AutoSamplingTheory.TechnicalLemmas.Analysis.BoundedQuadraticCostIntegrability
3 named declarations scanned from AutoSamplingTheory/TechnicalLemmas/Analysis/BoundedQuadraticCostIntegrability.lean.
Declarations
theorem AutoSamplingTheory.TechnicalLemmas.Analysis.BoundedQuadraticCostIntegrability.norm_sub_lt_center_distance_add_two_radius Partial Not mapped
- Points lying in two radius-`r` balls have pairwise distance bounded by the center distance plus `2r`.
theorem norm_sub_lt_center_distance_add_two_radius
{x y a b : E} {r : ℝ}
(hx : x ∈ Metric.ball a r) (hy : y ∈ Metric.ball b r) :
‖x - y‖ < ‖a - b‖ + 2 * r := by
have hxa : dist x a < r := Metric.mem_ball.mp hx
have hyb : dist b y < r := by
have h := Metric.mem_ball.mp hy
simpa [dist_comm] using h
have hay : dist a y < dist a b + r :=
(dist_triangle a b y).trans_lt (add_lt_add_left hyb _)
have hxy : dist x y < r + (dist a b + r) :=
(dist_triangle x a y).trans_lt (add_lt_add hxa hay)
rw [dist_eq_norm, dist_eq_norm] at hxy
nlinarith
/-- A probability law concentrated on a bounded product rectangle has
integrable squared displacement. -/
AutoSamplingTheory/TechnicalLemmas/Analysis/BoundedQuadraticCostIntegrability.lean:33published source at ed709a7f320d
theorem AutoSamplingTheory.TechnicalLemmas.Analysis.BoundedQuadraticCostIntegrability.integrable_norm_sub_sq_of_prob_one_bounded_rectangle Partial Not mapped
- A probability law concentrated on a bounded product rectangle has integrable squared displacement.
theorem integrable_norm_sub_sq_of_prob_one_bounded_rectangle
(mu : ProbabilityMeasure (E × E))
{U V : Set E} {a b : E} {r : ℝ}
(hr : 0 < r)
(hUmeas : MeasurableSet U) (hVmeas : MeasurableSet V)
(hprob : mu (U ×ˢ V) = 1)
(hU : U ⊆ Metric.ball a r)
(hV : V ⊆ Metric.ball b r) :
Integrable (fun z : E × E => ‖z.1 - z.2‖ ^ 2)
(mu : Measure (E × E)) := by
have hsm : AEStronglyMeasurable
(fun z : E × E => ‖z.1 - z.2‖ ^ 2)
(mu : Measure (E × E)) := by
apply Measurable.aestronglyMeasurable
fun_prop
let M : ℝ := ‖a - b‖ + 2 * r
have hM : 0 ≤ M := by
dsimp [M]
positivity
apply Integrable.of_bound hsm (M ^ 2)
have hmem : ∀ᵐ z ∂(mu : Measure (E × E)), z ∈ U ×ˢ V :=
(mem_ae_iff_prob_eq_one (hUmeas.prod hVmeas)).2 hprob
filter_upwards [hmem] with z hz
have hlt : ‖z.1 - z.2‖ < M := by
dsimp [M]
exact norm_sub_lt_center_distance_add_two_radius (hU hz.1) (hV hz.2)
have hsq : ‖z.1 - z.2‖ ^ 2 ≤ M ^ 2 := by
rw [sq_le_sq]
simpa [abs_of_nonneg (norm_nonneg _), abs_of_nonneg hM] using le_of_lt hlt
simpa [Real.norm_eq_abs, abs_sq] using hsq
/-- If two probability laws on joint pairs are respectively concentrated on
bounded rectangles, then the cross squared displacement formed from the first
source coordinate and second target coordinate is integrable under their
product law. -/
AutoSamplingTheory/TechnicalLemmas/Analysis/BoundedQuadraticCostIntegrability.lean:50published source at ed709a7f320d
theorem AutoSamplingTheory.TechnicalLemmas.Analysis.BoundedQuadraticCostIntegrability.integrable_cross_norm_sub_sq_of_prob_one_bounded_rectangles Partial Not mapped
- If two probability laws on joint pairs are respectively concentrated on bounded rectangles, then the cross squared displacement formed from the first source coordinate and second target coordinate is integrable under their product law.
