import OAI.Geometry.HarmonicGrowth.PulseSystem import OAI.Geometry.HarmonicGrowth.AngularStream namespace OAI noncomputable section namespace HarmonicCounterexample.LinearODE variable {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] open scoped InnerProductSpace lemma weighted_slope_gap_deriv {A S : ℝ → E →L[ℝ] E} {b : ℝ → ℝ} (hb : Continuous b) {C t : ℝ} (hS : (S t).IsSymmetric) (hD : HasDerivAt S (A t-b t • S t-S t*S t) t) (v : E) : HasDerivAt (fun s => integratingWeight (fun s => 2*C+b s) s * ⟪v,C • v-S s v⟫_ℝ) (integratingWeight (fun s => 2*C+b s) t * (‖C • v-S t v‖^2+(C^2+b t*C)*‖v‖^2-⟪v,A t v⟫_ℝ)) t := by have hv : HasDerivAt (fun s => C • v-S s v) (-(A t v-b t • S t v-S t (S t v))) t := by simpa only [map_zero,add_zero,sub_apply,smul_apply,mul_apply_eq_comp,zero_sub] using (hasDerivAt_const t (C • v)).fun_sub (hD.clm_apply (hasDerivAt_const t v)) have hd := (integratingWeight_deriv (b := fun s => 2*C+b s) (continuous_const.add hb) t).fun_mul ((hasDerivAt_const t v).inner ℝ hv) have hs : ⟪v,S t (S t v)⟫_ℝ = ‖S t v‖^2 := by calc ⟪v,S t (S t v)⟫_ℝ = ⟪S t v,S t v⟫_ℝ := (hS v (S t v)).symm _ = ‖S t v‖^2 := real_inner_self_eq_norm_sq _ have hn : ‖C • v-S t v‖^2 = C^2*‖v‖^2-2*C*⟪v,S t v⟫_ℝ+‖S t v‖^2 := by rw [norm_sub_sq_real,norm_smul,Real.norm_eq_abs,mul_pow,sq_abs, real_inner_smul_left] ring convert hd using 1; first | rfl | (simp only [inner_zero_left,inner_neg_right,inner_sub_right, inner_smul_right,real_inner_self_eq_norm_sq,hs,hn]; ring) lemma riccati_quadratic_upper {A S : ℝ → E →L[ℝ] E} {b : ℝ → ℝ} (hb : Continuous b) {C l MA Mb : ℝ} (hC : 0 ≤ C) (hlC : l ≤ C) (hbnd : ∀ t, |b t| ≤ Mb) (hCbound : MA ≤ C^2-Mb*C) (hAbnd : ∀ t v, ⟪v,A t v⟫_ℝ ≤ MA*‖v‖^2) (hS : ∀ t, 0 ≤ t → (S t).IsSymmetric) (hD : ∀ t, 0 ≤ t → HasDerivAt S (A t-b t • S t-S t*S t) t) (hi : S 0 = l • (1 : E →L[ℝ] E)) {t : ℝ} (ht : 0 ≤ t) (v : E) : ⟪v,S t v⟫_ℝ ≤ C*‖v‖^2 := by let F (s : ℝ) := integratingWeight (fun s => 2*C+b s) s * ⟪v,C • v-S s v⟫_ℝ have hnonneg (s : ℝ) : 0 ≤ ‖C • v-S s v‖^2+(C^2+b s*C)*‖v‖^2-⟪v,A s v⟫_ℝ := by have hb0 : -Mb ≤ b s := (abs_le.1 (hbnd s)).1 have hcoef : MA ≤ C^2+b s*C := by nlinarith [mul_le_mul_of_nonneg_right hb0 hC] have := mul_le_mul_of_nonneg_right hcoef (sq_nonneg ‖v‖) have := hAbnd s v nlinarith [sq_nonneg ‖C • v-S s v‖] have hmono : MonotoneOn F (Set.Ici (0:ℝ)) := by apply monotoneOn_of_hasDerivWithinAt_nonneg (convex_Ici 0) · intro s hs exact (weighted_slope_gap_deriv hb (hS s hs) (hD s hs) v).continuousAt.continuousWithinAt · intro s hs exact (weighted_slope_gap_deriv hb (hS s (interior_subset hs)) (hD s (interior_subset hs)) v).hasDerivWithinAt · intro s _ exact mul_nonneg (integratingWeight_pos _ _).le (hnonneg s) have hzero : 0 ≤ F 0 := by simp only [F,hi,integratingWeight_initial,one_mul,smul_apply,one_apply_eq_self, inner_sub_right,inner_smul_right,real_inner_self_eq_norm_sq] nlinarith [sq_nonneg ‖v‖] have hpos : 0 ≤ F t := hzero.trans (hmono (by simp : (0:ℝ) ∈ Set.Ici (0:ℝ)) ht ht) have hiq : 0 ≤ ⟪v,C • v-S t v⟫_ℝ := (mul_nonneg_iff_of_pos_left (integratingWeight_pos _ _)).1 hpos simpa only [inner_sub_right,inner_smul_right,real_inner_self_eq_norm_sq,sub_nonneg] using hiq lemma symmetric_norm_bound {S : E →L[ℝ] E} {C : ℝ} (hC : 0 ≤ C) (hs : S.IsSymmetric) (hpos : ∀ v, 0 ≤ ⟪v,S v⟫_ℝ) (hb : ∀ v, ⟪v,S v⟫_ℝ ≤ C*‖v‖^2) : ‖S‖ ≤ C := by rw [S.norm_eq_iSup_rayleighQuotient hs] apply ciSup_le intro v by_cases hv : v = 0 · simp [hv,hC] · have hn : 0 < ‖v‖^2 := sq_pos_of_pos (norm_pos_iff.2 hv) have hp := hpos v have hupper := hb v change |⟪S v,v⟫_ℝ / ‖v‖^2| ≤ C rw [real_inner_comm v (S v),abs_of_nonneg (div_nonneg hp hn.le)] exact (div_le_iff₀ hn).2 hupper end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open scoped InnerProductSpace variable {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] /-- The history-independent Riccati bound is proved for the actual center-regular PB solution. It is not an assumption on an arbitrary incoming solution. -/ theorem actual_slope_norm_bound {A : ℝ → E →L[ℝ] E} {p : ℝ → ℝ} (hA : Continuous A) (hp : Continuous p) {MA Mp : ℝ} (hMA : 0 ≤ MA) (hMp : 0 ≤ Mp) (hAn : ∀ t,‖A t‖ ≤ MA) (hpn : ∀ t,|p t| ≤ Mp) (hAs : ∀ t x y,inner ℝ (A t x) y=inner ℝ x (A t y)) (hAp : ∀ t x,0 ≤ inner ℝ x (A t x)) {l B : ℝ} (hl : 0 < l) (hAc : ∀ t ≤ 0,∀ x,A t x=(l*(l+B)) • x) (hpc : ∀ t ≤ 0,p t=B) {t : ℝ} (ht : 0 ≤ t) : ‖slope A p l t‖ ≤ l+MA+Mp+1 := by let C := l+MA+Mp+1 have hC : 0 ≤ C := by dsimp [C];linarith have hCbound : MA ≤ C^2-Mp*C := by have hc1 : 1 ≤ C-Mp := by dsimp [C];linarith have hc2 : MA ≤ C := by dsimp [C];linarith have hm := mul_le_mul_of_nonneg_left hc1 hC nlinarith have hu (s : ℝ) := actual_value_unit_all_time hA hp hMA hMp hAn hpn hAp hl hAc hpc s have hsym (s : ℝ) : (slope A p l s).IsSymmetric := slope_symmetric hA hp hMA hMp hAn hpn hAs l s (hu s) apply symmetric_norm_bound hC (hsym t) · exact slope_nonnegative hA hp hMA hMp hAn hpn hAp hl ht (hu t) · apply riccati_quadratic_upper hp hC (show l ≤ C by dsimp [C];linarith) hpn hCbound · intro s x calc inner ℝ x (A s x) ≤ ‖x‖*‖A s x‖ := real_inner_le_norm _ _ _ ≤ ‖x‖*(MA*‖x‖) := mul_le_mul_of_nonneg_left (((A s).le_opNorm x).trans (mul_le_mul_of_nonneg_right (hAn s) (norm_nonneg x))) (norm_nonneg x) _ = MA*‖x‖^2 := by ring · intro s _;exact hsym s · intro s _;exact slope_deriv hA hp hMA hMp hAn hpn l s (hu s) · exact slope_initial A p l · exact ht end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses open scoped Topology Matrix.Norms.Frobenius InnerProductSpace variable {E ι : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E] [FiniteDimensional ℝ E] [Fintype ι] [DecidableEq ι] local instance : NormedAddCommGroup (E →L[ℝ] E) := ContinuousLinearMap.toNormedAddCommGroup local instance : NormedSpace ℝ (E →L[ℝ] E) := ContinuousLinearMap.toNormedSpace local instance : NormedAddCommGroup ((E →L[ℝ] E) →L[ℝ] Matrix ι ι ℝ) := ContinuousLinearMap.toNormedAddCommGroup local instance : NormedSpace ℝ ((E →L[ℝ] E) →L[ℝ] Matrix ι ι ℝ) := ContinuousLinearMap.toNormedSpace /-- A single late threshold resets EVERY positive symmetric bounded history. Only the actual preceding round interval is used. -/ theorem uniform_round_reset (basis : OrthonormalBasis ι ℝ E) {α p : ℝ → ℝ} (hp : Continuous p) {β p₀ γ θ B l B₀ MA Mp : ℝ} (hαlim : Tendsto α atTop (𝓝 β)) (hplim : Tendsto p atTop (𝓝 p₀)) (hγ : 0 < γ) (hθ : 0 < θ) (hpl : ∀ᶠ t in atTop,γ ≤ p t) (hroot : β*B-p₀*θ-θ^2=0) (hMA : 0 ≤ MA) (hMp : 0 ≤ Mp) (hpn : ∀ t,|p t| ≤ Mp) (hl : 0 < l) (hpc : ∀ t ≤ 0,p t=B₀) {ε : ℝ} (hε : 0 < ε) : ∃ J : ℕ,∀ j,J ≤ j → ∀ A : ℝ → E →L[ℝ] E, Continuous A → (∀ t,‖A t‖ ≤ MA) → (∀ t x y,inner ℝ (A t x) y=inner ℝ x (A t y)) → (∀ t x,0 ≤ inner ℝ x (A t x)) → (∀ t ≤ 0,∀ x,A t x=(l*(l+B₀)) • x) → (∀ t ∈ Icc (time j+3*pulse j+dwell j) (time (j+1)), A t=α t • (B • (1:E →L[ℝ] E))) → ‖orthogonalMatrix basis (slope A p l (time (j+1)))-θ • (1:Matrix ι ι ℝ)‖ ≤ ε := by let lam := γ+θ have hlam : 0 < lam := by dsimp [lam];linarith let C := ‖orthogonalMatrix basis‖*(l+MA+Mp+1)+|θ| * ‖(1:Matrix ι ι ℝ)‖ let M := ε/2*lam have hM : 0 < M := mul_pos (by linarith) hlam have hroot' : β*B-(p₀*θ+θ^2)=0 := by linarith have hf : Tendsto (fun t : ℝ => ‖(α t*B-(p t*θ+θ^2)) • (1:Matrix ι ι ℝ)‖) atTop (𝓝 0) := by have hh := (((hαlim.mul_const B).sub ((hplim.mul_const θ).add_const (θ^2))).smul_const (1:Matrix ι ι ℝ)).norm simpa only [hroot',zero_smul,norm_zero] using hh obtain ⟨a₀,ha₀⟩ := eventually_atTop.1 ((hf.eventually (gt_mem_nhds hM)).and hpl) have he : Tendsto (fun j => C*Real.exp (-lam*pulse j)) atTop (𝓝 0) := by have hh := (Real.tendsto_exp_neg_atTop_nhds_zero.comp (pulse_atTop_limit.const_mul_atTop hlam)).const_mul C simpa only [Function.comp_apply,neg_mul,mul_zero] using hh obtain ⟨J,hJ⟩ := eventually_atTop.1 ((time_atTop.eventually_ge_atTop a₀).and (he.eventually (gt_mem_nhds (show 0<ε/2 by linarith)))) refine ⟨J,fun j hj A hA hAn hAs hAp hAc hround => ?_⟩ let a := time j+3*pulse j+dwell j have ha : 0 ≤ a := by dsimp [a];linarith [time_pos j,pulse_pos j,dwell_pos j] have hab : a ≤ time (j+1) := by dsimp [a];rw [time_succ];linarith [pulse_pos j] have hat (t : ℝ) (ht : t ∈ Icc a (time (j+1))) : a₀ ≤ t := by have := (hJ j hj).1 dsimp [a] at ht linarith [ht.1,pulse_pos j,dwell_pos j] have hinit : ‖orthogonalMatrix basis (slope A p l a)-θ • (1:Matrix ι ι ℝ)‖ ≤ C := by calc _ ≤ ‖orthogonalMatrix basis (slope A p l a)‖+‖θ • (1:Matrix ι ι ℝ)‖ := norm_sub_le _ _ _ ≤ ‖orthogonalMatrix basis‖*(l+MA+Mp+1)+|θ| * ‖(1:Matrix ι ι ℝ)‖ := by rw [norm_smul,Real.norm_eq_abs] exact add_le_add (((orthogonalMatrix basis).le_opNorm _).trans (mul_le_mul_of_nonneg_left (actual_slope_norm_bound hA hp hMA hMp hAn hpn hAs hAp hl hAc hpc ha) (norm_nonneg _))) le_rfl _ = C := rfl have hforce (t : ℝ) (ht : t ∈ Icc a (time (j+1))) : ‖orthogonalMatrix basis (A t)-(p t*θ+θ^2) • (1:Matrix ι ι ℝ)‖ ≤ M := by rw [hround t ht,map_smul,map_smul,orthogonalMatrix_one,smul_smul,← sub_smul] exact (ha₀ t (hat t ht)).1.le have hh := actual_round_reset basis hA hp hMA hMp hAn hpn hAp hl hAc hpc ha hlam hM.le (fun t ht => (ha₀ t (hat t ht)).2) hforce hinit (time (j+1)) ⟨hab,le_rfl⟩ have hlen : time (j+1)-a=pulse j := by dsimp [a];rw [time_succ];ring rw [hlen] at hh have hdiv : M/lam=ε/2 := by dsimp [M];exact mul_div_cancel_right₀ _ (ne_of_gt hlam) change _ ≤ C*Real.exp (-lam*pulse j)+M/lam at hh rw [hdiv] at hh linarith [(hJ j hj).2] end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open scoped Topology ContDiff InnerProductSpace Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace /-- Primitive radial coefficients and fixed angular operators. All fields are scalar/asymptotic or pointwise geometric facts; no transmission/reset/growth conclusion is part of this data. -/ structure HistoryGeometry (S : PulseSystem E ι κ) where D₀ : ∀ b,E b →L[ℝ] E b D₀nonpos : ∀ b v,inner ℝ v (D₀ b v) ≤ 0 BD₀ : ∀ b v,-(S.B b*‖v‖^2) ≤ inner ℝ v (D₀ b v) D₀symm : ∀ b x y,inner ℝ (D₀ b x) y=inner ℝ x (D₀ b y) Dsymm : ∀ b j x y,inner ℝ (S.D b j x) y=inner ℝ x (S.D b j y) qstar : ℝ qstar_ge : 1 ≤ qstar l : ξ → ℝ lpos : ∀ b,0 < l b B₀ : ℝ B_eq : ∀ b,S.B b=l b*(l b+B₀) α : ℝ → ℝ drift : ℝ → ℝ Mp : ℝ Mpnonneg : 0 ≤ Mp αsmooth : ContDiff ℝ ∞ α driftContinuous : Continuous drift αbound : ∀ t,|α t| ≤ S.M αnonneg : ∀ t,0 ≤ α t driftBound : ∀ t,|drift t| ≤ Mp αcenter : ∀ t ≤ 0,α t=1 driftCenter : ∀ t ≤ 0,drift t=B₀ αlimit : ∀ b,Tendsto α atTop (𝓝 (S.β b)) driftLimit : Tendsto drift atTop (𝓝 S.p₀) driftLower : ∀ᶠ t in atTop,S.γ ≤ drift t variable {S : PulseSystem E ι κ} (G : HistoryGeometry S) {n : ℕ} [NeZero n] (slot : Fin n → κ) def HistoryGeometry.coefficient (s : ℕ → Fin n → ℝ) (j0 : ℕ) (b : ξ) (t : ℝ) : E b →L[ℝ] E b := G.α t • angular S.r (S.B b • (1:E b →L[ℝ] E b)) (G.D₀ b) (fun i => S.D b (slot i)) s G.qstar j0 t def HistoryGeometry.bound (b : ξ) : ℝ := S.M * (angular_uniform_bound S.r (S.B b • (1:E b →L[ℝ] E b)) (G.D₀ b) (fun i => S.D b (slot i)) G.qstar_ge).choose omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.bound_nonneg (b : ξ) : 0 ≤ G.bound slot b := mul_nonneg S.hM (angular_uniform_bound S.r (S.B b • (1:E b →L[ℝ] E b)) (G.D₀ b) (fun i => S.D b (slot i)) G.qstar_ge).choose_spec.1 variable (s : ℕ → Fin n → ℝ) (j0 : ℕ) (hpos : ∀ j,j0 ≤ j → ∀ t i,packetStretch (s j) (pulse j) t i ∈ Icc (1/2:ℝ) (3/2)) include hpos omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.coefficient_smooth (b : ξ) : ContDiff ℝ ∞ (G.coefficient slot s j0 b) := G.αsmooth.smul (angular_smooth S.r _ _ _ s G.qstar_ge j0 (fun j hj t i => by linarith [(hpos j hj t i).1])) omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.coefficient_bound (b : ξ) (t : ℝ) : ‖G.coefficient slot s j0 b t‖ ≤ G.bound slot b := by rw [HistoryGeometry.coefficient,norm_smul,Real.norm_eq_abs] apply mul_le_mul (G.αbound t) ((angular_uniform_bound S.r (S.B b • (1:E b →L[ℝ] E b)) (G.D₀ b) (fun i => S.D b (slot i)) G.qstar_ge).choose_spec.2 s j0 hpos t) (norm_nonneg _) S.hM omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.coefficient_nonnegative (b : ξ) (t : ℝ) (x : E b) : 0 ≤ inner ℝ x (G.coefficient slot s j0 b t x) := by simp only [HistoryGeometry.coefficient,smul_apply,inner_smul_right] apply mul_nonneg (G.