePreserving (self.flow t) ↑self.muL ↑self.muL
P4: each time-
tmap preserves the Liouville measure (Liouville's theorem).
Instances For
The trivial (identity-flow) dynamics with a given finite reference measure. The isolated
evolution is the identity; useful when the physical content of a model is a de-isolation interaction
(DeisolationModel) rather than a nontrivial isolated flow.
Equations
- CSD.SigmaLayer.trivialDynamics μ = { muL := μ, flow := fun (x : CSD.SigmaLayer.OnticTime) => id, measurable_flow := ⋯, flow_zero := ⋯, flow_add := ⋯, flow_preserves := ⋯ }
Instances For
Reversing the flow undoes it on the left: flow (-t) (flow t x) = x. Derived from the group law,
so reversibility is not a separate postulate.
Reversing the flow undoes it on the right: flow t (flow (-t) x) = x.
Each time-t flow map is a bijection, with inverse flow (-t) (derived from the real-flow group
laws, not postulated separately).