OAI/NumberTheory/JointDickman/Probability/LowExclusiveKernel.lean
16 declarations, 0 contain sorry, 0 declared as axioms
The finite low-exclusive kernel
The common variable and the two exclusive variables have independent
finite masses. Cells are specified by an Option-valued map, allowing
discarded outputs. Restricting the second exclusive variable to low
has separate row and column estimates, proved from these actual masses.
- def
OAI.JointDickman.optionCellMassline 22 - theorem
OAI.JointDickman.optionCellMass_nonnegline 26 - theorem
OAI.JointDickman.optionCellMass_sum_leline 32 - def
OAI.JointDickman.lowExclusiveProbabilityline 42 - theorem
OAI.JointDickman.lowExclusiveProbability_nonnegline 45 - def
OAI.JointDickman.independentCellMarginalline 51 - def
OAI.JointDickman.lowExclusiveMassline 57Source documentation
The common mass is integrated after multiplying the two independent exclusive cell probabilities; only the second exclusive is restricted.
noncomputable def lowExclusiveMass (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (a b : A) : ℝ := … - theorem
OAI.JointDickman.lowExclusiveMass_nonnegline 63 - theorem
OAI.JointDickman.lowExclusiveMass_eq_tripleline 75Source documentation
This factorized definition is precisely the restricted independent triple law; it includes no assumption about its row or column behavior.
theorem lowExclusiveMass_eq_triple (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (a b : A) : lowExclusiveMass w v cell low a b = ∑ c, ∑ e₂, ∑ e₁, if low e₂ ∧ cell c e₁ = some a ∧ cell c e₂ = some b then w c * v e₁ * v e₂ else 0 := by …Mentions: OAI.JointDickman.lowExclusiveMass
- theorem
OAI.JointDickman.lowExclusiveMass_rowline 93Source documentation
The row estimate uses the fact that an exclusive output belongs to at most one retained cell.
theorem lowExclusiveMass_row (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (hw : ∀ c, 0 ≤ w c) (hv : ∀ e, 0 ≤ v e) (a : A) : (∑ b, lowExclusiveMass w v cell low a b) ≤ lowExclusiveProbability v low * independentCellMarginal w v cell a := by …Mentions: OAI.JointDickman.lowExclusiveMass, OAI.JointDickman.lowExclusiveProbability, OAI.JointDickman.independentCellMarginal
- theorem
OAI.JointDickman.lowExclusiveMass_integrate_commonline 117Source documentation
Integrating the common variable after conditioning on the restricted exclusive variable. This is the precise conditional mass used for columns.
theorem lowExclusiveMass_integrate_common (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (b : A) : (∑ c, w c * optionCellMass (fun e => if low e then v e else 0) (cell c) b) = ∑ e, if low e then v e * optionCellMass w (fun c => cell c e) b else 0 := by …Mentions: OAI.JointDickman.optionCellMass
- theorem
OAI.JointDickman.lowExclusiveMass_columnline 135Source documentation
The column estimate uses the normalized first exclusive law and a uniform conditional common-variable cell estimate at every low exclusive.
theorem lowExclusiveMass_column (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (hw : ∀ c, 0 ≤ w c) (hv : ∀ e, 0 ≤ v e) (hv1 : ∑ e, v e = 1) {H : ℝ} (hcommon : ∀ e, low e → ∀ b, optionCellMass w (fun c => cell c e) b ≤ H) (b : A) : (∑ a, lowExclusiveMass w v cell low a b) ≤ lowExclusiveProbability v low * H := by …Mentions: OAI.JointDickman.optionCellMass, OAI.JointDickman.lowExclusiveMass, OAI.JointDickman.lowExclusiveProbability
- def
OAI.JointDickman.lowExclusiveKernelline 172Source documentation
Equal cell atom weights give the manuscript's
m⁻²kernel.noncomputable def lowExclusiveKernel (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (m : ℝ) (a b : A) : ℝ := lowExclusiveMass w v cell low a b / (m * m)Mentions: OAI.JointDickman.lowExclusiveMass
- theorem
OAI.JointDickman.lowExclusiveKernel_weighted_rowline 176 - theorem
OAI.JointDickman.lowExclusiveKernel_weighted_columnline 191 - theorem
OAI.JointDickman.lowExclusiveKernel_square_boundline 209Source documentation
A finite Schur conclusion derived from the two distinct local-law estimates; neither a discarded-event operator bound nor a row bound is assumed.
theorem lowExclusiveKernel_square_bound (w : C → ℝ) (v : E → ℝ) (cell : C → E → Option A) (low : E → Prop) [DecidablePred low] (hw : ∀ c, 0 ≤ w c) (hv : ∀ e, 0 ≤ v e) (hv1 : ∑ e, v e = 1) {m H : ℝ} (hm : 0 < m) (hH : 0 ≤ H) (hmarginal : ∀ a, independentCellMarginal w v cell a ≤ H * m) (hcommon : ∀ e, low e → ∀ b, optionCellMass w (fun c => cell c e) b ≤ H * m) (f : A → ℝ) : (∑ a, m * finiteKernelAction (fun _ => m) (lowExclusiveKernel w v cell low m) f a ^ 2) ≤ (lowExclusiveProbability v low * H) ^ 2 * ∑ a, m * f a ^ 2 := by …Mentions: OAI.JointDickman.independentCellMarginal, OAI.JointDickman.optionCellMass, OAI.JointDickman.finiteKernelAction, OAI.JointDickman.lowExclusiveKernel, OAI.JointDickman.lowExclusiveProbability