import OAI.Geometry.RCD.Coordinates.TransverseFrameData namespace OAI /-! # Bounded axial and transverse potentials before imposing any Gram identities -/ open Set Filter MeasureTheory Finset open scoped NNReal InnerProductSpace noncomputable section namespace RegularPointCoordinates variable {X : Type*} [MetricSpace X] [MeasurableSpace X] (μ : Measure X) (Q : QuadraticCheegerEnergy μ) theorem bounded_transverse_potentials {n : ℕ} (u : Fin n → SobolevSpace μ Q) (A : Fin n → ℝ≥0) (hA : ∀ i, ∀ᵐ x ∂μ, |SobolevSpace.toLp μ Q (u i) x|≤A i) (Ω : Set X) (v : X → Euclidean n) (hu : ∀ i, SobolevSpace.toLp μ Q (u i) =ᵐ[μ.restrict Ω] fun x => v x i) (hH : ∀ i, IsSobolevHarmonicOn μ Q Ω (u i)) (a : Euclidean n) : ∃ (w s : SobolevSpace μ Q) (B D : ℝ≥0), (∀ᵐ x ∂μ, |SobolevSpace.toLp μ Q w x|≤B) ∧ (∀ᵐ x ∂μ, |SobolevSpace.toLp μ Q s x|≤D) ∧ (SobolevSpace.toLp μ Q w =ᵐ[μ.restrict Ω] fun x => ⟪v x,a⟫_ℝ) ∧ (SobolevSpace.toLp μ Q s =ᵐ[μ.restrict Ω] fun x => ‖v x‖^2-⟪v x,a⟫_ℝ^2) ∧ IsSobolevHarmonicOn μ Q Ω w ∧ w=sobolevColumnMap μ Q u a ∧ s=(∑ i, SobolevSpace.square μ Q (u i) (A i))-SobolevSpace.square μ Q w B := by let w := sobolevColumnMap μ Q u a let B : ℝ≥0 := ∑ i, ‖a i‖₊*A i have hwglobal : SobolevSpace.toLp μ Q w =ᵐ[μ] fun x => ∑ i, a i*SobolevSpace.toLp μ Q (u i) x := by have h := sobolevColumnMap_representative μ Q u univ (fun x => WithLp.toLp 2 (fun i => SobolevSpace.toLp μ Q (u i) x)) (fun _ => EventuallyEq.rfl) a simpa only [Measure.restrict_univ,PiLp.inner_apply,RCLike.inner_apply,conj_trivial] using h have hwB : ∀ᵐ x ∂μ, |SobolevSpace.toLp μ Q w x|≤B := by filter_upwards [hwglobal,ae_all_iff.mpr hA] with x hx hb rw [hx] calc _ ≤ ∑ i, |a i*SobolevSpace.toLp μ Q (u i) x| := Finset.abs_sum_le_sum_abs _ _ _ ≤ ∑ i, |a i| * (A i:ℝ) := sum_le_sum (fun i _ => by rw [abs_mul]; exact mul_le_mul_of_nonneg_left (hb i) (abs_nonneg _)) _ = B := by simp [B,Real.norm_eq_abs] let z := ∑ i, SobolevSpace.square μ Q (u i) (A i) have hz : SobolevSpace.toLp μ Q z =ᵐ[μ] fun x => ∑ i, (SobolevSpace.toLp μ Q (u i) x)^2 := by change SobolevSpace.toLpCLM μ Q (∑ i, SobolevSpace.square μ Q (u i) (A i)) =ᵐ[μ] _ rw [map_sum] change (∑ i, SobolevSpace.toLp μ Q (SobolevSpace.square μ Q (u i) (A i))) =ᵐ[μ] _ filter_upwards [Lp.coeFn_finsetSum univ (fun i => SobolevSpace.toLp μ Q (SobolevSpace.square μ Q (u i) (A i))),ae_all_iff.mpr (fun i => SobolevSpace.square_coe μ Q (u i) (A i) (hA i))] with x hx hs rw [hx] simp only [Finset.sum_apply,hs] let s := z-SobolevSpace.square μ Q w B have hs : SobolevSpace.toLp μ Q s =ᵐ[μ] fun x => (∑ i, (SobolevSpace.toLp μ Q (u i) x)^2)-(SobolevSpace.toLp μ Q w x)^2 := by filter_upwards [hz,SobolevSpace.square_coe μ Q w B hwB, Lp.coeFn_sub (SobolevSpace.toLp μ Q z) (SobolevSpace.toLp μ Q (SobolevSpace.square μ Q w B))] with x hx hy hsub change (SobolevSpace.toLp μ Q z-SobolevSpace.toLp μ Q (SobolevSpace.square μ Q w B)) x=_ simp only [hsub,Pi.sub_apply,hx,hy] let D : ℝ≥0 := (∑ i, A i^2)+B^2 have hsD : ∀ᵐ x ∂μ, |SobolevSpace.toLp μ Q s x|≤D := by filter_upwards [hs,ae_all_iff.mpr hA,hwB] with x hx hb hw rw [hx] calc _ ≤ |∑ i, (SobolevSpace.toLp μ Q (u i) x)^2|+|(SobolevSpace.toLp μ Q w x)^2| := abs_sub _ _ _ = (∑ i, |SobolevSpace.toLp μ Q (u i) x|^2)+|SobolevSpace.toLp μ Q w x|^2 := by rw [abs_of_nonneg (sum_nonneg (fun _ _ => sq_nonneg _))] simp only [abs_pow,sq_abs] _ ≤ (∑ i, (A i:ℝ)^2)+(B:ℝ)^2 := add_le_add (sum_le_sum (fun i _ => pow_le_pow_left₀ (abs_nonneg _) (hb i) 2)) (pow_le_pow_left₀ (abs_nonneg _) hw 2) _ = D := by simp [D] have hw := sobolevColumnMap_representative μ Q u Ω v hu a refine ⟨w,s,B,D,hwB,hsD,hw,?_,IsSobolevHarmonicOn.linearCombination μ Q hH a,rfl,rfl⟩ · filter_upwards [ae_restrict_of_ae hs,ae_all_iff.mpr hu,hw] with x hx hux hwx rw [hx,hwx,EuclideanSpace.real_norm_sq_eq] simp only [hux] end RegularPointCoordinates end end OAI