theorem integrable_cross_norm_sub_sq_of_prob_one_bounded_rectangles
(muA muB : ProbabilityMeasure (E × E))
{UA VA UB VB : Set E} {aA bA aB bB : E} {r : ℝ}
(hr : 0 < r)
(hUAmeas : MeasurableSet UA) (hVAmeas : MeasurableSet VA)
(hUBmeas : MeasurableSet UB) (hVBmeas : MeasurableSet VB)
(hprobA : muA (UA ×ˢ VA) = 1)
(hprobB : muB (UB ×ˢ VB) = 1)
(hUA : UA ⊆ Metric.ball aA r)
(_hVA : VA ⊆ Metric.ball bA r)
(_hUB : UB ⊆ Metric.ball aB r)
(hVB : VB ⊆ Metric.ball bB r) :
Integrable
(fun z : (E × E) × (E × E) => ‖z.1.1 - z.2.2‖ ^ 2)
((muA : Measure (E × E)).prod (muB : Measure (E × E))) := by
let muAB : ProbabilityMeasure ((E × E) × (E × E)) := muA.prod muB
have hprobAB : muAB ((UA ×ˢ VA) ×ˢ (UB ×ˢ VB)) = 1 := by
dsimp [muAB]
simp [hprobA, hprobB]
have hmem :
∀ᵐ z ∂(muAB : Measure ((E × E) × (E × E))),
z ∈ (UA ×ˢ VA) ×ˢ (UB ×ˢ VB) :=
(mem_ae_iff_prob_eq_one
((hUAmeas.prod hVAmeas).prod (hUBmeas.prod hVBmeas))).2 hprobAB
have hsm : AEStronglyMeasurable
(fun z : (E × E) × (E × E) => ‖z.1.1 - z.2.2‖ ^ 2)
(muAB : Measure ((E × E) × (E × E))) := by
apply Measurable.aestronglyMeasurable
fun_prop
let M : ℝ := ‖aA - bB‖ + 2 * r
have hM : 0 ≤ M := by
dsimp [M]
positivity
have hint : Integrable
(fun z : (E × E) × (E × E) => ‖z.1.1 - z.2.2‖ ^ 2)
(muAB : Measure ((E × E) × (E × E))) := by
apply Integrable.of_bound hsm (M ^ 2)
filter_upwards [hmem] with z hz
have hlt : ‖z.1.1 - z.2.2‖ < M := by
dsimp [M]
exact norm_sub_lt_center_distance_add_two_radius
(hUA hz.1.1) (hVB hz.2.2)
have hsq : ‖z.1.1 - z.2.2‖ ^ 2 ≤ M ^ 2 := by
rw [sq_le_sq]
-- Source excerpt truncated; follow the exact source link.
AutoSamplingTheory/TechnicalLemmas/Analysis/BoundedQuadraticCostIntegrability.lean:85published source at ed709a7f320d
Excerpt truncated; the exact source link is authoritative.
Complete Lean source
AutoSamplingTheory/TechnicalLemmas/Analysis/BoundedQuadraticCostIntegrability.lean — full module with imports and context
import Mathlib.MeasureTheory.Integral.IntegrableOn
import Mathlib.MeasureTheory.Measure.FiniteMeasureProd
import Mathlib.MeasureTheory.Measure.ProbabilityMeasure
import Mathlib.Tactic
/-!
# Quadratic-cost integrability from bounded rectangle support
The local Brenier perturbation uses probability-normalized finite measures that
are concentrated on bounded rectangles. This module turns that geometric
support information into the `Integrable` hypotheses consumed by the product-law
cost comparison.
No cyclic monotonicity, common-mass construction, or transport optimality is
used here.
-/
namespace AutoSamplingTheory
namespace TechnicalLemmas
namespace Analysis
namespace BoundedQuadraticCostIntegrability
open MeasureTheory Set
open scoped Topology
noncomputable section
variable {E : Type*} [NormedAddCommGroup E]
[MeasurableSpace E] [BorelSpace E] [SecondCountableTopology E]
/-- Points lying in two radius-`r` balls have pairwise distance bounded by the
center distance plus `2r`. -/
theorem norm_sub_lt_center_distance_add_two_radius
{x y a b : E} {r : ℝ}
(hx : x ∈ Metric.ball a r) (hy : y ∈ Metric.ball b r) :
‖x - y‖ < ‖a - b‖ + 2 * r := by
have hxa : dist x a < r := Metric.mem_ball.mp hx
have hyb : dist b y < r := by
have h := Metric.mem_ball.mp hy
simpa [dist_comm] using h
have hay : dist a y < dist a b + r :=
(dist_triangle a b y).trans_lt (add_lt_add_left hyb _)
