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Comparative Requirements for Information-Recovery Frameworks

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A durable comparison of information-recovery frameworks must preserve the type of every claim. An exact theorem, a controlled model, a consistency condition, a conjecture, an unknown, and an operational prediction are different kinds of knowledge. This page combines the chapter’s requirements into one matrix and asks what derivation, adverse check, error bound, or observable would satisfy each cell. It does not rank proposals with a single score: a framework can be strong on microscopic unitarity, conditional on its interior reconstruction, and silent on feasible verification.

Required background. Quantum Information for Black-Hole Physics supplies channels, entropy, recovery, and error metrics.

Helpful background. Black-Hole Thermodynamics and Semiclassical Gravity supplies generalized entropy and backreaction; Quantum Fields in Curved Spacetime supplies the horizon EFT baseline; Black-Hole Information supplies the results being compared; Quantum Gravity supplies candidate microscopic completions.

For every framework, record the same objects:

C=(claim,system,state,regime,derivation,error,adverse check,test).\mathcal C= (\text{claim},\text{system},\text{state},\text{regime}, \text{derivation},\text{error},\text{adverse check},\text{test}).

The claim is one sentence that could be false. The system includes Hilbert space or observable algebra and all endpoint sectors. The state and regime fix semiclassical, large-entropy, code-subspace, replica, or protected-sector assumptions. The derivation has an exact source locator. The error names a norm and scaling. The adverse check changes a consequential assumption. The test gives a probability or bounded observable that differs from a competitor.

Missing entries are marked unknown, not inferred from the framework’s motivation. A claim that is meaningful only after ensemble averaging is marked ensemble result, not silently upgraded to one-theory unitarity. A recovery map that exists but has no efficient algorithm is marked existence, not operationally feasible.

Six-axis comparison of representative frameworks

Section titled “Six-axis comparison of representative frameworks”

The table summarizes the strongest conservative statement supported by the named approach. Each cell remains conditional on the detailed page and source; it is not a substitute for those derivations.

Framework or proposalUnitarity and entropyHorizon and EFTInterior and causalityFactorization and microscopic definitionDynamics and errorsOperations and tests
Semiclassical Hawking evolution with complete evaporation, Hawking 1976, §§II–IV, pp. 2462–2471Leading exterior calculation gives thermal flux and rising radiation entropy; a pure-to-mixed endpoint follows if no additional output is admittedControlled for low-curvature exterior observables in the stated state and adiabatic regimeConventional smooth horizon initially, but no unitary late-time interior completionEffective field theory, not a microscopic one-theory completionPredicts flux and stress tensor, but no correlation-restoring late-time channel under its complete-endpoint assumptionsExterior flux is observable; a fine-grained recovery test would require many preparations or microscopic access not supplied by the approximation
Replica wormholes and islands, Almheiri et al. 2020, §§2–6Controlled Page-like generalized entropy in selected bath and holographic modelsCan retain local smooth-horizon EFT while changing the dominant entropy saddleIsland may enter the radiation wedge; recovery exists on a declared code subspaceJT amplitudes admit specified matrix-integral ensemble completions, while the bath-island entropy remains a semiclassical result; the baby-universe interpretation is analyzed in Marolf and Maxfield 2020, §§2–5Entropy transitions are calculable, while individual amplitudes and Lorentzian information transfer are not fixed by the entropy formula aloneDecoder cost and direct verification remain unknown in the generic regime
Holographic error correction, Almheiri, Dong, and Harlow 2015, §§2–4 and Dong, Harlow, and Wall 2016, complete Letter and proofBoundary evolution is unitary in a fixed CFT and bulk entropy is reproduced in controlled large-N settingsSmooth bulk EFT within a semiclassical code subspaceMultiple boundary representations can encode one logical interior operator without cloningFixed boundary theory is defined, but bulk reconstruction is subspace- and order-dependentExact recovery follows under the finite theorem’s hypotheses; approximate gravitational recovery needs a separately derived norm conversionEfficient decoding, coherent radiation access, and a feasible bulk verification protocol remain separate requirements
String microstate and fuzzball programs, Bena et al. 2022, §§2–8Exact state counts and unitary microscopic dynamics exist in important protected sectorsSome constructions replace or modify the conventional horizon; behavior of typical states is disputedInterior may be emergent, state-specific, or absent depending on the proposalFixed string theory supplies a microscopic setting for the constructed sectorsGeneric collapse, radiation dynamics, and approximation error remain incompleteDistinctive observations require predictions stable under source populations, propagation, and detector uncertainty
Soft nonlocal information transfer, Giddings 2013, §§2–5Introduces effective atmosphere-scale couplings designed to transfer correlations with modest energy fluxModifies locality over an atmosphere-scale region rather than imposing a Planckian wallInterior consistency depends on the nonlocal algebra and causal signaling boundsUsually an effective interaction class rather than a UV definitionTransfer rates and exterior response can be estimated once the interaction and state are fixedA useful test must distinguish the transfer from ordinary environmental or near-horizon effects within its time, energy, and backreaction budget
Final-state or postselected interior, Horowitz and Maldacena 2004, §§2–3 and Gottesman and Preskill 2004, complete critiqueCan induce a teleportation-like conditional map with specially entangled final dataMay leave much of exterior EFT unchanged before the endpointReplaces ordinary interior evolution by a final boundary conditionRequires a microscopic rule for postselection and normalizationGeneric interior interactions spoil the ideal map unless additional tuning is imposed; linearity, signaling, and normalization are decisive adverse checksThe proposal must specify probabilities available to exterior observers without assuming access to the postselected interior outcome

