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import OAI.Geometry.RuledCovering.NilpotentLattice
namespace OAI
noncomputable section
open Set MeasureTheory Filter Metric
open scoped Topology ContDiff Pointwise
namespace RuledApproximation
/-- Convert the finite weighted lattice certificate into actual perpendicular Euclidean cylinders.
The factor is the exact area inflation caused by the derivative remainder. -/
theorem framed_local_cover_of_shape (M : Coordinates ≃L[ℝ] Plane) {h L R delta : ℝ}
(shape : Cylinder → Prop)
(hshape : ∀ b : Coordinates, ∀ a : ℝ, 0 < a → ∀ g : Plane,
shape (projectedCylinder h g (M '' closedBall b a)))
(hh : 0 < h) (hL : 0 ≤ L) (hR : 0 ≤ R) (hd : 0 ≤ delta)
{K U : Set Coordinates} (hK : IsCompact K) (hU : IsOpen U) (hKU : K ⊆ U)
(v : Plane → Plane) (A : Coordinates →L[ℝ] Coordinates)
(hmodel : LatticeModel A L R)
(hrem : ∀ p ∈ U, ∀ b ∈ U,
‖M.symm (v (M p)) - M.symm (v (M b)) - A (p - b)‖ ≤ delta * ‖p - b‖)
{F : Coordinates → ℝ} (hF : Continuous F) (hFpos : ∀ p, 0 ≤ F p)
(hFval : ∀ p ∈ U, F p = physicalWeight h (v (M p)))
{eps : ℝ} (heps : 0 < eps) :
HasFiniteCover shape (physicalRuled h (M '' K) v L)
(h * (1 + 2 * L * delta * R) ^ 2 *
(∫ p in M '' K, physicalWeight h (v p)) + eps) := by
classical
let B : ℝ := (1 + 2 * L * delta * R) ^ 2
have hB : 0 < B := by dsimp [B]; positivity
have hscale : 0 < h * frameJacobian M * B := mul_pos (mul_pos hh (frameJacobian_pos M)) hB
obtain ⟨n, hn, S, hS, hSU, hcov, hcost⟩ := local_finite_certificate hK hU hKU
(fun p => M.symm (v (M p))) A hL hd hmodel hrem hF hFpos (div_pos heps hscale)
let : Fintype S := hS.fintype
let a : ℝ := (1 / 2 + L * delta * R) / n
have hnR : 0 < (n : ℝ) := by exact_mod_cast hn
have ha : 0 < a := by dsimp [a]; positivity
let C : S → Cylinder := fun b => projectedCylinder h (v (M b)) (M '' closedBall (b : Coordinates) a)
have harea (b : S) : (C b).area = h * frameJacobian M * (2 * a) ^ 2 * F b := by
dsimp only [C]
rw [projectedCylinder_area hh, frame_volume_image M isClosed_closedBall.measurableSet,
coordinates_closedBall_volume b ha.le, hFval b (hSU b.property)]
ring
have hBrel : (2 * a) ^ 2 = B / (n : ℝ) ^ 2 := by
dsimp [a, B]
ring
have hintegral : (∫ p in M '' K, physicalWeight h (v p)) =
frameJacobian M * ∫ x in K, F x := by
rw [frame_integral_image M hK.measurableSet]
congr 1
apply setIntegral_congr_fun hK.measurableSet
intro x hx
exact (hFval x (hKU hx)).symm
apply HasFiniteCover.of_fintype C
· intro b
exact hshape b a ha (v (M b))
· rintro x ⟨_, ⟨p, hp, rfl⟩, s, hs, rfl⟩
obtain ⟨b, hb, hc⟩ := hcov p hp s hs
apply mem_iUnion.mpr
refine ⟨⟨b, hb⟩, ?_⟩
apply physicalRuled_mem_projectedCylinder
refine ⟨p + s • (M.symm (v (M p)) - M.symm (v (M b))), ?_, ?_⟩
· rw [mem_closedBall, dist_eq_norm]
convert hc using 1
congr 1
module
· simp
· have hsum : (∑ b : S, (C b).area) =
(h * frameJacobian M * B) * ((∑' b : S, F b) / (n : ℝ) ^ 2) := by
simp_rw [harea, hBrel]
rw [tsum_fintype, ← Finset.mul_sum]
