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import OAI.Analysis.CoulombIonization.FormDomain.CoerciveOperator
namespace OAI
noncomputable section
open MeasureTheory Filter
open scoped Topology BigOperators ContDiff
open MeasureTheory Filter
open scoped Topology BigOperators ContDiff InnerProductSpace Convolution
namespace CoulombAtom
variable {V H : Type*} [NormedAddCommGroup V] [InnerProductSpace ℂ V] [CompleteSpace V]
[NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
def formLift (j : V →L[ℂ] H) (A : V →L[ℂ] V) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) : H →L[ℂ] V :=
(coerciveEquiv A hc hA).symm.toContinuousLinearMap.comp j.adjoint
lemma formLift_eq (j : V →L[ℂ] H) (A : V →L[ℂ] V) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (y : H) :
A (formLift j A hc hA y) = j.adjoint y :=
(coerciveEquiv A hc hA).apply_symm_apply _
lemma formLift_inner (j : V →L[ℂ] H) (A : V →L[ℂ] V) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (u : V) (y : H) :
⟪u, A (formLift j A hc hA y)⟫_ℂ = ⟪j u, y⟫_ℂ := by
rw [formLift_eq, j.adjoint_inner_right]
lemma formResolvent_apply (j : V →L[ℂ] H) (A : V →L[ℂ] V) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (y : H) :
formResolvent j A hc hA y = j (formLift j A hc hA y) := rfl
lemma formLift_self (j : V →L[ℂ] H) (A : V →L[ℂ] V) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (y : H) :
⟪formLift j A hc hA y, A (formLift j A hc hA y)⟫_ℂ =
⟪formResolvent j A hc hA y, y⟫_ℂ := formLift_inner j A hc hA _ y
lemma formResolvent_positive (j : V →L[ℂ] H) (A : V →L[ℂ] V)
(hs : IsSelfAdjoint A) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) :
(formResolvent j A hc hA).IsPositive := by
apply ContinuousLinearMap.isPositive_def'.mpr
refine ⟨formResolvent_selfAdjoint j A hs hc hA, fun y => ?_⟩
change 0 ≤ (⟪formResolvent j A hc hA y, y⟫_ℂ).re
rw [← formLift_self]
exact (mul_nonneg hc.le (sq_nonneg _)).trans (hA _)
omit [CompleteSpace V] in
lemma coercive_nonneg (A : V →L[ℂ] V) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (u : V) :
0 ≤ (⟪u, A u⟫_ℂ).re := (mul_nonneg hc.le (sq_nonneg _)).trans (hA u)
lemma hermitian_quadratic_sub (A : V →L[ℂ] V) (hs : IsSelfAdjoint A) (u v : V) :
(⟪u - v, A (u - v)⟫_ℂ).re =
(⟪u, A u⟫_ℂ).re - 2 * (⟪u, A v⟫_ℂ).re + (⟪v, A v⟫_ℂ).re := by
have he : (⟪v, A u⟫_ℂ).re = (⟪u, A v⟫_ℂ).re := by
have hh : ⟪A u, v⟫_ℂ = ⟪u, A v⟫_ℂ :=
(ContinuousLinearMap.isSelfAdjoint_iff_isSymmetric.mp hs) u v
rw [← hh]
exact inner_re_symm (𝕜 := ℂ) v (A u)
