OAI/Geometry/PinnedDistances/MinPotentials.lean
44 declarations, 0 contain sorry, 0 declared as axioms
- lemma
OAI.WeakPinned.Variance.cell_second_momentline 38Source documentation
The giant-complement second moment estimate needed to compare W and W₂. The linear error, unlike an absolute singleton error, can be integrated.
lemma cell_second_moment (w : I → ℝ) (B : I → Finset P) (T M κ : ℝ) (hw : ∀ i, 0≤w i) (hW : (∑ i, w i)≤1) (hT : 1≤T) (hκ : 0≤κ) (hk : ∀ i, 2/((B i).card:ℝ)≤κ) (hdom : ∀ x, (∑ i, w i*prob (B i) x)≤M*prob Finset.univ x) (C : Finset P) : (∑ i, w i*(cellProb (B i) C)^2) ≤ 2*varianceCell w B T C + 4*pairCell Finset.univ C + κ*M*cellProb Finset.univ C := by …Mentions: OAI.WeakPinned.B, OAI.WeakPinned.Variance.prob, OAI.WeakPinned.Variance.cellProb, OAI.WeakPinned.Variance.varianceCell, OAI.WeakPinned.Variance.pairCell
- lemma
OAI.WeakPinned.Variance.small_mass_qCellline 79Source documentation
Small positive-mass cut contributions are slice contributions or variance.
lemma small_mass_qCell {w : I → ℝ} {B : I → Finset P} (src : I → P) (T δ : ℝ) (hw : ∀ i, 0≤w i) (hδ : 0<δ) (hk : ∀ i, 2/((B i).card:ℝ)≤2*δ) (C : Finset P) (hC : cellProb Finset.univ C≤δ) : (∑ i, w i*(if src i ∈ C then cellProb (B i) C else 0)) ≤ (∑ i, w i*(if src i ∈ C ∧ cellProb (B i) C<2*δ then cellProb (B i) C else 0)) + (2/δ)*varianceCell w B T C := by …Mentions: OAI.WeakPinned.B, OAI.WeakPinned.Variance.cellProb, OAI.WeakPinned.Variance.varianceCell
- lemma
OAI.WeakPinned.Hierarchy.Depth.mem_giant_iff_cellline 129 - lemma
OAI.WeakPinned.Hierarchy.Depth.mem_giant_existsline 141 - lemma
OAI.WeakPinned.Hierarchy.Depth.mem_giant_monoline 152 - lemma
OAI.WeakPinned.Hierarchy.Depth.isClosed_mem_giantline 157 - lemma
OAI.WeakPinned.Hierarchy.Depth.mem_giant_lowline 174 - lemma
OAI.WeakPinned.Hierarchy.Depth.mem_giant_le_Mline 178 - def
OAI.WeakPinned.Hierarchy.Depth.departureline 183Source documentation
The last level at which the vertex belongs to the nested giant.
def departure (x : P) : ℝ := sSup {r : ℝ | x ∈ d.giant r} - lemma
OAI.WeakPinned.Hierarchy.Depth.departure_cutoffline 185 - lemma
OAI.WeakPinned.Hierarchy.Depth.departure_le_Mline 191 - lemma
OAI.WeakPinned.Hierarchy.Depth.outside_departureline 194 - lemma
OAI.WeakPinned.Hierarchy.Depth.integral_one_Iocline 201 - lemma
OAI.WeakPinned.Hierarchy.Depth.potential_departureline 206 - lemma
OAI.WeakPinned.Hierarchy.Depth.outside_productline 210 - lemma
OAI.WeakPinned.Hierarchy.Depth.min_potentialline 219Source documentation
Exact layer-cake identity, including the finite set of threshold ties.