αnonneg t) apply angular_nonnegative S.r (S.B b) (G.D₀ b) (fun i => S.D b (slot i)) s G.qstar_ge j0 hpos · intro d x;cases d with | none => exact G.D₀nonpos b x | some i => exact S.hD b (slot i) x · intro d x;cases d with | none => exact G.BD₀ b x | some i => exact S.hBD b (slot i) x omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.coefficient_symmetric (b : ξ) (t : ℝ) (x y : E b) : inner ℝ (G.coefficient slot s j0 b t x) y=inner ℝ x (G.coefficient slot s j0 b t y) := by simp only [HistoryGeometry.coefficient,smul_apply,real_inner_smul_left,inner_smul_right] congr 1 apply angular_symmetric S.r (S.B b) (G.D₀ b) (fun i => S.D b (slot i)) s G.qstar_ge j0 hpos intro d x y;cases d with | none => exact G.D₀symm b x y | some i => exact G.Dsymm b (slot i) x y omit hpos [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.coefficient_center (b : ξ) (t : ℝ) (ht : t ≤ 0) (x : E b) : G.coefficient slot s j0 b t x=(G.l b*(G.l b+G.B₀)) • x := by rw [HistoryGeometry.coefficient,angular_initial S.r _ _ _ s (ht.trans (time_pos j0).le), G.αcenter t ht,one_smul,G.B_eq b] rfl omit hpos [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.coefficient_round (b : ξ) {j : ℕ} (hj : j0 ≤ j) (hz : s j=0) (t : ℝ) (ht : t ∈ Icc (time j) (time j+pulse j)) : G.coefficient slot s j0 b t=G.α t • (S.B b • (1:E b →L[ℝ] E b)) := by rw [HistoryGeometry.coefficient,angular_zero_pulse S.r _ _ _ s hj hz ht.1 ht.2] omit hpos [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.coefficient_rest (b : ξ) (j : ℕ) (t : ℝ) (ht : t ∈ Icc (time j+3*pulse j+dwell j) (time (j+1))) : G.coefficient slot s j0 b t=G.α t • (S.B b • (1:E b →L[ℝ] E b)) := by rw [HistoryGeometry.coefficient,angular_rest S.r _ _ _ s ht.1 ht.2] end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open scoped Topology ContDiff InnerProductSpace Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace variable {S : PulseSystem E ι κ} (G : HistoryGeometry S) {n : ℕ} [NeZero n] (slot : Fin n → κ) omit [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in /-- Uniform reset for the explicit smooth angular stream, including the first active period and arbitrary prior admissible control choices. -/ theorem HistoryGeometry.uniform_incoming {ε : ℝ} (hε : 0 < ε) : ∃ J : ℕ,∀ j0 j,J ≤ j → ∀ s : ℕ → Fin n → ℝ, (∀ k,j0 ≤ k → ∀ t i,packetStretch (s k) (pulse k) t i ∈ Icc (1/2:ℝ) (3/2)) → ∀ b,‖orthogonalMatrix (S.basis b) (slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j))- S.θ b • (1:Matrix (ι b) (ι b) ℝ)‖ ≤ ε := by classical have hex (b : ξ) := uniform_round_reset (S.basis b) G.driftContinuous (G.αlimit b) G.driftLimit S.hγ (S.hθ b) G.driftLower (S.hroot b) (G.bound_nonneg slot b) G.Mpnonneg G.driftBound (G.lpos b) G.driftCenter hε choose J hJ using hex refine ⟨Finset.univ.sup J+1,fun j0 j hj s hpos b => ?_⟩ have hji : J b ≤ j-1 := by have hsup := Finset.le_sup (s:=Finset.univ) (f:=J) (Finset.mem_univ b) omega have he : j-1+1=j := by omega have hh := hJ b (j-1) hji (G.coefficient slot s j0 b) (G.coefficient_smooth slot s j0 hpos b).continuous (G.coefficient_bound slot s j0 hpos b) (G.coefficient_symmetric slot s j0 hpos b) (G.coefficient_nonnegative slot s j0 hpos b) (G.coefficient_center slot s j0 b) (G.coefficient_rest slot s j0 b (j-1)) simpa only [he] using hh omit [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.uniform_radial_tail {δ : ℝ} (hδ : 0 < δ) : ∃ J : ℕ,∀ j,J ≤ j → ∀ t,time j ≤ t → (∀ b,|G.α t-S.β b| ≤ δ) ∧ |G.drift t-S.p₀| ≤ δ ∧ S.γ ≤ G.drift t := by have hα : ∀ᶠ t in atTop,∀ b,|G.α t-S.β b| ≤ δ := by apply Filter.eventually_all.2 intro b have hh : Tendsto (fun t => |G.α t-S.β b|) atTop (𝓝 0) := by simpa only [sub_self,abs_zero] using ((G.αlimit b).sub_const (S.β b)).abs exact (hh.eventually (gt_mem_nhds hδ)).mono (fun _ h => h.le) have hp : Tendsto (fun t => |G.drift t-S.p₀|) atTop (𝓝 0) := by simpa only [sub_self,abs_zero] using (G.driftLimit.sub_const S.p₀).abs obtain ⟨a,ha⟩ := eventually_atTop.1 (hα.and ((hp.eventually (gt_mem_nhds hδ)).and G.driftLower)) obtain ⟨J,hJ⟩ := eventually_atTop.1 (time_atTop.eventually_ge_atTop a) exact ⟨J,fun j hj t ht => ⟨(ha t ((hJ j hj).trans ht)).1, (ha t ((hJ j hj).trans ht)).2.1.le,(ha t ((hJ j hj).trans ht)).2.2⟩⟩ omit [Nonempty ξ] [Nonempty κ] [∀ b, Nontrivial (ι b)] in /-- All scalar and incoming thresholds simultaneously, chosen BEFORE the start index, entire control stream, and current history. -/ theorem HistoryGeometry.eventual_history_conditions (T₀ : ℝ) {ρ : ℝ} (hρ : 0 < ρ) : ∃ J : ℕ,∀ j0 j,J ≤ j0 → j0 ≤ j → T₀ ≤ pulse j ∧ ρ/4+(pulse j)⁻¹+ρ/4 ≤ ρ ∧ (∀ t,time j ≤ t → (∀ b,|G.α t-S.β b| ≤ ρ/4) ∧ |G.drift t-S.p₀| ≤ ρ/4 ∧ S.γ ≤ G.drift t) ∧ ∀ s : ℕ → Fin n → ℝ, (∀ k,j0 ≤ k → ∀ t i,packetStretch (s k) (pulse k) t i ∈ Icc (1/2:ℝ) (3/2)) → ∀ b,‖orthogonalMatrix (S.basis b) (slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j))- S.θ b • (1:Matrix (ι b) (ι b) ℝ)‖ ≤ ρ/4 := by have hquarter : 0 < ρ/4 := by linarith obtain ⟨J₁,hJ₁⟩ := G.uniform_incoming slot hquarter obtain ⟨J₂,hJ₂⟩ := G.uniform_radial_tail hquarter have hi : Tendsto (fun j => (pulse j)⁻¹) atTop (𝓝 0) := tendsto_inv_atTop_zero.comp pulse_atTop_limit obtain ⟨J₃,hJ₃⟩ := eventually_atTop.1 ((pulse_atTop_limit.eventually_ge_atTop T₀).and (hi.eventually (gt_mem_nhds (show 0 < ρ/2 by linarith)))) refine ⟨max J₁ (max J₂ J₃),fun j0 j hj0 hj => ?