rw [map_sub, inner_sub_left, inner_sub_right, inner_sub_right]
simp only [Complex.sub_re]
rw [he]
ring
omit [CompleteSpace H] in
lemma bounded_quadratic_upper (R : H →L[ℂ] H) (y : H) :
(⟪R y, y⟫_ℂ).re ≤ ‖R‖ * ‖y‖ ^ 2 := by
calc
_ ≤ ‖R y‖ * ‖y‖ := by simpa only [RCLike.re_eq_complex_re] using re_inner_le_norm (𝕜 := ℂ) (R y) y
_ ≤ (‖R‖ * ‖y‖) * ‖y‖ := mul_le_mul_of_nonneg_right (R.le_opNorm y) (norm_nonneg _)
_ = _ := by ring
omit [CompleteSpace H] in
lemma injective_norm_pos [Nontrivial H] (R : H →L[ℂ] H) (hinj : Function.Injective R) :
0 < ‖R‖ := by
apply norm_pos_iff.mpr
intro hz
obtain ⟨x, hx⟩ := exists_ne (0 : H)
apply hx
apply hinj
simp [hz]
lemma form_reciprocal_resolvent_bound [Nontrivial H] (j : V →L[ℂ] H)
(hj : Function.Injective j) (hd : DenseRange j) (A : V →L[ℂ] V)
(hs : IsSelfAdjoint A) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (u : V) :
‖formResolvent j A hc hA‖⁻¹ * ‖j u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re := by
let R := formResolvent j A hc hA
have hR : 0 < ‖R‖ := injective_norm_pos R (formResolvent_injective j hj hd A hc hA)
let y : H := (‖R‖⁻¹ : ℂ) • j u
let v := formLift j A hc hA y
have hp := coercive_nonneg A hc hA (u - v)
rw [hermitian_quadratic_sub A hs] at hp
have hv : ⟪v, A v⟫_ℂ = ⟪R y, y⟫_ℂ := formLift_self j A hc hA y
have huv : (⟪u, A v⟫_ℂ).re = ‖R‖⁻¹ * ‖j u‖ ^ 2 := by
rw [formLift_inner]
simp [y, norm_sq_eq_re_inner (𝕜 := ℂ)]
have hny : ‖y‖ ^ 2 = ‖R‖⁻¹ ^ 2 * ‖j u‖ ^ 2 := by
simp [y, norm_smul, mul_pow]
have hq := bounded_quadratic_upper R y
rw [hny] at hq
rw [hv, huv] at hp
have hn : ‖R‖ * (‖R‖⁻¹ ^ 2 * ‖j u‖ ^ 2) = ‖R‖⁻¹ * ‖j u‖ ^ 2 := by
field_simp
rw [hn] at hq
change ‖R‖⁻¹ * ‖j u‖ ^ 2 ≤ _
linarith
lemma resolvent_norm_le_of_form_bound (j : V →L[ℂ] H) (A : V →L[ℂ] V)
{c : ℝ} (hc : 0 < c) (hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re)
{b : ℝ} (hb : 0 < b) (hbound : ∀ u, b * ‖j u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) :
‖formResolvent j A hc hA‖ ≤ b⁻¹ := by
let R := formResolvent j A hc hA
apply ContinuousLinearMap.opNorm_le_bound _ (inv_nonneg.mpr hb.le)
intro y
have hv := hbound (formLift j A hc hA y)
rw [formLift_self] at hv
change b * ‖R y‖ ^ 2 ≤ (⟪R y, y⟫_ℂ).re at hv
have hi : (⟪R y, y⟫_ℂ).re ≤ ‖R y‖ * ‖y‖ := re_inner_le_norm (𝕜 := ℂ) _ _
by_cases hz : ‖R y‖ = 0
· change ‖R y‖ ≤ _
rw [hz]
exact mul_nonneg (inv_nonneg.mpr hb.le) (norm_nonneg _)
· have hn : 0 < ‖R y‖ := lt_of_le_of_ne (norm_nonneg _) (Ne.symm hz)
have hby : b * ‖R y‖ ≤ ‖y‖ := by nlinarith
change ‖R y‖ ≤ b⁻¹ * ‖y‖
