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Shadow Theory

Observable Quotients and Exact Projected Dynamics: Closure, Memory, Minimal Dynamical Completion, and Effective Field Operators

The exact observable quotient

Jeremy RodgersSection 3 of 14Original PDF ↗Publication DOI ↗

The exact observable quotient

Assumption 2.1.

Hsrc\mathcal{H}_{\mathrm{src}} and Hobs\mathcal{H}_{\mathrm{obs}} are Hilbert spaces and K∈B(Hsrc,Hobs)K\in\mathcal{B}(\mathcal{H}_{\mathrm{src}},\mathcal{H}_{\mathrm{obs}}).

Definition 2.2 (Observational equivalence).

For Ψ,Ψ′∈Hsrc\Psi,\Psi'\in\mathcal{H}_{\mathrm{src}} set Ψ∼KΨ′:⟺KΨ=KΨ′⟺Ψ−Ψ′∈ker⁡K.(2.1) \Psi\sim_{K}\Psi' \quad:\Longleftrightarrow\quad K\Psi=K\Psi' \quad\Longleftrightarrow\quad \Psi-\Psi'\in\ker K .\tag{2.1}

Since KK is continuous, N:=ker⁡KN:=\ker K is a closed subspace of Hsrc\mathcal{H}_{\mathrm{src}}. The quotient vector space HK:=Hsrc/ker⁡K(2.2) \mathcal{H}_{K}:=\mathcal{H}_{\mathrm{src}}/\ker K\tag{2.2} therefore carries the quotient norm ∥[Ψ]∥K:=inf⁡n∈ker⁡K∥Ψ+n∥Hsrc=dist⁡(Ψ,ker⁡K),(2.3) \bigl\lVert[\Psi]\bigr\rVert_{K}:=\inf_{n\in\ker K}\lVert\Psi+n\rVert_{\mathcal{H}_{\mathrm{src}}} =\operatorname{dist}\bigl(\Psi,\ker K\bigr),\tag{2.3} and (HK,∥⋅∥K)(\mathcal{H}_{K},\lVert\cdot\rVert_{K}) is a Hilbert space: the canonical map (ker⁡K)⊥→HK(\ker K)^{\perp}\to\mathcal{H}_{K}, Ψ↦[Ψ]\Psi\mapsto[\Psi], is a linear bijection, and it is isometric because the infimum in (2.3) is attained at the orthogonal projection of Ψ\Psi onto (ker⁡K)⊥(\ker K)^{\perp}. Thus the quotient norm is induced by the inner product ⟨[Ψ],[Ψ′]⟩K:=⟨ΠΨ,ΠΨ′⟩Hsrc\langle [\Psi] , [\Psi'] \rangle_{K}:=\langle \Pi\Psi , \Pi\Psi' \rangle_{\mathcal{H}_{\mathrm{src}}}, where Π\Pi is the orthogonal projection onto (ker⁡K)⊥(\ker K)^{\perp}, and completeness is inherited from that of the closed subspace (ker⁡K)⊥(\ker K)^{\perp}.

The exact observable state associated with a source state Ψ\Psi is the coset [Ψ]K=Ψ+ker⁡K.(2.4) [\Psi]_{K}=\Psi+\ker K .\tag{2.4} It is essential to the logic of what follows that the quotient distinguishes no representative within this coset. The orthogonal representative ΠΨ\Pi\Psi is a choice made by the ambient inner product of Hsrc\mathcal{H}_{\mathrm{src}}, not by the readout.

Theorem 2.3 (Observable quotient theorem).