lemma min_potential (hn : 2 ≤ Fintype.card P) (x y : P) : min (d.potential x) (d.potential y) = ∫ r, d.outsideIndicator r x*d.outsideIndicator r y := by … - def
OAI.WeakPinned.MinKernel.stepline 233 - lemma
OAI.WeakPinned.MinKernel.integrable_stepline 235 - lemma
OAI.WeakPinned.MinKernel.step_mulline 239 - lemma
OAI.WeakPinned.MinKernel.integral_stepline 244 - def
OAI.WeakPinned.MinKernel.tailline 248 - def
OAI.WeakPinned.MinKernel.energyline 250 - lemma
OAI.WeakPinned.MinKernel.tail_productline 252 - lemma
OAI.WeakPinned.MinKernel.integrable_tail_productline 265 - lemma
OAI.WeakPinned.MinKernel.energy_integralline 270 - lemma
OAI.WeakPinned.MinKernel.energy_crossline 276 - lemma
OAI.WeakPinned.MinKernel.min_add_fourline 286 - lemma
OAI.WeakPinned.MinKernel.energy_sumline 291 - def
OAI.WeakPinned.Hierarchy.Depth.outsideMassline 312 - lemma
OAI.WeakPinned.Hierarchy.Depth.integrable_outside_productline 314 - lemma
OAI.WeakPinned.Hierarchy.Depth.outsideMass_squareline 319 - lemma
OAI.WeakPinned.Hierarchy.Depth.iid_min_potentialline 330 - theorem
OAI.WeakPinned.Hierarchy.Depth.iid_min_two_potentialsline 339Source documentation
The source min-potential upper bound before averaging places and grids.
theorem iid_min_two_potentials (d' : Depth P) (hn : 2 ≤ Fintype.card P) (p : P → ℝ) (hp : ∀ x, 0≤p x) : (∑ x, ∑ y, p x*p y*min (d.potential x+d'.potential x) (d.potential y+d'.potential y)) ≤ 2*((∫ r, (d.outsideMass p r)^2)+(∫ r, (d'.outsideMass p r)^2)) := by …Mentions: OAI.WeakPinned.Hierarchy.Depth
- lemma
OAI.WeakPinned.Hierarchy.Depth.outsideMass_probline 353 - lemma
OAI.WeakPinned.Hierarchy.Depth.outsideMass_zeroline 361 - lemma
OAI.WeakPinned.Hierarchy.Depth.sumCells_nonnegline 364 - lemma
OAI.WeakPinned.Hierarchy.Depth.complement_le_sumCellsline 368 - lemma
OAI.WeakPinned.Hierarchy.Depth.outside_square_boundline 376 - lemma
OAI.WeakPinned.Hierarchy.Depth.integrable_outsideMass_squareline 394 - lemma
OAI.WeakPinned.Hierarchy.Depth.integral_outsideMassline 400 - theorem
OAI.WeakPinned.Hierarchy.Depth.integrated_outside_squareline 408Source documentation
The integrable complement second moment estimate. All singleton terms are charged to the finite potential, not integrated as constant errors.
theorem integrated_outside_square (hn : 2≤Fintype.card P) (w : I → ℝ) (B : I → Finset P) (T M κ : ℝ) (hw : ∀ i, 0≤w i) (hW : (∑ i, w i)≤1) (hT : 1≤T) (hκ : 0≤κ) (hB : ∀ i, 2≤(B i).card) (hk : ∀ i, 2/((B i).card:ℝ)≤κ) (hdom : ∀ x, (∑ i, w i*prob (B i) x)≤M*prob Finset.univ x) : (∑ i, w i*(∫ r, (d.outsideMass (prob (B i)) r)^2)) ≤ 2*weightedIntegral d.mass (varianceCell w B T) + 4*weightedIntegral d.mass (pairCell Finset.univ) + κ*M*(∑ x, prob Finset.univ x*d.potential x) := by …Mentions: OAI.WeakPinned.B, OAI.WeakPinned.Hierarchy.Depth.M
- lemma
OAI.WeakPinned.MinKernel.energy_lowerline 448Source documentation
A fiber whose potential is a constant plus nonnegative overlap and a small signed grid error has a large iid minimum. This preserves self-pairs in the sampling, exactly as in the unbounded-scale argument.
lemma energy_lower (p S L E : P → ℝ) (c : ℝ) (hp : ∀ x, 0≤p x) (hsum : (∑ x, p x)=1) (hL : ∀ x, 0≤L x) (hS : ∀ x, p x≠0 → S x=c+L x-E x) : (∑ x, p x*S x)-(∑ x, p x*L x)-(∑ x, p x*|E x|)≤energy p S S := by …Mentions: OAI.WeakPinned.MinKernel.energy
- lemma
OAI.WeakPinned.Hierarchy.Depth.min_upper_familyline 483 - lemma
OAI.WeakPinned.Hierarchy.Depth.local_potential_fiber_boundline 508