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Add lean source and binary files (part 16)
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import Mathlib
import OAI.Analysis.CoulombIonization.FormDomain.UnboundedSpectrum
namespace OAI
noncomputable section
open MeasureTheory Filter
open scoped Topology BigOperators ContDiff
open MeasureTheory Filter
open scoped Topology BigOperators ContDiff InnerProductSpace Convolution
namespace CoulombAtom
section ShiftedFormBottom
variable {V H : Type*} [NormedAddCommGroup V] [InnerProductSpace ℂ V] [CompleteSpace V]
[NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
theorem shifted_form_spectral_infimum [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) (b : ℝ) :
sInf {r : ℝ | (r : ℂ) ∈ unboundedSpectrum
(inverseShift (formResolvent j A hc hA) b)} =
sInf {e : ℝ | ∃ u : V, ‖j u‖ ^ 2 = 1 ∧ (⟪u, A u⟫_ℂ).re - b = e} := by
let S := {e : ℝ | ∃ u : V, ‖j u‖ ^ 2 = 1 ∧ (⟪u, A u⟫_ℂ).re = e}
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 hbb : BddBelow S := ⟨0, fun e ⟨u, _, he⟩ => he ▸ coercive_nonneg A hc hA u⟩
have he : (OrderIso.addRight (-b)) '' S =
{e : ℝ | ∃ u : V, ‖j u‖ ^ 2 = 1 ∧ (⟪u, A u⟫_ℂ).re - b = e} := by
ext e
constructor
· rintro ⟨a, ⟨u, hu, rfl⟩, rfl⟩
exact ⟨u, hu, rfl⟩
· rintro ⟨u, hu, rfl⟩
exact ⟨(⟪u, A u⟫_ℂ).re, ⟨u, hu, rfl⟩, rfl⟩
have hi := (OrderIso.addRight (-b)).map_csInf' hne hbb
rw [he] at hi
change sInf S - b = _ at hi
rw [form_infimum_eq_reciprocal j hj hd A hs hc hA] at hi
rw [inverseShift_spectral_bottom _
(ContinuousLinearMap.nonneg_iff_isPositive.mpr (formResolvent_positive j A hs hc hA))
(formResolvent_injective j hj hd A hc hA)]
exact hi
end ShiftedFormBottom
variable {V H : Type*} [NormedAddCommGroup V] [InnerProductSpace ℂ V] [CompleteSpace V]
[NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
theorem shifted_representedOperator_graph (j : V →L[ℂ] H) (hj : Function.Injective j)
(hd : DenseRange j) (A B : V →L[ℂ] V) (b : ℝ)
(hAB : ∀ u v, ⟪v, A u⟫_ℂ = ⟪v, B u⟫_ℂ + (b : ℂ) * ⟪j v, j u⟫_ℂ)
{c : ℝ} (hc : 0 < c) (hA : ∀ u, c * ‖u‖ ^ 2 ≤ (⟪u, A u⟫_ℂ).re) (x y : H) :
(x, y) ∈ (inverseShift (formResolvent j A hc hA) b).graph ↔
∃ u : V, j u = x ∧ ∀ v : V, ⟪v, B u⟫_ℂ = ⟪j v, y⟫_ℂ := by
have hi := formResolvent_injective j hj hd A hc hA
have hg := representedOperator_graph j hj hd A hc hA x (y + (b : ℂ) • x)
rw [representedOperator, inverseOperator_graph hi] at hg
rw [inverseShift_graph _ hi, hg]
constructor
· rintro ⟨u, hu, he⟩
refine ⟨u, hu, fun v => ?_⟩
have hh := he v
rw [hAB, inner_add_right, inner_smul_right, hu] at hh
exact add_right_cancel hh
· rintro ⟨u, hu, he⟩
refine ⟨u, hu, fun v => ?_⟩
rw [hAB, he, inner_add_right, inner_smul_right, hu]
end CoulombAtom
end
end OAI