ring
rw [hsum, hintegral]
have hc := (mul_lt_mul_of_pos_left hcost hscale).le
calc
_ ≤ (h * frameJacobian M * B) *
((∫ x in K, F x) + eps / (h * frameJacobian M * B)) := hc
_ = _ := by
rw [mul_add, mul_div_cancel₀ _ hscale.ne']
dsimp [B]
ring
/-- Every square-zero label has a patch whose compact subsets admit finite covers,
with one prescribed arbitrarily small area inflation. -/
theorem nilpotent_local_patch {h B : ℝ} (hh : 0 < h) (hB : 1 < B)
{v : Plane → Plane} {U : Set Plane} (hU : IsOpen U) (hv : ContDiffOn ℝ 1 v U)
{p : Plane} (hp : p ∈ U) (hnil : (fderiv ℝ v p).comp (fderiv ℝ v p) = 0) :
∃ V : Set Plane, IsOpen V ∧ p ∈ V ∧ ∀ K : Set Plane, IsCompact K → K ⊆ V →
∀ eps : ℝ, 0 < eps → HasFiniteCover (squareProjected h) (physicalRuled h K v 1)
(h * B * (∫ q in K, physicalWeight h (v q)) + eps) := by
obtain ⟨Q, d, hQ⟩ := nilpotent_frame (fderiv ℝ v p) hnil
let M := orthogonalFrame Q
have hM (z : Coordinates) : M.symm ((fderiv ℝ v p) (M z)) = ![d*z 1,0] := by
have hz := congrArg WithLp.ofLp (hQ (WithLp.toLp 2 z))
exact hz
let A : Coordinates →L[ℝ] Coordinates := d • shearCLM
let R : ℝ := (1+|d|)/2
have hR : 0 < R := by dsimp [R]; positivity
have hmodel : LatticeModel A 1 R := nilpotent_lattice_model d
obtain ⟨delta, hd, hDB⟩ := exists_small_inflation 1 R hB
let w : Coordinates → Coordinates := fun x => M.symm (v (M x))
let Uc : Set Coordinates := M ⁻¹' U
have hUco : IsOpen Uc := hU.preimage M.continuous
have hpc : M.symm p ∈ Uc := by simpa [Uc]
have hvc : ContDiffOn ℝ 1 (fun x => v (M x)) Uc :=
hv.comp M.contDiff.contDiffOn (fun x hx => hx)
have hwc : ContDiffOn ℝ 1 w Uc := M.symm.contDiff.comp_contDiffOn hvc
have hvder := (hv.contDiffAt (hU.mem_nhds hp)).differentiableAt (by norm_num)
have hwd : fderiv ℝ w (M.symm p) = A := by
have hvd : HasFDerivAt (fun x => v (M x))
((fderiv ℝ v p).comp M.toContinuousLinearMap) (M.symm p) := by
have hvdp : HasFDerivAt v (fderiv ℝ v p) (M (M.symm p)) := by
simpa using hvder.hasFDerivAt
exact hvdp.comp (M.symm p) M.hasFDerivAt
have hcomp := M.symm.hasFDerivAt.comp (M.symm p) hvd
change fderiv ℝ (M.symm ∘ (fun x => v (M x))) (M.symm p) = A
rw [hcomp.fderiv]
ext z i
have hz := congrArg (fun a : Coordinates => a i) (hM z)
fin_cases i <;> simpa [A, shearCLM, shearLinear] using hz
obtain ⟨r, hr, hrU, hrem⟩ := c1_local_remainder hUco hwc hpc hd
let Vc := ball (M.symm p) (r / 2)
have hrhalf : r / 2 < r := by linarith
have hclU : closedBall (M.symm p) (r / 2) ⊆ Uc :=
(closedBall_subset_ball hrhalf).trans hrU
have hclF : ContinuousOn (fun x => physicalWeight h (v (M x)))
(closedBall (M.symm p) (r / 2)) :=
(physicalWeight_continuous h).comp_continuousOn (hvc.continuousOn.mono hclU)
obtain ⟨F, hF, hFnon, hFeq⟩ := continuous_nonneg_extension isClosed_closedBall hclF
(fun x _ => (physicalWeight_pos h (v (M x))).le)
refine ⟨M '' Vc, M.isOpenMap _ isOpen_ball, ?_, ?_⟩
· exact ⟨M.symm p, mem_ball_self (half_pos hr), M.apply_symm_apply p⟩