have hxy : dist x y < r + (dist a b + r) :=
(dist_triangle x a y).trans_lt (add_lt_add hxa hay)
rw [dist_eq_norm, dist_eq_norm] at hxy
nlinarith
/-- A probability law concentrated on a bounded product rectangle has
integrable squared displacement. -/
theorem integrable_norm_sub_sq_of_prob_one_bounded_rectangle
(mu : ProbabilityMeasure (E × E))
{U V : Set E} {a b : E} {r : ℝ}
(hr : 0 < r)
(hUmeas : MeasurableSet U) (hVmeas : MeasurableSet V)
(hprob : mu (U ×ˢ V) = 1)
(hU : U ⊆ Metric.ball a r)
(hV : V ⊆ Metric.ball b r) :
Integrable (fun z : E × E => ‖z.1 - z.2‖ ^ 2)
(mu : Measure (E × E)) := by
have hsm : AEStronglyMeasurable
(fun z : E × E => ‖z.1 - z.2‖ ^ 2)
(mu : Measure (E × E)) := by
apply Measurable.aestronglyMeasurable
fun_prop
let M : ℝ := ‖a - b‖ + 2 * r
have hM : 0 ≤ M := by
dsimp [M]
positivity
apply Integrable.of_bound hsm (M ^ 2)
have hmem : ∀ᵐ z ∂(mu : Measure (E × E)), z ∈ U ×ˢ V :=
(mem_ae_iff_prob_eq_one (hUmeas.prod hVmeas)).2 hprob
filter_upwards [hmem] with z hz
have hlt : ‖z.1 - z.2‖ < M := by
dsimp [M]
exact norm_sub_lt_center_distance_add_two_radius (hU hz.1) (hV hz.2)
have hsq : ‖z.1 - z.2‖ ^ 2 ≤ M ^ 2 := by
rw [sq_le_sq]
simpa [abs_of_nonneg (norm_nonneg _), abs_of_nonneg hM] using le_of_lt hlt
simpa [Real.norm_eq_abs, abs_sq] using hsq
/-- If two probability laws on joint pairs are respectively concentrated on
bounded rectangles, then the cross squared displacement formed from the first
source coordinate and second target coordinate is integrable under their
product law. -/
theorem integrable_cross_norm_sub_sq_of_prob_one_bounded_rectangles
(muA muB : ProbabilityMeasure (E × E))
{UA VA UB VB : Set E} {aA bA aB bB : E} {r : ℝ}
(hr : 0 < r)
(hUAmeas : MeasurableSet UA) (hVAmeas : MeasurableSet VA)
(hUBmeas : MeasurableSet UB) (hVBmeas : MeasurableSet VB)
(hprobA : muA (UA ×ˢ VA) = 1)
(hprobB : muB (UB ×ˢ VB) = 1)
(hUA : UA ⊆ Metric.ball aA r)
(_hVA : VA ⊆ Metric.ball bA r)
(_hUB : UB ⊆ Metric.ball aB r)
(hVB : VB ⊆ Metric.ball bB r) :
Integrable
(fun z : (E × E) × (E × E) => ‖z.1.1 - z.2.2‖ ^ 2)
((muA : Measure (E × E)).prod (muB : Measure (E × E))) := by
let muAB : ProbabilityMeasure ((E × E) × (E × E)) := muA.prod muB
have hprobAB : muAB ((UA ×ˢ VA) ×ˢ (UB ×ˢ VB)) = 1 := by
dsimp [muAB]
simp [hprobA, hprobB]
have hmem :
∀ᵐ z ∂(muAB : Measure ((E × E) × (E × E))),
z ∈ (UA ×ˢ VA) ×ˢ (UB ×ˢ VB) :=
(mem_ae_iff_prob_eq_one
((hUAmeas.prod hVAmeas).prod (hUBmeas.prod hVBmeas))).2 hprobAB
have hsm : AEStronglyMeasurable
(fun z : (E × E) × (E × E) => ‖z.1.1 - z.2.2‖ ^ 2)
(muAB : Measure ((E × E) × (E × E))) := by
apply Measurable.aestronglyMeasurable
fun_prop
let M : ℝ := ‖aA - bB‖ + 2 * r
have hM : 0 ≤ M := by
dsimp [M]
positivity
have hint : Integrable
(fun z : (E × E) × (E × E) => ‖z.1.1 - z.2.2‖ ^ 2)
(muAB : Measure ((E × E) × (E × E))) := by
apply Integrable.of_bound hsm (M ^ 2)
filter_upwards [hmem] with z hz
have hlt : ‖z.1.1 - z.2.2‖ < M := by
dsimp [M]
exact norm_sub_lt_center_distance_add_two_radius
(hUA hz.1.1) (hVB hz.2.2)
have hsq : ‖z.1.1 - z.2.2‖ ^ 2 ≤ M ^ 2 := by
rw [sq_le_sq]
simpa [abs_of_nonneg (norm_nonneg _), abs_of_nonneg hM] using le_of_lt hlt
simpa [Real.norm_eq_abs, abs_sq] using hsq
simpa [muAB] using hint
end
end BoundedQuadraticCostIntegrability
end Analysis
end TechnicalLemmas
end AutoSamplingTheory