Under Assumption 2.1, the map K~:HK⟶Ran⁡K,K~[Ψ]:=KΨ,(2.5) \widetilde{K}:\mathcal{H}_{K}\longrightarrow\operatorname{Ran}K, \qquad \widetilde{K}[\Psi]:=K\Psi,\tag{2.5} is well defined, linear, bijective, and bounded, with ∥K~∥op=∥K∥op\lVert\widetilde{K}\rVert_{\mathrm{op}}=\lVert K\rVert_{\mathrm{op}}, where Ran⁡K\operatorname{Ran}K carries the norm inherited from Hobs\mathcal{H}_{\mathrm{obs}}. Moreover the following are equivalent:

  1. K~−1:Ran⁡K→HK\widetilde{K}^{-1}:\operatorname{Ran}K\to\mathcal{H}_{K} is bounded when Ran⁡K\operatorname{Ran}K carries the inherited norm;

  2. Ran⁡K\operatorname{Ran}K is closed in Hobs\mathcal{H}_{\mathrm{obs}};

  3. there exists c>0c>0 with ∥KΨ∥Hobs≥c dist⁡(Ψ,ker⁡K)\lVert K\Psi\rVert_{\mathcal{H}_{\mathrm{obs}}}\ge c\,\operatorname{dist}(\Psi,\ker K) for all Ψ∈Hsrc\Psi\in\mathcal{H}_{\mathrm{src}}.

Proof. Well-definedness and bijectivity. If [Ψ]=[Ψ′][\Psi]=[\Psi'] then Ψ−Ψ′∈ker⁡K\Psi-\Psi'\in\ker K, so KΨ=KΨ′K\Psi=K\Psi'; hence (2.5) does not depend on the representative. Linearity is immediate. Surjectivity onto Ran⁡K\operatorname{Ran}K holds by definition of the range. If K~[Ψ]=0\widetilde{K}[\Psi]=0 then KΨ=0K\Psi=0, i.e. Ψ∈ker⁡K\Psi\in\ker K, i.e. [Ψ]=0[\Psi]=0; hence K~\widetilde{K} is injective.

Boundedness. For every n∈ker⁡Kn\in\ker K, ∥K~[Ψ]∥Hobs=∥KΨ∥=∥K(Ψ+n)∥≤∥K∥op ∥Ψ+n∥Hsrc.\lVert\widetilde{K}[\Psi]\rVert_{\mathcal{H}_{\mathrm{obs}}}=\lVert K\Psi\rVert=\lVert K(\Psi+n)\rVert \le\lVert K\rVert_{\mathrm{op}}\,\lVert\Psi+n\rVert_{\mathcal{H}_{\mathrm{src}}}. Taking the infimum over n∈ker⁡Kn\in\ker K gives ∥K~[Ψ]∥≤∥K∥op∥[Ψ]∥K\lVert\widetilde{K}[\Psi]\rVert\le\lVert K\rVert_{\mathrm{op}}\lVert[\Psi]\rVert_{K}, so ∥K~∥op≤∥K∥op\lVert\widetilde{K}\rVert_{\mathrm{op}}\le\lVert K\rVert_{\mathrm{op}}. Conversely ∥KΨ∥=∥K~[Ψ]∥≤∥K~∥op∥[Ψ]∥K≤∥K~∥op∥Ψ∥\lVert K\Psi\rVert=\lVert\widetilde{K}[\Psi]\rVert\le\lVert\widetilde{K}\rVert_{\mathrm{op}}\lVert[\Psi]\rVert_{K} \le\lVert\widetilde{K}\rVert_{\mathrm{op}}\lVert\Psi\rVert, so the two operator norms coincide.

(1)⇒\Rightarrow(2). Suppose ∥K~−1∥op=:M<∞\lVert\widetilde{K}^{-1}\rVert_{\mathrm{op}}=:M<\infty. Then K~\widetilde{K} is a linear homeomorphism from the complete space HK\mathcal{H}_{K} onto Ran⁡K\operatorname{Ran}K with its inherited norm; hence (Ran⁡K,∥⋅∥Hobs)(\operatorname{Ran}K,\lVert\cdot\rVert_{\mathcal{H}_{\mathrm{obs}}}) is complete. A complete subspace of a normed space is closed, so Ran⁡K\operatorname{Ran}K is closed in Hobs\mathcal{H}_{\mathrm{obs}}.

