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How statement and proof provenance work

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These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Continuous monitoring versus pulsed syndrome protocols

Definition

Fix a nonzero finite-dimensional complex inner-product system space H and a finite time horizon [0,T], where T>0. A pulsed syndrome protocol specifies separated checking times. At checking time tj, for every earlier outcome history h, it specifies a finite-dimensional output space Kj,h, a finite instrument with outcome maps Ij,h,a:L(H)→L(Kj,h), and decoder channels Dj,h,a:L(Kj,h)→L(H) selected using h and the newly observed outcome a. Thus the branch operation Dj,h,a∘Ij,h,a returns an operator on H, the input space for the next checking operation; any intervening evolution in the protocol must also accept and return operators on H. The instrument outcome is called a syndrome record; a zero-probability outcome has no assigned conditional state.

For this interface, a continuous-monitoring protocol specifies an effective conditional evolution together with a time-indexed measurement record. For a specified initial density operator, the model supplies a probability space (Ω,F,P) and, at each t∈[0,T], a measurable record value space (Et,Et) and a random element Yt:(Ω,F)→(Et,Et). The record may be accumulated continuous-current values or a jump record listing detected event times and their labels up to t; the chosen record value spaces and measurable structures are part of the model. Define the available record history by

Gt=σΩ({Ys−1(B):0≤s≤t, B∈Es}).

This increasing family of sub-sigma-algebras of F is the history used here, without completion or right-continuous augmentation. Write D(H) for the density operators on H and equip it with the sigma-algebra ΣD generated by preimages of real Borel sets under the real and imaginary matrix-entry maps in a fixed basis of H. The conditional-state rule supplies maps ρt:Ω→D(H) measurable from Gt to ΣD. Feedback, when present, supplies measurable control value spaces (Ut,Ut) and maps ut:Ω→Ut measurable from Gt to Ut. These measurability requirements mean that states and controls are adapted to the available record history, rather than to unobserved future outcomes. The model specifies the law, initial state and evolution rule linking these objects, the measured coupling, its strength, and the detection efficiency (the modeled fraction of the monitored signal registered). Any additional regularity or stochastic-integration convention needed by that evolution or feedback law is also a model input. A no-feedback model specifies the absence of feedback. This definition asserts neither existence nor uniqueness of a solution of any proposed evolution rule.

Engineered dissipative stabilization is a separate specification of additional generator terms intended to influence the evolution without requiring a measurement record. In the finite GKSL model these terms are specified by their additional coupling matrices and the resulting dissipators. A model may combine stabilization with either protocol.

A comparison as the pulsed interval tends to zero must separately specify a family of pulsed models, the proposed continuous model, a common set X of comparison objects with assignments xδ,xc∈X representing the pulsed model at interval δ>0 and the continuous model, a topology T on X, and an error observable or performance functional with its domain and codomain specified. No convergence of xδ to xc or equality of performance is part of this definition.

Facts & Assumptions

[F1]

A finite instrument has specified input and output spaces and completely positive outcome maps whose sum preserves trace; the supplier defines outcome weights and conditional states only for positive weights. Finite instruments and conditional states

[F2]

A finite-dimensional quantum channel has specified input and output spaces and is a completely positive, trace-preserving linear map on the full operator space. Finite-dimensional quantum channel

[F3]

A finite GKSL generator is specified by a Hermitian Hamiltonian and finitely many coupling matrices; its definition alone asserts neither existence nor uniqueness of a propagator. Finite GKSL generators and units

[F4]

A probability space carries a measure of total mass one, and a random element is a measurable map to its specified measurable value space. Probability measures and probability spaces Random elements and real random variables

[F5]

A density operator on a nonzero finite-dimensional complex inner-product space is a nonnegative endomorphism of trace one. Density operator

[F6]

Every family of subsets of a set generates a unique smallest sigma-algebra containing it; hence that sigma-algebra lies in any ambient sigma-algebra containing the generators. Nonempty intersections of sigma-algebras are sigma-algebras, so the generated sigma-algebra exists and is minimal

[F7]

A topology on a set contains the empty set and the whole set and is closed under arbitrary unions and finite intersections; the Borel sigma-algebra is generated by its open sets. Topology on a set, open and closed sets, clopen sets, the closed-set axiomatisation, and the coarser/finer comparison The Borel sigma-algebra of a topological space

External input

Ahn, Doherty and Landahl describe weak-measurement unravellings of a master equation, a conditioned state and measurement record, and record-dependent feedback in their stated Born–Markov setting. Their diffusive example uses one coupling operator. This is an input to the terminology and model distinction above, not a proof that a particular pulsed protocol has a continuous limit.

Justification

Given: The stated model data and the mathematical interfaces in F1–F7. The independent monitoring citation supplies terminology, not a general stochastic existence theorem.

Goal: Justify the compatibility and information structure of the specifications without asserting a physical realization or a limiting theorem.

1.1 The output operator space of each Ij,h,a is exactly the input operator space of Dj,h,a, whose output is L(H). Their composition therefore has the required input for the next operation. Decoder selection uses only recorded outcomes, and conditional states retain the instrument's positive-weight convention. [given, F1, F2]

1.2 Every generating set Ys−1(B) belongs to F by record measurability, so F6 gives Gt⊆F. For s≤t the generators at s are included among those at t, and minimality gives Gs⊆Gt. The same generated-sigma-algebra construction defines ΣD on the density-operator set using real Borel coordinate tests. Measurability of the supplied ρt and ut relative to Gt is the stipulated information constraint; no conditional-expectation construction or solution theorem is inferred. [given, F4, F5, F6, F7]

2.1 The stabilization clause names additional terms within the finite GKSL definition; it does not claim that an arbitrary added linear map is a physical generator. The comparison data put both represented objects in the same set X with a specified topology, so the proposed limiting claim has a defined setting. Neither this specification nor the monitoring citation proves convergence or equality of performance. [given, F3, F7, step 1.1, step 1.2] ∎

Depends on

Used by · 1

Dependency tree · 2 levels

Each result is drawn at its shortest distance from this item. Arrows run from prerequisites to the items that use them; this item has a heavier outline. External source nodes link directly to the cited text. The view shows up to two dependency steps; open a prerequisite to continue.

External dependencies

Continuous quantum error correction via quantum feedback control · Section II A–B, PDF pp. 2–3, equations (1)–(14).

In the Born–Markov setting, Ahn, Doherty and Landahl describe master-equation unravellings, a conditioned state and measurement record, and record-dependent feedback; equations (8)–(10) are a one-coupling diffusive example.

Hypotheses: Weak system–reservoir coupling and reservoir correlation time short compared with system and interaction times; the diffusive example uses one coupling operator.

Reading limits: Read Section II A–B, equations (1)–(14), including both feedback discussions. Only terminology is imported; the general measurable interface is defined locally. No source-proof audit, experiment, numerical replay or pulsed-limit theorem is claimed.

Sources