_⟩ have hh := hj0.trans hj have h1 : J₁ ≤ j := (le_max_left _ _).trans hh have h2 : J₂ ≤ j := (le_max_left _ _).trans ((le_max_right _ _).trans hh) have h3 : J₃ ≤ j := (le_max_right _ _).trans ((le_max_right _ _).trans hh) exact ⟨(hJ₃ j h3).1,by linarith [(hJ₃ j h3).2],hJ₂ j h2,hJ₁ j0 j h1⟩ end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set HarmonicCounterexample.FiniteControl HarmonicCounterexample.FiniteControl.SmoothWord open HarmonicCounterexample.FiniteControl.Frobenius HarmonicCounterexample.Transmission open scoped ContDiff InnerProductSpace BigOperators Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace local instance (d : ℕ) : NormedAddCommGroup (EuclideanSpace ℝ (Fin d) →L[ℝ] MatrixProduct ι) := ContinuousLinearMap.toNormedAddCommGroup local instance (d : ℕ) : NormedSpace ℝ (EuclideanSpace ℝ (Fin d) →L[ℝ] MatrixProduct ι) := ContinuousLinearMap.toNormedSpace omit [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma PhysicalWord.ideal_factor (S : PulseSystem E ι κ) (w : PhysicalWord κ) : (fun x b => orthogonalMatrix (S.basis b) (flow (fun t => ContinuousLinearMap.mul ℝ (E b →L[ℝ] E b) (unitPacketCoefficient (fun j => w.amps j x) (fun j => bergerSlowGenerator S.r (S.B b) (S.β b) S.p₀ (S.θ b) 1 (S.D b (w.slot j))) t)) 1 1))=w.ideal S := by funext x b rw [orthogonalMatrix_packet] exact (actual_packet_apply (fun j => w.amps j x) (S.generator ∘ w.slot) b).symm omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma PhysicalWord.value_factor (S : PulseSystem E ι κ) (w : PhysicalWord κ) (H : PulseHistory S) : (fun x b => orthogonalMatrix (S.basis b) (Real.exp (-(∫ t in H.a..H.a+H.T, scalarBaseline (fun s => H.α (H.a+s)*S.B b) (fun s => H.drift (H.a+s)) (S.θ b) (max 0 (t-H.a)))) • (operatorValue (insertWord (H.history b) H.α S.r (S.B b • (1:E b →L[ℝ] E b)) (fun j => S.D b (w.slot j)) (fun j => w.amps j x) H.a H.T) H.drift (H.l b) (H.a+H.T)* Ring.inverse (operatorValue (insertWord (H.history b) H.α S.r (S.B b • (1:E b →L[ℝ] E b)) (fun j => S.D b (w.slot j)) (fun j => w.amps j x) H.a H.T) H.drift (H.l b) H.a)))) = w.value S H := rfl omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma PhysicalWord.defect_factor (S : PulseSystem E ι κ) (w : PhysicalWord κ) (H : PulseHistory S) : (fun x b => orthogonalMatrix (S.basis b) (slope (insertWord (H.history b) H.α S.r (S.B b • (1:E b →L[ℝ] E b)) (fun j => S.D b (w.slot j)) (fun j => w.amps j x) H.a H.T) H.drift (H.l b) (H.a+H.T))-S.θ b • (1:Matrix (ι b) (ι b) ℝ)) = w.defect S H := rfl omit [Nonempty κ] [∀ b,Nontrivial (ι b)] in /-- Packaged uniform estimate with precisely the data that occur in a recursive center-regular geometric construction. -/ theorem word_physical_C1 (S : PulseSystem E ι κ) (w : PhysicalWord κ) : ∃ T₀ ρ C : ℝ,1 ≤ T₀ ∧ 0 < ρ ∧ 1 ≤ C ∧ ∀ H : PulseHistory S,T₀ ≤ H.T → H.δ+H.T⁻¹+H.ε ≤ ρ → ∀ x ∈ w.ball, DifferentiableAt ℝ (w.value S H) x ∧ DifferentiableAt ℝ (w.defect S H) x ∧ max (max ‖w.value S H x-w.ideal S x‖ ‖fderiv ℝ (w.value S H) x-fderiv ℝ (w.ideal S) x‖) (max ‖w.defect S H x‖ ‖fderiv ℝ (w.defect S H) x‖) ≤ C*(H.δ+H.T⁻¹+H.ε) := by classical let : NeZero w.n := ⟨w.n_ne⟩ obtain ⟨threshold,smallness,constant,hthreshold,hsmallness,hconstant,hestimate⟩ := compact_simultaneous_physical_C1 S.basis (EuclideanSpace.basisFun (Fin w.d) ℝ) (isCompact_closedBall _ _) S.r S.p₀ S.γ S.M S.B S.β S.θ (fun block index => S.D block (w.slot index)) (fun block index => S.hD block (w.slot index)) (fun block index => S.hBD block (w.slot index)) S.hM S.hB S.hθ S.hγ S.hden S.hroot w.amps (fun index => fderiv ℝ (w.amps index)) (fun point (_ : point ∈ Metric.closedBall (0:w.Parameter) (w.radius+1)) index => ((w.smooth index).differentiable (by simp) point).hasFDerivAt) (fun index => (w.smooth index).continuous.continuousOn) (fun index => ((w.smooth index).continuous_fderiv (by simp)).continuousOn) refine ⟨threshold,smallness,constant,hthreshold,hsmallness,hconstant,?_⟩ intro H hT hsmall x hx have hlocal := hestimate H.T hT H.history H.α H.drift H.MH H.Mb H.l H.B₀ H.a H.δ H.ε (Metric.ball (0:w.Parameter) (w.radius+1)) Metric.isOpen_ball (convex_ball _ _).isPreconnected Metric.ball_subset_closedBall H.smooth H.αsmooth H.driftContinuous H.MHnonneg H.Mbnonneg H.αbound H.αnonneg H.driftBound H.bound H.nonneg H.round H.lpos H.center H.driftCenter H.apos H.δnonneg H.εnonneg H.αclose H.driftClose H.driftLower hsmall H.incoming have hball : w.ball ⊆ Metric.ball (0:w.Parameter) (w.radius+1) := Metric.closedBall_subset_ball (by linarith) simp only [← w.ideal_factor S,← w.value_factor S H,← w.defect_factor S H] exact hlocal x (hball hx) end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set HarmonicCounterexample.FiniteControl HarmonicCounterexample.FiniteControl.SmoothWord open HarmonicCounterexample.FiniteControl.Frobenius HarmonicCounterexample.Transmission open scoped ContDiff InnerProductSpace BigOperators Matrix.Norms.Frobenius attribute [local instance 100] LieRing.ofAssociativeRing variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace local instance (d : ℕ) : NormedAddCommGroup (EuclideanSpace ℝ (Fin d) →L[ℝ] MatrixProduct ι) := ContinuousLinearMap.toNormedAddCommGroup local instance (d : ℕ) : NormedSpace ℝ (EuclideanSpace ℝ (Fin d) →L[ℝ] MatrixProduct ι) := ContinuousLinearMap.toNormedSpace /-- The uniform local producer: the genuine simultaneous Lie packet admits exact physical whole-period tuning, with all thresholds chosen before histories and BEFORE the bounded complete diagonal-leg normalizers. -/ theorem local_physical_tuning (S : PulseSystem E ι κ) (htrace : ∀ j b,(S.generator j b).trace=0) (hfull : ∀ X : MatrixProduct ι,(∀ b,(X b).trace=0) → X ∈ LieSubalgebra.lieSpan ℝ _ (Set.range S.generator)) (target : ∀ b,Matrix.SpecialLinearGroup (ι b) ℝ) {K₀ : ℝ} (hK₀ : 0 ≤ K₀) : ∃ (w : PhysicalWord κ) (T₀ ρ : ℝ),1 ≤ T₀ ∧ 0 < ρ ∧ ∀ H : PulseHistory S,T₀ ≤ H.T → H.δ+H.T⁻¹+H.ε ≤ ρ → ∀ K : MatrixProduct ι,‖K‖ ≤ K₀ → ∃ x ∈ w.ball,∀ b,∃ c : ℝ,c ∈ Ioo (1/2:ℝ) (3/2) ∧ wholePeriod K (w.defect S H x) (w.value S H x) b= c • ((slProductToUnits target:MatrixProduct ι) b) := by classical obtain ⟨d,n,hn,slot,amps,A,ha,hΦs,hΦ₀,hΦjet⟩ := smooth_SL_packet_submersion S.generator htrace hfull target let Φ := fun x => flow (fun t => ContinuousLinearMap.mul ℝ (MatrixProduct ι) (unitPacketCoefficient (fun j => amps j x) (S.generator ∘ slot) t)) 1 1 have hΦs' : ContDiff ℝ ∞ Φ := hΦs obtain ⟨R,σ,hR,hσ,hatt⟩ := Frobenius.whole_period_uniform_attainment (slProductToUnits target) Φ (fderiv ℝ Φ) A hΦs'.continuous (hΦs'.continuous_fderiv (by simp)) hΦ₀ (by convert! hΦjet using 1) hK₀ let w : PhysicalWord κ := ⟨d,n,hn.out,slot,amps,ha,R,hR⟩ obtain ⟨T₀,ρ,C,hT₀,hρ,hC,hworks⟩ := word_physical_C1 S w have hCpos : 0 < C := lt_of_lt_of_le zero_lt_one hC refine ⟨w,T₀,min ρ (σ/C),hT₀,lt_min hρ (div_pos hσ hCpos),?