Exactly consistent Pauli readouts with arbitrary ancillary states #
In a bipartite model (Phase 4 of planning/mipco-track.md) the ancillary state is a model Ξ,
and the EPR state on the sampled register is adjoined to it: the register model
Ξ.reg (Fin n → F) (BipartiteModel.reg), whose state has the norm of Ξ's
(BipartiteModel.norm_reg_ψ).
theorem
MIPRE.Introspection.mirror_expand
{𝒞 : Type u_1}
{𝒜 : Type u_2}
{ℬ : Type u_3}
[Ring 𝒞]
[StarRing 𝒞]
[Algebra ℂ 𝒞]
[Ring 𝒜]
[StarRing 𝒜]
[Algebra ℂ 𝒜]
[Ring ℬ]
[StarRing ℬ]
[Algebra ℂ ℬ]
(Ξ : BipartiteModel 𝒞 𝒜 ℬ)
{V : Type u_4}
{W : Type u_5}
[Fintype V]
[DecidableEq V]
[Fintype W]
[DecidableEq W]
(ψ : V × W → ℂ)
(P : Matrix V V ℂ)
(Q : Matrix W W ℂ)
(h : stateVec ψ P = stateVecB ψ Q)
:
Exact consistency survives adjoining any bipartite ancillary state.
theorem
MIPRE.Introspection.synOf_transpose
{F : Type u_6}
[Field F]
[Fintype F]
[DecidableEq F]
[Algebra (ZMod 2) F]
{n : ℕ}
{w : (Fin n → F) → Matrix (Fin n → F) (Fin n → F) ℂ}
(hw : ∀ (a : Fin n → F), (w a).transpose = w a)
{C : Type u_7}
[DecidableEq C]
(φ : (Fin n → F) → C)
(o : C)
:
A coarse-grained eigenbasis measurement of a symmetric family is symmetric.
theorem
MIPRE.Introspection.reg_wX_mirror
{𝒞 : Type u_1}
{𝒜 : Type u_2}
{ℬ : Type u_3}
[Ring 𝒞]
[StarRing 𝒞]
[Algebra ℂ 𝒞]
[Ring 𝒜]
[StarRing 𝒜]
[Algebra ℂ 𝒜]
[Ring ℬ]
[StarRing ℬ]
[Algebra ℂ ℬ]
(Ξ : BipartiteModel 𝒞 𝒜 ℬ)
{F : Type u_6}
[Field F]
[Fintype F]
[DecidableEq F]
[Algebra (ZMod 2) F]
{n : ℕ}
(v : Fin n → F)
:
The same X Pauli on the two EPR halves is an exact mirror, with arbitrary ancillas.
theorem
MIPRE.Introspection.reg_readout_mirror
{𝒞 : Type u_1}
{𝒜 : Type u_2}
{ℬ : Type u_3}
[Ring 𝒞]
[StarRing 𝒞]
[Algebra ℂ 𝒞]
[Ring 𝒜]
[StarRing 𝒜]
[Algebra ℂ 𝒜]
[Ring ℬ]
[StarRing ℬ]
[Algebra ℂ ℬ]
(Ξ : BipartiteModel 𝒞 𝒜 ℬ)
{F : Type u_6}
[Field F]
[Fintype F]
[DecidableEq F]
[Algebra (ZMod 2) F]
{n : ℕ}
(L : (Fin n → F) →ₗ[F] Fin n → F)
(y : Fin n → F)
:
A coarse-grained Z readout has the same exact mirror.