OAI/Probability/GammaPassage/BKBitLaw.lean
6 declarations, 0 contain sorry, 0 declared as axioms
- def
OAI.GammaFPP.gammaDyadicRankCellline 13 - lemma
OAI.GammaFPP.measurableSet_gammaDyadicRankCellline 17 - lemma
OAI.GammaFPP.gammaDyadicRankCell_disjointline 29 - lemma
OAI.GammaFPP.GammaEnvironment.gammaDyadicRankCell_realline 37 - theorem
OAI.GammaFPP.GammaEnvironment.gammaDyadicRankCells_realline 50Source documentation
Uniform bit-cube probabilities, obtained from the actual Gamma edge law through an exact disjoint partition into dyadic rank cells.
theorem GammaEnvironment.gammaDyadicRankCells_real (h : GammaEnvironment shape rate P τ) (hs : 0 < shape) (hr : 0 < rate) (S : Finset Edge) (t : ℕ) (A : Finset (Finset (Edge × Fin t))) (hA : A ⊆ (S ×ˢ Finset.univ).powerset) : P.real (⋃ x ∈ A, gammaDyadicRankCell shape rate τ S t x) = fairFamilyMass (S ×ˢ Finset.univ) A := by …Mentions: OAI.GammaFPP.GammaEnvironment, OAI.GammaFPP.gammaDyadicRankCell
- theorem
OAI.GammaFPP.GammaEnvironment.ae_gammaDyadicRankCellline 70Source documentation
Every original environment lies in one of the bit cells almost surely. Coverage follows from exact mass one, so no choice of a binary expansion on null endpoint configurations is needed.
theorem GammaEnvironment.ae_gammaDyadicRankCell (h : GammaEnvironment shape rate P τ) (hs : 0 < shape) (hr : 0 < rate) (S : Finset Edge) (t : ℕ) : ∀ᵐ ω ∂P, ∃ x ∈ (S ×ˢ (Finset.univ : Finset (Fin t))).powerset, ω ∈ gammaDyadicRankCell shape rate τ S t x := by …Mentions: OAI.GammaFPP.GammaEnvironment, OAI.GammaFPP.gammaDyadicRankCell