· intro K hK hKV eps heps
let Kc := M.symm '' K
have hKc : IsCompact Kc := hK.image M.symm.continuous
have hKcV : Kc ⊆ Vc := by
rintro _ ⟨q, hq, rfl⟩
obtain ⟨x, hx, rfl⟩ := hKV hq
simpa using hx
have himg : M '' Kc = K := by simp [Kc]
have hc := framed_local_cover_of_shape M (squareProjected h)
(fun b a ha g => ⟨_,g,orthogonal_closedBall_square Q b ha,rfl⟩)
hh (by norm_num : (0:ℝ)≤1) hR.le hd.le hKc isOpen_ball hKcV v A hmodel
(fun x hx y hy => by
rw [← hwd]
exact hrem x (ball_subset_ball hrhalf.le hx) y (ball_subset_ball hrhalf.le hy))
hF hFnon (fun x hx => hFeq (ball_subset_closedBall hx)) heps
rw [himg] at hc
apply hc.mono Subset.rfl
have hI : 0 ≤ ∫ q in K, physicalWeight h (v q) :=
integral_nonneg (fun q => (physicalWeight_pos h (v q)).le)
linarith [mul_le_mul_of_nonneg_right (mul_le_mul_of_nonneg_left hDB.le hh.le) hI]
/-- Finite square-tile approximation, with unrestricted local shear and arbitrary
compact labels. -/
theorem nilpotent_physical_cover {h : ℝ} {D : Set Plane} {v : Plane → Plane}
(hh : 0 < h) (hD : IsCompact D) (hv : SmoothNear 1 D v)
(hnil : ∀ p ∈ D, (fderiv ℝ v p).comp (fderiv ℝ v p) = 0)
{eps : ℝ} (heps : 0 < eps) :
HasFiniteCover (squareProjected h) (physicalRuled h D v 1)
(h * (∫ p in D, physicalWeight h (v p)) + eps) := by
obtain ⟨U, hU, hDU, hv⟩ := hv
have hF : IntegrableOn (fun p => physicalWeight h (v p)) D :=
((physicalWeight_continuous h).comp_continuousOn (hv.continuousOn.mono hDU)).integrableOn_compact hD
obtain ⟨B, hB, hbudget⟩ := exists_inflation_budget
(h * ∫ p in D, physicalWeight h (v p)) (half_pos heps)
have hc := globalize_local_covers h 1 v (fun p => physicalWeight h (v p)) (h*B) hD hF
(fun p hp => nilpotent_local_patch hh hB hU hv (hDU hp) (hnil p hp)) (half_pos heps)
apply hc.mono Subset.rfl
nlinarith
lemma unitSquare_parallelogram : IsParallelogram unitSquare := by
have he : unitSquare = (EuclideanSpace.equiv (Fin 2) ℝ).symm ''
closedBall (0 : Coordinates) (1/2:ℝ) := by
ext x
constructor
· intro hx
refine ⟨WithLp.ofLp x, ?_, rfl⟩
rw [mem_closedBall,dist_zero_right,pi_norm_le_iff_of_nonneg (by norm_num : (0:ℝ)≤1/2)]
exact hx
· rintro ⟨y,hy,rfl⟩
rw [mem_closedBall,dist_zero_right,pi_norm_le_iff_of_nonneg (by norm_num : (0:ℝ)≤1/2)] at hy
exact hy
rw [he]
exact (coordinates_closedBall_parallelogram 0 (by norm_num : (0:ℝ)<1/2)).linear_image
(EuclideanSpace.equiv (Fin 2) ℝ).symm.toLinearMap
(EuclideanSpace.equiv (Fin 2) ℝ).symm.injective
lemma IsSquareTile.parallelogram {T : Set Plane} (hT : IsSquareTile T) :
IsParallelogram T := by
obtain ⟨c,R,a,ha,rfl⟩ := hT
have hi : Function.Injective (a • R.toLinearMap) := by
intro x y hxy
apply R.injective
exact (smul_right_injective Plane ha.ne') hxy
have he : (fun x => c+a • R x) '' unitSquare =
(fun x => c+x) '' ((a • R.toLinearMap) '' unitSquare) := by
rw [← image_comp]
rfl
rw [he]
exact (unitSquare_parallelogram.linear_image (a • R.toLinearMap) hi).translate c
end RuledApproximation
end
end OAI