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Add lean source and binary files (part 85)
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import OAI.MathematicalPhysics.Boltzmann.Branching.AeKernelHistoryOrder
import Mathlib.Probability.Kernel.Composition.MeasureComp
namespace OAI
section
/-! # Finite sums commute with applying a kernel to a measure -/
noncomputable section
open MeasureTheory ProbabilityTheory
open scoped ProbabilityTheory
namespace BoltzmannNonuniqueness
variable {X Y : Type*} [MeasurableSpace X] [MeasurableSpace Y]
theorem kernel_finset_comp_measure {ι : Type*} (I : Finset ι) (K : ι → Kernel X Y)
(μ : Measure X) :
((∑ i ∈ I, K i) : Kernel X Y) ∘ₘ μ = ∑ i ∈ I, K i ∘ₘ μ := by
classical
induction I using Finset.induction_on with
| empty => simp
| @insert i I hi ih => simp only [Finset.sum_insert hi,Measure.add_comp,ih]
end BoltzmannNonuniqueness
end
end
section
/-! # Finite history comparison only needs kernel order on the reachable region -/
noncomputable section
open MeasureTheory ProbabilityTheory Set
open scoped ProbabilityTheory
namespace BoltzmannNonuniqueness
variable {X : Type*} [MeasurableSpace X]
theorem kernel_pow_le_on_invariant (K L : Kernel X X) (A : Set X)
(hinv : ∀ x ∈ A, ∀ᵐ y ∂K x, y ∈ A) (hle : ∀ x ∈ A, K x ≤ L x)
(n : ℕ) : ∀ x ∈ A, (K^n) x ≤ (L^n) x := by
induction n with
| zero => intro x hx; exact le_rfl
| succ n ih =>
intro x hx
rw [show K^(n+1) = (K^n) ∘ₖ K by simpa only [pow_one] using Kernel.pow_add K n 1,
show L^(n+1) = (L^n) ∘ₖ L by simpa only [pow_one] using Kernel.pow_add L n 1]
have h : ∀ᵐ y ∂K x, (K^n) y ≤ (L^n) y := by
filter_upwards [hinv x hx] with y hy
exact ih y hy
exact KernelHistoryOrder.measure_comp_mono_ae h (hle x hx)
end BoltzmannNonuniqueness
end
end
end OAI