_⟩ intro H hT hsmall K hK have heσ : C*(H.δ+H.T⁻¹+H.ε) ≤ σ := by have he := (le_div_iff₀ hCpos).1 (hsmall.trans (min_le_right ρ (σ/C))) simpa only [mul_comm] using he have hlocal := hworks H hT (hsmall.trans (min_le_left ρ (σ/C))) apply hatt K (w.defect S H) (w.value S H) (fderiv ℝ (w.defect S H)) (fderiv ℝ (w.value S H)) hK · intro x hx;exact (hlocal x hx).2.1.hasFDerivAt · intro x hx;exact (hlocal x hx).1.hasFDerivAt · intro x hx;exact ((le_max_left _ _).trans ((le_max_right _ _).trans (hlocal x hx).2.2)).trans heσ · intro x hx;exact ((le_max_left _ _).trans ((le_max_left _ _).trans (hlocal x hx).2.2)).trans heσ · intro x hx;exact ((le_max_right _ _).trans ((le_max_right _ _).trans (hlocal x hx).2.2)).trans heσ · intro x hx;exact ((le_max_right _ _).trans ((le_max_left _ _).trans (hlocal x hx).2.2)).trans heσ end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses FiniteControl.SmoothWord open scoped Topology ContDiff BigOperators variable {κ : Type*} (w : PhysicalWord κ) /-- Zero belongs to the admissible control space as a genuinely absent pulse, not as the generally nonzero word at parameter zero. -/ def PhysicalWord.admissible : Set (Fin w.n → ℝ) := {a | a=0 ∨ ∃ x ∈ w.ball,a=(fun i => w.amps i x)} lemma PhysicalWord.zero_admissible : (0:Fin w.n → ℝ) ∈ w.admissible := Or.inl rfl lemma PhysicalWord.amplitudes_admissible {x : w.Parameter} (hx : x ∈ w.ball) : (fun i => w.amps i x) ∈ w.admissible := Or.inr ⟨x,hx,rfl⟩ lemma PhysicalWord.admissible_uniform_bound : ∃ U : ℝ,0 ≤ U ∧ ∀ a ∈ w.admissible,∀ i,|a i| ≤ U := by classical choose C hC using fun i : Fin w.n => (isCompact_closedBall (0:w.Parameter) w.radius).exists_bound_of_continuousOn (f:=w.amps i) ((w.smooth i).continuous.continuousOn : ContinuousOn (w.amps i) w.ball) let U := ∑ i : Fin w.n,max (C i) 0 have hU : 0 ≤ U := Finset.sum_nonneg (fun i _ => le_max_right _ _) refine ⟨U,hU,fun a ha i => ?_⟩ rcases ha with rfl | ⟨x,hx,rfl⟩ · simpa using hU · exact (hC i x hx).trans ((le_max_left _ _).trans (Finset.single_le_sum (fun j _ => le_max_right (C j) 0) (Finset.mem_univ i))) /-- The same compact parameter ball works in every later pulse, with a threshold independent of histories or later parameter choices. -/ theorem PhysicalWord.admissible_stretch_threshold : ∃ J : ℕ,∀ j,J ≤ j → ∀ a ∈ w.admissible,∀ t i,packetStretch a (pulse j) t i ∈ Icc (1/2:ℝ) (3/2) := by obtain ⟨U,hU,hbound⟩ := w.admissible_uniform_bound obtain ⟨C,hC,hpos⟩ := packetStretch_uniform_positive w.n obtain ⟨J,hJ⟩ := eventually_atTop.1 (pulse_atTop_limit.eventually_ge_atTop (2*C*U)) exact ⟨J,fun j hj a ha => hpos a U (pulse j) hU (hbound a ha) (pulse_pos j) (hJ j hj)⟩ end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open HarmonicCounterexample.Transmission HarmonicCounterexample.FiniteControl HarmonicCounterexample.FiniteControl.Frobenius open scoped Topology ContDiff InnerProductSpace Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace variable {S : PulseSystem E ι κ} (G : HistoryGeometry S) {n : ℕ} [NeZero n] (slot : Fin n → κ) def HistoryGeometry.baseline (j : ℕ) (b : ξ) (t : ℝ) : ℝ := scalarBaseline (fun s => G.α (time j+s)*S.B b) (fun s => G.drift (time j+s)) (S.θ b) (max 0 (t-time j)) def HistoryGeometry.packet (s : ℕ → Fin n → ℝ) (j0 j : ℕ) : MatrixProduct ι := fun b => orthogonalMatrix (S.basis b) (Real.exp (-(∫ t in time j..time j+pulse j,G.baseline j b t)) • (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)* Ring.inverse (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j)))) def HistoryGeometry.defect (s : ℕ → Fin n → ℝ) (j0 j : ℕ) : MatrixProduct ι := fun b => orthogonalMatrix (S.basis b) (slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j))- S.θ b • (1:Matrix (ι b) (ι b) ℝ) omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.coefficient_causal {s u : ℕ → Fin n → ℝ} {j0 j : ℕ} (he : ∀ i < j,s i=u i) {t : ℝ} (ht : t ≤ time j) (b : ξ) : G.coefficient slot s j0 b t=G.coefficient slot u j0 b t := by dsimp [HistoryGeometry.coefficient] rw [angular_causal S.r _ _ _ G.qstar j0 he ht] omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.packet_causal {s u : ℕ → Fin n → ℝ} {j0 j : ℕ} (he : ∀ i < j+1,s i=u i) : G.packet slot s j0 j=G.packet slot u j0 j ∧ G.defect slot s j0 j=G.defect slot u j0 j := by have ht1 : time j ∈ Icc 0 (time (j+1)) := ⟨(time_pos j).le,time_strictMono.monotone (by omega)⟩ have ht2 : time j+pulse j ∈ Icc 0 (time (j+1)) := by constructor · linarith [time_pos j,pulse_pos j] · rw [time_succ];linarith [dwell_pos j,pulse_pos j] have hcoeff (b : ξ) : EqOn (G.coefficient slot s j0 b) (G.coefficient slot u j0 b) (Icc 0 (time (j+1))) := fun t ht => G.coefficient_causal slot he ht.2 b constructor · funext b simp only [HistoryGeometry.packet,(operator_history_eq (hcoeff b) G.drift (G.l b) ht1).1, (operator_history_eq (hcoeff b) G.drift (G.l b) ht2).1] · funext b simp only [HistoryGeometry.defect,slope_history_eq (hcoeff b) G.drift (G.l b) ht2] end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open HarmonicCounterexample.Transmission HarmonicCounterexample.FiniteControl open scoped Topology ContDiff InnerProductSpace Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace variable {S : PulseSystem E ι κ} (G : HistoryGeometry S) {n : ℕ} [NeZero n] (slot : Fin n → κ) variable (s : ℕ → Fin n → ℝ) (j0 j : ℕ) (δ ε : ℝ) (hpos : ∀ k,j0 ≤ k → ∀ t i,packetStretch (s k) (pulse k) t i ∈ Icc (1/2:ℝ) (3/2)) (hj : j0 ≤ j) (hz : s j=0) (hδ : 0 ≤ δ) (hε : 0 ≤ ε) (hr : ∀ t,time j ≤ t → (∀ b,|G.α t-S.β b| ≤ δ) ∧ |G.drift t-S.p₀| ≤ δ ∧ S.γ ≤ G.drift t) (hi : ∀ b,‖orthogonalMatrix (S.basis b) (slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j))- S.