(2)⇒\Rightarrow(1). If Ran⁡K\operatorname{Ran}K is closed in the Hilbert space Hobs\mathcal{H}_{\mathrm{obs}}, then (Ran⁡K,∥⋅∥Hobs)(\operatorname{Ran}K,\lVert\cdot\rVert_{\mathcal{H}_{\mathrm{obs}}}) is itself a Banach space. Since K~\widetilde{K} is a bounded linear bijection between the Banach spaces HK\mathcal{H}_{K} and Ran⁡K\operatorname{Ran}K, the bounded inverse theorem [1, Cor. 2.7] yields boundedness of K~−1\widetilde{K}^{-1}.

(1)⇔\Leftrightarrow(3). Statement (1) says exactly that there is M<∞M<\infty with ∥[Ψ]∥K≤M∥KΨ∥\lVert[\Psi]\rVert_{K}\le M\lVert K\Psi\rVert for all Ψ\Psi; by (2.3) this is (3) with c=1/Mc=1/M. ◻

Remark 4 (The two norms on Ran⁡K\operatorname{Ran}K).

Theorem 2.3 always allows us to transport the quotient norm to Ran⁡K\operatorname{Ran}K by declaring ∥KΨ∥♯:=∥[Ψ]∥K\lVert K\Psi\rVert_{\sharp}:=\lVert[\Psi]\rVert_{K}; with this transported norm K~\widetilde{K} is by construction an isometric isomorphism, and (Ran⁡K,∥⋅∥♯)(\operatorname{Ran}K,\lVert\cdot\rVert_{\sharp}) is a Hilbert space. What is not generally true is that ∥⋅∥♯\lVert\cdot\rVert_{\sharp} coincides with, or is even equivalent to, the norm inherited from Hobs\mathcal{H}_{\mathrm{obs}}. The inequality ∥⋅∥Hobs≤∥K∥op∥⋅∥♯\lVert\cdot\rVert_{\mathcal{H}_{\mathrm{obs}}}\le\lVert K\rVert_{\mathrm{op}} \lVert\cdot\rVert_{\sharp} always holds on Ran⁡K\operatorname{Ran}K; the reverse inequality holds, with some constant, exactly in the closed-range case. We therefore never write HK≅Ran⁡K\mathcal{H}_{K}\cong\operatorname{Ran}K without saying which norm Ran⁡K\operatorname{Ran}K carries. Every later statement about topologies on the observable side is subject to this distinction.

Corollary 2.5 (Exact loss criterion).

The observation map KK loses exact source distinctions, i.e. there exist Ψ≠Ψ′\Psi\neq\Psi' with Ψ∼KΨ′\Psi\sim_{K}\Psi', if and only if ker⁡K≠{0}\ker K\neq\{0\}. If ker⁡K={0}\ker K=\{0\}, then KK is injective and the source state is uniquely determined by its readout, even if K~−1=K−1\widetilde{K}^{-1}=K^{-1} is unbounded on Ran⁡K\operatorname{Ran}K.

Proof. Immediate from (2.1): Ψ∼KΨ′\Psi\sim_K\Psi' with Ψ≠Ψ′\Psi\neq\Psi' iff Ψ−Ψ′∈ker⁡K∖{0}\Psi-\Psi'\in\ker K\setminus\{0\}. The second sentence is the content of Theorem 2.3: injectivity is the statement ker⁡K={0}\ker K=\{0\} and is logically independent of closedness of Ran⁡K\operatorname{Ran}K, which is what governs boundedness of the inverse. ◻

Corollary 2.5 is the formal separation of (D1) from (D2). Nonidentifiability is a statement about the kernel; instability is a statement about the range. An injective compact operator exhibits the second without the first, as we show in Example 4.5.

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