exact (le_inv_mul_iff₀ hb).mpr hby
omit [CompleteSpace V] [CompleteSpace H] in
lemma form_lower_of_unit (j : V →L[ℂ] H) (hj : Function.Injective j)
(A : V →L[ℂ] V) {b : ℝ}
(hb : ∀ u, ‖j u‖ ^ 2 = 1 → b ≤ (⟪u, A u⟫_ℂ).re) (u : V) :
b * ‖j u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re := by
by_cases hz : j u = 0
· have hu : u = 0 := hj (hz.trans (map_zero j).symm)
simp [hu]
have hn : 0 < ‖j u‖ := norm_pos_iff.mpr hz
let v : V := (‖j u‖⁻¹ : ℂ) • u
have hnv : ‖j v‖ ^ 2 = 1 := by
simp [v, norm_smul, hn.ne']
have hv := hb v hnv
have he : (⟪v, A v⟫_ℂ).re = (‖j u‖ ^ 2)⁻¹ * (⟪u, A u⟫_ℂ).re := by
simp [v, Complex.mul_re, pow_two]
ring
rw [he] at hv
simpa only [mul_comm] using (le_inv_mul_iff₀ (sq_pos_of_pos hn)).mp hv
omit [CompleteSpace V] [CompleteSpace H] in
lemma denseRange_exists_nonzero [Nontrivial H] (j : V →L[ℂ] H) (hd : DenseRange j) :
∃ u, j u ≠ 0 := by
by_contra! h
obtain ⟨x, hx⟩ := exists_ne (0 : H)
have hh : x = 0 := hd.induction_on x (isClosed_eq continuous_id continuous_const) (fun u => h u)
exact hx hh
theorem form_infimum_eq_reciprocal [Nontrivial H] (j : V →L[ℂ] H)
(hj : Function.Injective j) (hd : DenseRange j) (A : V →L[ℂ] V)
(hs : IsSelfAdjoint A) {c : ℝ} (hc : 0 < c)
(hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) :
sInf {e : ℝ | ∃ u : V, ‖j u‖ ^ 2 = 1 ∧ (⟪u, A u⟫_ℂ).re = e} =
‖formResolvent j A hc hA‖⁻¹ := by
let S := {e : ℝ | ∃ u : V, ‖j u‖ ^ 2 = 1 ∧ (⟪u, A u⟫_ℂ).re = e}
let R := formResolvent j A hc hA
have hR : 0 < ‖R‖ := injective_norm_pos R (formResolvent_injective j hj hd A hc hA)
have hne : S.Nonempty := by
obtain ⟨u, hu⟩ := denseRange_exists_nonzero j hd
let v : V := (‖j u‖⁻¹ : ℂ) • u
refine ⟨(⟪v, A v⟫_ℂ).re, v, ?_, rfl⟩
simp [v, norm_smul, hu]
have hl : ∀ e ∈ S, ‖R‖⁻¹ ≤ e := by
rintro e ⟨u, hn, rfl⟩
have hh := form_reciprocal_resolvent_bound j hj hd A hs hc hA u
simpa only [hn, mul_one] using hh
have hbb : BddBelow S := ⟨‖R‖⁻¹, hl⟩
apply le_antisymm
· change sInf S ≤ ‖R‖⁻¹
by_contra! ht
have hm : 0 < sInf S := (inv_pos.mpr hR).trans ht
have hu : ∀ u, ‖j u‖ ^ 2 = 1 → sInf S ≤ (⟪u, A u⟫_ℂ).re :=
fun u hn => csInf_le hbb ⟨u, hn, rfl⟩
have hb := resolvent_norm_le_of_form_bound j A hc hA hm (form_lower_of_unit j hj A hu)
change ‖R‖ ≤ (sInf S)⁻¹ at hb
have hmul := mul_lt_mul_of_pos_right ht hR
have hmle := mul_le_mul_of_nonneg_right hb hm.le
rw [inv_mul_cancel₀ hR.ne'] at hmul
rw [inv_mul_cancel₀ hm.ne'] at hmle
nlinarith
· exact le_csInf hne hl
end CoulombAtom
end
end OAI
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