θ b • (1:Matrix (ι b) (ι b) ℝ)‖ ≤ ε) /-- This is a constructor from the actual stream. All nontrivial input facts are supplied by the single history-independent threshold theorem. -/ def HistoryGeometry.pulseHistory : PulseHistory S where history := G.coefficient slot s j0 α := G.α drift := G.drift MH := G.bound slot Mb := G.Mp l := G.l B₀ := G.B₀ a := time j T := pulse j δ := δ ε := ε smooth := G.coefficient_smooth slot s j0 hpos αsmooth := G.αsmooth driftContinuous := G.driftContinuous MHnonneg := G.bound_nonneg slot Mbnonneg := G.Mpnonneg αbound := G.αbound αnonneg := G.αnonneg driftBound := G.driftBound bound := G.coefficient_bound slot s j0 hpos nonneg := G.coefficient_nonnegative slot s j0 hpos round := fun b t ht => G.coefficient_round slot s j0 b hj hz t ht lpos := G.lpos center := G.coefficient_center slot s j0 driftCenter := G.driftCenter apos := (time_pos j).le δnonneg := hδ εnonneg := hε αclose := fun b t ht => (hr t ht.1).1 b driftClose := fun t ht => (hr t ht.1).2.1 driftLower := fun t ht => (hr t ht.1).2.2 incoming := hi end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open HarmonicCounterexample.Transmission HarmonicCounterexample.FiniteControl open scoped Topology ContDiff InnerProductSpace Matrix.Norms.Frobenius attribute [local instance 100] LieRing.ofAssociativeRing variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace /-- One smooth infinite stream simultaneously tunes every whole-period packet. All thresholds precede EVERY history. The bounded normalizers may be any predetermined actual complete diagonal legs; they do not supply transmissions. -/ theorem global_physical_tuning (S : PulseSystem E ι κ) (G : HistoryGeometry S) (htrace : ∀ j b,(S.generator j b).trace=0) (hfull : ∀ X : MatrixProduct ι,(∀ b,(X b).trace=0) → X ∈ LieSubalgebra.lieSpan ℝ _ (Set.range S.generator)) (target : ∀ b,Matrix.SpecialLinearGroup (ι b) ℝ) {K₀ : ℝ} (hK₀ : 0 ≤ K₀) : ∃ w : PhysicalWord κ,∃ J : ℕ,∀ j0,J ≤ j0 → ∀ K : ℕ → MatrixProduct ι,(∀ j,j0 ≤ j → ‖K j‖ ≤ K₀) → ∃ s : ℕ → Fin w.n → ℝ, (∀ j,s j ∈ w.admissible) ∧ (∀ j,j ?_⟩ have hj1 : J₁ ≤ j0 := (le_max_left _ _).trans hj0 have hj2 : J₂ ≤ j0 := (le_max_right _ _).trans hj0 let good (j : ℕ) (s : ℕ → Fin w.n → ℝ) (a : Fin w.n → ℝ) : Prop := (j hJ₂ k (hj2.trans hk) (s k) (hsall k) obtain ⟨hT,hsmall,hr,hin⟩ := hJ₁ j0 j hj1 hj have hquarter : 0 ≤ ρ/4 := by linarith let H := G.pulseHistory w.slot s j0 j (ρ/4) (ρ/4) hpos hj (hz j le_rfl) hquarter hquarter hr (hin s hpos) obtain ⟨x,hx,hxTune⟩ := htune H hT hsmall (K j) (hK j hj) let a : Fin w.n → ℝ := fun i => w.amps i x have hc (b : ξ) : w.coefficient S H b x=G.coefficient w.slot (Function.update s j a) j0 b := by change insertWord (G.coefficient w.slot s j0 b) G.α S.r (S.B b • (1:E b →L[ℝ] E b)) (fun i => S.D b (w.slot i)) a (time j) (pulse j)=_ exact (coefficient_update S.r _ (G.D₀ b) _ s a G.qstar G.α hj (hz j le_rfl)).symm have hv : w.value S H x=G.packet w.slot (Function.update s j a) j0 j := by funext b unfold PhysicalWord.value HistoryGeometry.packet rw [hc b] rfl have hd : w.defect S H x=G.defect w.slot (Function.update s j a) j0 j := by funext b unfold PhysicalWord.defect HistoryGeometry.defect rw [hc b] rfl refine ⟨a,w.amplitudes_admissible hx,?_,?_⟩ · intro h;omega · intro _ rw [←hv,←hd] exact hxTune · refine ⟨0,w.zero_admissible,fun _ => rfl,?_⟩ intro h;exact (hj h).elim obtain ⟨s,hs,hgood⟩ := CausalConstruction.causal_choice 0 w.admissible good produce refine ⟨s,hs,fun j hj => (hgood j).1 hj,?_,?_⟩ · intro j hj exact hJ₂ j (hj2.trans hj) (s j) (hs j) · intro j hj have ht := (hgood j).2 hj have he : ∀ i < j+1,s i=Function.update (fun k => if k (D b:Matrix (ι b) (ι b) ℝ)*X) hf rw [← mul_assoc,Units.mul_inv,one_mul,he,Matrix.mul_smul] at hh exact hh variable {R : Type*} [NormedRing R] [NormedAlgebra ℝ R] /-- Undo ONLY the harmless scalar pulse normalization. The scalar logarithmic cost is separated from the genuine diagonal factor of the entire leg. -/ lemma unnormalize_whole_leg {Fa Fc Fd U V P D M : R} {I c : ℝ} (hvalue : Fd=(U+V*P)*Fc) (htune : (U+V*P)*(Real.exp (-I) • (Fc*Fa))=c • (D*M)) : Fd*Fa=(Real.exp I*c) • (D*M) := by have he := congrArg (fun X : R => Real.exp I • X) htune rw [mul_smul_comm,smul_smul,← Real.exp_add,add_neg_cancel,Real.exp_zero,one_smul] at he rw [hvalue,mul_assoc] simpa only [smul_smul] using he end HarmonicCounterexample.Transmission end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open HarmonicCounterexample.Transmission HarmonicCounterexample.FiniteControl open scoped Topology ContDiff InnerProductSpace BigOperators Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace local instance (b : ξ) : NormedAddCommGroup ((E b →L[ℝ] E b) →L[ℝ] Matrix (ι b) (ι b) ℝ) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ ((E b →L[ℝ] E b) →L[ℝ] Matrix (ι b) (ι b) ℝ) := ContinuousLinearMap.toNormedSpace local instance (b : ξ) : NormedAddCommGroup (Matrix (ι b) (ι b) ℝ →L[ℝ] ℝ) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (Matrix (ι b) (ι b) ℝ →L[ℝ] ℝ) := ContinuousLinearMap.toNormedSpace local instance (b : ξ) : NormedAddCommGroup ((ι b → ℝ) →L[ℝ] Matrix (ι b) (ι b) ℝ) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ ((ι b → ℝ) →L[ℝ] Matrix (ι b) (ι b) ℝ) := ContinuousLinearMap.toNormedSpace variable {S : PulseSystem E ι κ} (G : HistoryGeometry S) {n : ℕ} [NeZero n] omit [NeZero n] in lemma zero_stretch (j : ℕ) (t : ℝ) (i : Fin n) : packetStretch (0:Fin n → ℝ) (pulse j) t i ∈ Icc (1/2:ℝ) (3/2) := by norm_num [packetStretch] /-- Background diagonal coefficient, independent of all control choices. -/ def HistoryGeometry.baseCoefficient (j0 : ℕ) (b : ξ) (t : ℝ) : E b →L[ℝ] E b := G.