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Shadow Theory

Target-Relative Necessity of Completion: When Readout Loss Obstructs, and What a Sufficient Extension Must Retain

Reduced source, readout, and target

Jeremy RodgersSection 3 of 16Original PDF ↗Publication DOI ↗

Reduced source, readout, and target

The reduced source space

Throughout, SS denotes a reduced source space. By this we mean the space obtained from whatever raw description one began with after quotienting by every redundancy that has been declared physically inert: local gauge transformations, coordinate reparametrizations, relabelings of identical constituents, and any further identification that the modeling commitments of the problem require. The point of insisting on this is not fastidiousness. If SS still carried gauge copies, then pp would appear to lose information whenever it merely forgot a gauge label, and every theorem below would be vacuous or misleading: one would be proving obstructions that could be dissolved by a change of gauge. By working on the reduced space we guarantee that two distinct points of SS are genuinely distinct physical configurations, so that a fiber of pp containing two points is a genuine collapse of physical distinctions and not a bookkeeping artifact.

Definition 2.1 (Readout).

A readout is a surjective map p ⁣:S→Tp\colon S\to T of sets. For t∈Tt\in T we write Ft:=p−1(t)={ s∈S:p(s)=t },(3) F_t := p^{-1}(t) = \{\, s\in S: p(s)=t \,\},\tag{3} and call FtF_t the readout fiber over tt. Surjectivity of pp means every fiber is nonempty, and the fibers partition SS.

We write ∼p\sim_p for the equivalence relation on SS induced by pp, so s∼ps′s\sim_p s' iff p(s)=p(s′)p(s)=p(s') iff ss and s′s' lie in a common fiber. The readout is lossy, or noninjective, when some fiber contains more than one point. No topological, smooth, or measurable structure is required for the results of Section 3, Section 4, Section 5, Section 6, Section 7, Section 8; those are statements about maps of sets, and their strength derives from that generality. Structure is imposed only in Section 9, Section 10, Section 11, where the source space is a moduli space of connections and the target values are spectra.

Targets

Definition 2.2 (Target and correct-answer map).

A target QQ on SS consists of

  1. a set AQA_Q of admissible answers, and

  2. a map aQ ⁣:S→AQa_Q\colon S\to A_Q, the correct-answer map, assigning to each reduced source state ss the answer aQ(s)a_Q(s) that is correct for ss.

That aQa_Q is a well-defined map on all of SS is a substantive standing assumption, and it is worth saying what it does and does not import. It asserts that the question has a determinate answer for each reduced source state , that once the physical configuration is fixed, so is the correct answer. It does not assert that the answer is computable, that it is known, or that it is accessible from any particular data. Indeed, the entire content of the paper is the analysis of when the answer, though determinate as a function on SS, fails to be a function of p(s)p(s). If a purported target does not have a determinate answer per reduced source state , if, say, the answer depends on further facts not encoded in SS , then it is not a target on SS in the sense of Definition 2.2, and the source space must be enlarged before the present analysis applies.

Definition 2.3 (Exact readout solvability).

The target QQ is exactly solvable from the readout pp if there exists a map aˉQ ⁣:T⟶AQsuch thataQ=aˉQ∘p.(4) \bar a_Q\colon T\longrightarrow A_Q \qquad\text{such that}\qquad a_Q=\bar a_Q\circ p .\tag{4} We then say that aQa_Q descends along pp, and call aˉQ\bar a_Q a readout-only solution of QQ.

Remark 2.4 (Solving a target is weaker than reconstructing the source).

Definition 2.3 asks only that the correct answer be recoverable from t=p(s)t=p(s). It does not ask that ss itself be recoverable. This is the asymmetry that makes the whole subject nontrivial. A readout can be violently noninjective , collapsing an infinite-dimensional fiber to a point , and still solve a target exactly, provided the target is blind to everything the fiber varies over. Conversely, an almost-injective readout that fails to separate a single critical pair of states can fail to solve a target that hinges on that pair. Injectivity of pp is therefore sufficient for exact solvability of every target, but it is wildly stronger than necessary for any given target, and the gap between the two is where the useful mathematics lives.

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