noncomputable def
Orthogonalization.fullAlgebra
(H : Type u_1)
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
:
The von Neumann algebra B(H) of all bounded operators on H.
Equations
- Orthogonalization.fullAlgebra H = { toStarSubalgebra := ⊤, centralizer_centralizer' := ⋯ }
Instances For
@[simp]
theorem
Orthogonalization.mem_fullAlgebra
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[CompleteSpace H]
(x : H →L[ℂ] H)
:
theorem
Orthogonalization.povm_orthogonalization_finDim
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[FiniteDimensional ℂ H]
{ι : Type u_2}
[Fintype ι]
(φ : (H →L[ℂ] H) →ₗ[ℂ] ℂ)
(hφ : ∀ (x : H →L[ℂ] H), 0 ≤ φ (star x * x))
(hφ1 : φ 1 = 1)
(a : ι → H →L[ℂ] H)
(ha0 : ∀ (i : ι), 0 ≤ a i)
(ha1 : ∑ i : ι, a i = 1)
(ε : ℝ)
(hε : 1 - ε < (φ (∑ i : ι, a i * a i)).re)
:
Theorem 1.2 for B(H), H finite-dimensional, any state. A POVM (a i)
on a finite-dimensional Hilbert space and a positive normalized linear functional
φ on B(H) with φ(∑ a i²) > 1 − ε admit a PVM (p i) on H with
φ(∑ |a i − p i|²) < 9ε.
theorem
Orthogonalization.povm_orthogonalization_of_mem_all
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[FiniteDimensional ℂ H]
{ι : Type u_2}
[Fintype ι]
(M : VonNeumannAlgebra H)
(hM : ∀ (x : H →L[ℂ] H), x ∈ M)
(φ : NormalState M)
(a : ι → H →L[ℂ] H)
(ha : IsPOVM M a)
(ε : ℝ)
(hε : 1 - ε < (φ.toLinearMap (∑ i : ι, a i * a i)).re)
:
Theorem 1.2 (povm_orthogonalization) for a von Neumann algebra M containing
every operator of the finite-dimensional space H: the instance of the signed
statement delivered by tier T1a.
theorem
Orthogonalization.povm_orthogonalization_fullAlgebra
{H : Type u_1}
[NormedAddCommGroup H]
[InnerProductSpace ℂ H]
[FiniteDimensional ℂ H]
{ι : Type u_2}
[Fintype ι]
(φ : NormalState (fullAlgebra H))
(a : ι → H →L[ℂ] H)
(ha : IsPOVM (fullAlgebra H) a)
(ε : ℝ)
(hε : 1 - ε < (φ.toLinearMap (∑ i : ι, a i * a i)).re)
:
Theorem 1.2 (povm_orthogonalization) for M = B(H), H finite-dimensional.