α t • PulseTaylor.angular S.r (S.B b • (1:E b →L[ℝ] E b)) (G.D₀ b) (base G.qstar j0 t) omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] [NeZero n] in lemma HistoryGeometry.baseCoefficient_eq (slot : Fin n → κ) (j0 : ℕ) (b : ξ) : G.baseCoefficient j0 b=G.coefficient slot 0 j0 b := by funext t unfold HistoryGeometry.baseCoefficient HistoryGeometry.coefficient angular have he : (fun j => activeIncrement S.r (S.B b • (1:E b →L[ℝ] E b)) (fun i => S.D b (slot i)) 0 j0 j t)=fun _ => (0:E b →L[ℝ] E b) := by funext j dsimp [activeIncrement] split_ifs · exact increment_zero S.r _ _ rfl t · rfl rw [he,tsum_zero,add_zero] omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.baseCoefficient_diagonal (d₀ : ∀ b,ι b → ℝ) (hd₀ : ∀ b,orthogonalMatrix (S.basis b) (G.D₀ b)=Matrix.diagonal (d₀ b)) (j0 : ℕ) (b : ξ) (t : ℝ) : orthogonalMatrix (S.basis b) (G.baseCoefficient j0 b t)=Matrix.diagonal (fun i => G.α t*((base G.qstar j0 t)^S.r*S.B b+ ((base G.qstar j0 t)^S.r-(base G.qstar j0 t)^(S.r-1))*d₀ b i)) := by simp only [HistoryGeometry.baseCoefficient,PulseTaylor.angular,map_smul,map_add, orthogonalMatrix_one,hd₀] ext i j by_cases h : i=j · subst j;simp [Matrix.diagonal_apply_eq,smul_eq_mul] · simp [h,smul_eq_mul] /-- The genuine fixed diagonal scalar coefficient. -/ def HistoryGeometry.legLambda (d₀ : ∀ b,ι b → ℝ) (j0 : ℕ) (b : ξ) (i : ι b) (t : ℝ) : ℝ := G.α t*((base G.qstar j0 t)^S.r*S.B b+ ((base G.qstar j0 t)^S.r-(base G.qstar j0 t)^(S.r-1))*d₀ b i) omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b,Nontrivial (ι b)] in lemma HistoryGeometry.legLambda_properties (slot : Fin n → κ) (d₀ : ∀ b,ι b → ℝ) (hd₀ : ∀ b,orthogonalMatrix (S.basis b) (G.D₀ b)=Matrix.diagonal (d₀ b)) (j0 : ℕ) (b : ξ) : ∃ N : ι b → ℝ,(∀ i,0 ≤ N i) ∧ (∀ i,Continuous (G.legLambda d₀ j0 b i)) ∧ (∀ i t,|G.legLambda d₀ j0 b i t| ≤ N i) ∧ (∀ i t,0 ≤ G.legLambda d₀ j0 b i t) := by have hp : ∀ j,j0 ≤ j → ∀ t i,packetStretch ((0:ℕ → Fin n → ℝ) j) (pulse j) t i ∈ Icc (1/2:ℝ) (3/2) := fun j _ t i => zero_stretch j t i have hbc := G.baseCoefficient_eq slot j0 b have hc : Continuous (G.baseCoefficient j0 b) := by rw [hbc];exact (G.coefficient_smooth slot 0 j0 hp b).continuous have he (i : ι b) (t : ℝ) : G.legLambda d₀ j0 b i t= matrixEntry i i (orthogonalMatrix (S.basis b) (G.baseCoefficient j0 b t)) := by rw [matrixEntry_apply,G.baseCoefficient_diagonal d₀ hd₀,Matrix.diagonal_apply_eq] rfl let N : ι b → ℝ := fun i => ‖matrixEntry i i‖*‖orthogonalMatrix (S.basis b)‖*G.bound slot b refine ⟨N,fun i => mul_nonneg (mul_nonneg (norm_nonneg _) (norm_nonneg _)) (G.bound_nonneg slot b),?_,?_,?_⟩ · intro i have hf : G.legLambda d₀ j0 b i=fun t => matrixEntry i i (orthogonalMatrix (S.basis b) (G.baseCoefficient j0 b t)) := funext (he i) rw [hf];exact (matrixEntry i i).continuous.comp ((orthogonalMatrix (S.basis b)).continuous.comp hc) · intro i t rw [he i t,← Real.norm_eq_abs] calc _ ≤ ‖matrixEntry i i‖*‖orthogonalMatrix (S.basis b) (G.baseCoefficient j0 b t)‖ := (matrixEntry i i).le_opNorm _ _ ≤ ‖matrixEntry i i‖*(‖orthogonalMatrix (S.basis b)‖*‖G.baseCoefficient j0 b t‖) := mul_le_mul_of_nonneg_left ((orthogonalMatrix (S.basis b)).le_opNorm _) (norm_nonneg _) _ ≤ N i := by dsimp [N];rw [mul_assoc,hbc] exact mul_le_mul_of_nonneg_left (mul_le_mul_of_nonneg_left (G.coefficient_bound slot 0 j0 hp b t) (norm_nonneg _)) (norm_nonneg _) · intro i t rw [he i t,matrixEntry_apply,orthogonalMatrix_apply,OrthonormalBasis.repr_apply_apply,hbc] exact G.coefficient_nonnegative slot 0 j0 hp b t (S.basis b i) /-- ACTUAL complete-leg columns with the physical schedule. -/ def HistoryGeometry.legU (d₀ : ∀ b,ι b → ℝ) (j0 j : ℕ) (b : ξ) : Matrix (ι b) (ι b) ℝ := Matrix.diagonal (fun i => scalarU (fun t => G.legLambda d₀ j0 b i (time j+pulse j+t)) (fun t => G.drift (time j+pulse j+t)) (time (j+1)-(time j+pulse j))) def HistoryGeometry.legV (d₀ : ∀ b,ι b → ℝ) (j0 j : ℕ) (b : ξ) : Matrix (ι b) (ι b) ℝ := Matrix.diagonal (fun i => scalarV (fun t => G.legLambda d₀ j0 b i (time j+pulse j+t)) (fun t => G.drift (time j+pulse j+t)) (time (j+1)-(time j+pulse j))) omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b, Nontrivial (ι b)] in lemma HistoryGeometry.leg_normalizer (slot : Fin n → κ) (d₀ : ∀ b,ι b → ℝ) (hd₀ : ∀ b,orthogonalMatrix (S.basis b) (G.D₀ b)=Matrix.diagonal (d₀ b)) (j0 j : ℕ) (b : ξ) : ∃ D : (Matrix (ι b) (ι b) ℝ)ˣ, (D:Matrix (ι b) (ι b) ℝ)=G.legU d₀ j0 j b+S.θ b • G.legV d₀ j0 j b ∧ (∀ i,0 < (D:Matrix (ι b) (ι b) ℝ) i i) ∧ ‖(↑D⁻¹:Matrix (ι b) (ι b) ℝ)*G.legV d₀ j0 j b‖ ≤ ‖diagonalL (ι:=ι b)‖*(S.θ b)⁻¹ := by obtain ⟨N,hN,hc,hb,hp⟩ := G.legLambda_properties slot d₀ hd₀ j0 b apply actual_diagonal_normalizer (fun i => (hc i).comp (continuous_const.add continuous_id)) (G.driftContinuous.comp (continuous_const.add continuous_id)) N hN G.Mpnonneg (fun i t => hb i _) (fun t => G.driftBound _) (fun i t _ => hp i _) ?_ (S.hθ b) rw [time_succ];linarith [pulse_pos j,dwell_pos j] end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open HarmonicCounterexample.Transmission HarmonicCounterexample.FiniteControl open scoped Topology ContDiff InnerProductSpace BigOperators Matrix.Norms.Frobenius variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ (E b →L[ℝ] E b) := ContinuousLinearMap.toNormedSpace variable {S : PulseSystem E ι κ} (G : HistoryGeometry S) {n : ℕ} [NeZero n] (slot : Fin n → κ) /-- Actual center-regular value transmission, including the complete diagonal leg and with no pulse scalar normalization. -/ def HistoryGeometry.transmission (s : ℕ → Fin n → ℝ) (j0 j : ℕ) (b : ξ) : Matrix (ι b) (ι b) ℝ := orthogonalMatrix (S.basis b) (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time (j+1))* Ring.inverse (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j))) omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b, Nontrivial (ι b)] in lemma HistoryGeometry.actual_leg_restart (d₀ : ∀ b,ι b → ℝ) (hd₀ : ∀ b,orthogonalMatrix (S.basis b) (G.D₀ b)=Matrix.diagonal (d₀ b)) (s : ℕ → Fin n → ℝ) (j0 j : ℕ) (hpos : ∀ k,j0 ≤ k → ∀ t i,packetStretch (s k) (pulse k) t i ∈ Icc (1/2:ℝ) (3/2)) (hj : j0 ≤ j) (b : ξ) : orthogonalMatrix (S.basis b) (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time (j+1)))= (G.legU d₀ j0 j b+G.legV d₀ j0 j b* orthogonalMatrix (S.basis b) (slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)))* orthogonalMatrix (S.basis b) (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)) := by obtain ⟨N,hN,hc,hb,hp⟩ := G.legLambda_properties slot d₀ hd₀ j0 b have hA := (G.coefficient_smooth slot s j0 hpos b).continuous have hbound := G.coefficient_bound slot s j0 hpos b have hnonneg := G.coefficient_nonnegative slot s j0 hpos b have hdiag (t : ℝ) (ht : t ∈ Ico (time j+pulse j) (time (j+1))) : orthogonalMatrix (S.basis b) (G.coefficient slot s j0 b t)= Matrix.diagonal (fun i => G.legLambda d₀ j0 b i t) := by change orthogonalMatrix (S.basis b) (G.