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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<j0 → s j=0) ∧
(∀ j,j0 ≤ j → ∀ t i,packetStretch (s j) (pulse j) t i ∈ Icc (1/2:ℝ) (3/2)) ∧
∀ j,j0 ≤ j → ∀ b,∃ c : ℝ,c ∈ Ioo (1/2:ℝ) (3/2) ∧
wholePeriod (K j) (G.defect w.slot s j0 j) (G.packet w.slot s j0 j) b=
c • ((slProductToUnits target:MatrixProduct ι) b) := by
classical
obtain ⟨w,T₀,ρ,hT₀,hρ,htune⟩ := local_physical_tuning S htrace hfull target hK₀
let : NeZero w.n := ⟨w.n_ne⟩
obtain ⟨J₁,hJ₁⟩ := G.eventual_history_conditions w.slot T₀ hρ
obtain ⟨J₂,hJ₂⟩ := w.admissible_stretch_threshold
refine ⟨w,max J₁ J₂,fun j0 hj0 K hK => ?_⟩
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<j0 → a=0) ∧ (j0 ≤ j → ∀ b,∃ c : ℝ,c ∈ Ioo (1/2:ℝ) (3/2) ∧
wholePeriod (K j) (G.defect w.slot (Function.update s j a) j0 j)
(G.packet w.slot (Function.update s j a) j0 j) b=
c • ((slProductToUnits target:MatrixProduct ι) b))
have produce : ∀ j s,(∀ i < j,s i ∈ w.admissible) → (∀ i,j ≤ i → s i=0) →
∃ a ∈ w.admissible,good j s a := by
intro j s hs hz
by_cases hj : j0 ≤ j
· have hsall (i : ℕ) : s i ∈ w.admissible := by
by_cases hi : i<j
· exact hs i hi
· rw [hz i (by omega)];exact w.zero_admissible
have hpos : ∀ k,j0 ≤ k → ∀ t i,packetStretch (s k) (pulse k) t i ∈ Icc (1/2:ℝ) (3/2) :=
fun k hk => 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<j then s k else 0) j (s j) i := by
intro i hi
by_cases hij : i=j
· subst i;simp
· rw [Function.update_of_ne hij,ite_eq_left (by omega)]
obtain ⟨hv,hd⟩ := G.packet_causal w.slot (j0:=j0) he
rw [←hv,←hd] at ht
exact ht
end HarmonicCounterexample.LinearODE
end
noncomputable section
namespace HarmonicCounterexample.Transmission
open Set
open scoped Matrix.Norms.Frobenius
variable {β : Type*} [Fintype β] {ι : β → Type*}
[∀ b,Fintype (ι b)] [∀ b,DecidableEq (ι b)]
omit [Fintype β] in
/-- Block-dependent Riccati roots are kept in the complete-leg identity. -/
lemma blockwise_whole_period_exact_leg
{U V P B : ∀ b,Matrix (ι b) (ι b) ℝ} (θ : β → ℝ)
(D M : ∀ b,(Matrix (ι b) (ι b) ℝ)ˣ)
(hD : ∀ b,(D b:Matrix (ι b) (ι b) ℝ)=U b+θ b • V b)
(hatt : ∀ b,∃ c : ℝ,c ∈ Ioo (1/2:ℝ) (3/2) ∧
wholePeriod ((↑(D b)⁻¹:Matrix (ι b) (ι b) ℝ)*V b) (P b-θ b • 1) (B b)=
c • (M b:Matrix (ι b) (ι b) ℝ)) :
∀ b,∃ c : ℝ,c ∈ Ioo (1/2:ℝ) (3/2) ∧
(U b+V b*P b)*B b=c • ((D b:Matrix (ι b) (ι b) ℝ)*(M b:Matrix (ι b) (ι b) ℝ)) := by
intro b
obtain ⟨c,hc,he⟩ := hatt b
refine ⟨c,hc,?_⟩
have hf := full_leg_factor (U b) (V b) (P b) (B b) (θ b) (D b) (hD b)
change (↑(D b)⁻¹:Matrix (ι b) (ι b) ℝ)*((U b+V b*P b)*B b)=
wholePeriod ((↑(D b)⁻¹:Matrix (ι b) (ι b) ℝ)*V b) (P b-θ b • 1) (B b) at hf
have hh := congrArg (fun X => (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<j0 → s j=0) ∧
(∀ j,j0 ≤ j → ∀ t i,packetStretch (s j) (pulse j) t i ∈ Icc (1/2:ℝ) (3/2)) ∧
∀ j,j0 ≤ j → ∀ b,∃ 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) ∧
∃ c : ℝ,c ∈ Ioo (1/2:ℝ) (3/2) ∧
G.transmission w.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)*((target b):Matrix (ι b) (ι b) ℝ)) := by
classical
let K₀ : ℝ := ∑ b : ξ,‖diagonalL (ι:=ι b)‖*(S.θ b)⁻¹
have hK₀ : 0 ≤ K₀ := Finset.sum_nonneg (fun b _ => 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