α t • angular _ _ _ _ _ _ _ _)=_ rw [angular_leg _ _ _ _ _ hj ht.1 ht.2.le] exact G.baseCoefficient_diagonal d₀ hd₀ j0 b t have he := actual_diagonal_restart (S.basis b) N (G.l b) hA G.driftContinuous hc (G.bound_nonneg slot b) G.Mpnonneg hN hbound G.driftBound hb hdiag (time (j+1)) ⟨by rw [time_succ];linarith [pulse_pos j,dwell_pos j],le_rfl⟩ change _=G.legU d₀ j0 j b*_ +G.legV d₀ j0 j b*orthogonalMatrix (S.basis b) (operatorVelocity (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)) at he have hu := operatorValue_isUnit hA G.driftContinuous (G.bound_nonneg slot b) G.Mpnonneg hbound G.driftBound hnonneg (G.lpos b) (t:=time j+pulse j) (by linarith [time_pos j,pulse_pos j]) have hs : operatorVelocity (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)= slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)* operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j) := by ext x;exact (slope_value hu x).symm rw [hs,orthogonalMatrix_mul,← mul_assoc,← add_mul] at he exact he omit [Fintype ξ] [Nonempty ξ] [Nonempty κ] [∀ b, Nontrivial (ι b)] in /-- Attainment in normalized pulse coordinates gives the actual WHOLE period, with its scalar exactly separated. -/ theorem HistoryGeometry.exact_period (d₀ : ∀ b,ι b → ℝ) (hd₀ : ∀ b,orthogonalMatrix (S.basis b) (G.D₀ b)=Matrix.diagonal (d₀ b)) (s : ℕ → Fin n → ℝ) (j0 j : ℕ) (hpos : ∀ k,j0 ≤ k → ∀ t i,packetStretch (s k) (pulse k) t i ∈ Icc (1/2:ℝ) (3/2)) (hj : j0 ≤ j) (b : ξ) (D : (Matrix (ι b) (ι b) ℝ)ˣ) (hD : (D:Matrix (ι b) (ι b) ℝ)=G.legU d₀ j0 j b+S.θ b • G.legV d₀ j0 j b) (M : Matrix (ι b) (ι b) ℝ) {c : ℝ} (htune : wholePeriod ((↑D⁻¹:Matrix (ι b) (ι b) ℝ)*G.legV d₀ j0 j b) (G.defect slot s j0 j b) (G.packet slot s j0 j b)=c • M) : G.transmission slot s j0 j b= (Real.exp (∫ t in time j..time j+pulse j,G.baseline j b t)*c) • ((D:Matrix (ι b) (ι b) ℝ)*M) := by let P := orthogonalMatrix (S.basis b) (slope (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j)) have hf := full_leg_factor (G.legU d₀ j0 j b) (G.legV d₀ j0 j b) P (G.packet slot s j0 j b) (S.θ b) D hD have he := congrArg (fun X => (D:Matrix (ι b) (ι b) ℝ)*X) hf rw [←mul_assoc,Units.mul_inv,one_mul] at he change (G.legU d₀ j0 j b+G.legV d₀ j0 j b*P)*G.packet slot s j0 j b= (D:Matrix (ι b) (ι b) ℝ)*wholePeriod _ (G.defect slot s j0 j b) (G.packet slot s j0 j b) at he rw [htune,Matrix.mul_smul] at he have hv := G.actual_leg_restart slot d₀ hd₀ s j0 j hpos hj b have hp : G.packet slot s j0 j b= Real.exp (-(∫ t in time j..time j+pulse j,G.baseline j b t)) • (orthogonalMatrix (S.basis b) (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j+pulse j))* orthogonalMatrix (S.basis b) (Ring.inverse (operatorValue (G.coefficient slot s j0 b) G.drift (G.l b) (time j)))) := by simp only [HistoryGeometry.packet,map_smul,orthogonalMatrix_mul] rw [hp] at he have hu := unnormalize_whole_leg hv he simpa only [HistoryGeometry.transmission,orthogonalMatrix_mul] using hu end HarmonicCounterexample.LinearODE end noncomputable section namespace HarmonicCounterexample.LinearODE open Set Filter Schedule Pulses AngularStream FiniteControl.SmoothWord open HarmonicCounterexample.Transmission HarmonicCounterexample.FiniteControl open scoped Topology ContDiff InnerProductSpace BigOperators Matrix.Norms.Frobenius attribute [local instance 100] LieRing.ofAssociativeRing variable {ξ κ : Type*} [Fintype ξ] [Nonempty ξ] [Nonempty κ] {E : ξ → Type*} {ι : ξ → Type*} [∀ b,NormedAddCommGroup (E b)] [∀ b,InnerProductSpace ℝ (E b)] [∀ b,FiniteDimensional ℝ (E b)] [∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)] [∀ b,Nontrivial (ι b)] local instance (b : ξ) : NormedAddCommGroup ((ι b → ℝ) →L[ℝ] Matrix (ι b) (ι b) ℝ) := ContinuousLinearMap.toNormedAddCommGroup local instance (b : ξ) : NormedSpace ℝ ((ι b → ℝ) →L[ℝ] Matrix (ι b) (ι b) ℝ) := ContinuousLinearMap.toNormedSpace /-- One actual infinite center-regular equation realizes ALL the requested complete-period transmissions. Its normalizers are the true second-order post-pulse columns U,V, not supplied targets or asymptotic substitutes. -/ theorem global_actual_transmission (S : PulseSystem E ι κ) (G : HistoryGeometry S) (d₀ : ∀ b,ι b → ℝ) (hd₀ : ∀ b,orthogonalMatrix (S.basis b) (G.D₀ b)=Matrix.diagonal (d₀ b)) (htrace : ∀ j b,(S.generator j b).trace=0) (hfull : ∀ X : MatrixProduct ι,(∀ b,(X b).trace=0) → X ∈ LieSubalgebra.lieSpan ℝ _ (Set.range S.generator)) (target : ∀ b,Matrix.SpecialLinearGroup (ι b) ℝ) : ∃ w : PhysicalWord κ,∃ J : ℕ,∀ j0,J ≤ j0 → ∃ s : ℕ → Fin w.n → ℝ, (∀ j,s j ∈ w.admissible) ∧ (∀ j,j mul_nonneg (norm_nonneg _) (inv_nonneg.2 (S.hθ b).le)) obtain ⟨w,J,htune⟩ := global_physical_tuning S G htrace hfull target hK₀ let : NeZero w.n := ⟨w.n_ne⟩ refine ⟨w,J,fun j0 hj0 => ?_⟩ let D (j : ℕ) (b : ξ) := (G.leg_normalizer w.slot d₀ hd₀ j0 j b).choose have hD (j : ℕ) (b : ξ) := (G.leg_normalizer w.slot d₀ hd₀ j0 j b).choose_spec let K (j : ℕ) : MatrixProduct ι := fun b => (↑(D j b)⁻¹:Matrix (ι b) (ι b) ℝ)*G.legV d₀ j0 j b have hK (j : ℕ) (_ : j0 ≤ j) : ‖K j‖ ≤ K₀ := by apply (pi_norm_le_iff_of_nonneg hK₀).2 intro b exact (hD j b).2.2.trans (Finset.single_le_sum (fun c _ => mul_nonneg (norm_nonneg (diagonalL (ι:=ι c))) (inv_nonneg.2 (S.hθ c).le)) (Finset.mem_univ b)) obtain ⟨s,hs,hzero,hpos,he⟩ := htune j0 hj0 K hK refine ⟨s,hs,hzero,hpos,fun j hj b => ?_⟩ obtain ⟨c,hc,ht⟩ := he j hj b refine ⟨D j b,(hD j b).1,(hD j b).2.1,c,hc,?_⟩ apply G.exact_period w.slot d₀ hd₀ s j0 j hpos hj b (D j b) (hD j b).1 _ ht end HarmonicCounterexample.LinearODE end end OAI