The matrix shows why no row receives a blanket label of “solution.” The island row contains a strong controlled entropy result; the holographic row contains a strong fixed-theory unitarity result; the microstate row contains strong constructions in selected sectors. Their unresolved cells are not the same. The modern entropy review explicitly distinguishes a Page curve from individual matrix elements in Almheiri et al. 2021, §§8–11, while the quantum-information review separates recoverability from decoding complexity in Harlow 2016, §§5.4–5.7 and Appendix E.

RequirementSufficient evidence in the claimed regimeStrong adverse check
Unitarity and fine-grained entropyComplete unitary or S-matrix preserving reference entanglement, charges, and final purity, together with a density operator or controlled replica derivation for the declared radiation algebraInclude soft, remnant, baby-universe, and endpoint sectors, test superpositions, and construct inequivalent channels with the same entropy curve
Horizon EFTDressed detector and stress-tensor bounds over stated distances, frequencies, times, and statesAccumulate the proposed corrections over an old hole and test backreaction
Interior consistencyOperator domain, commutators, reconstruction norm, causal access, and endpoint that pass no-cloning and overlap testsEnlarge the code, superpose reference states, or close a duplication protocol
FactorizationNonperturbative fixed-theory definition reproducing connected saddles while preserving independent-boundary productsCompare an ensemble covariance with a genuine one-member observable
Dynamics and errorsReal-time channel or amplitudes with convergence, a named error norm, and a controlled first omitted termChange timestep, regulator, saddle family, state, or coupling and test whether the claimed transfer survives
Operations and testsDecoder, copies, collection efficiency, memory, gates, time, energy, backreaction, and a distinguishable outcome distributionRequire the protocol to meet its actual causal and storage deadlines; an interior comparison must precede its endpoint, while a radiation-only test may occur later

A theorem can satisfy a row without an experiment if the claim is mathematical. An operational claim needs more: a realizable protocol and an outcome model. Conversely, a null astronomical observation cannot decide microscopic unitarity unless competing frameworks predict different likelihoods after source and instrument effects. Generic detector inference and explicit string construction are treated in their own volumes; this page preserves only the requirements they must export to the information question.

Avoid scalar scores and hidden assumptions

Section titled “Avoid scalar scores and hidden assumptions”

Assigning points to the matrix would create false precision. Unknown evidence is not a failed consistency test, and a theorem in a narrow regime is not equal to a qualitative universal claim. Instead, compare frameworks cell by cell using partial order: framework F1F_1 is better supported than F2F_2 on one axis only when both address the same claim and F1F_1 has stronger evidence under no stronger assumptions.

Assumptions should be visible as columns, not footnotes. Examples include a nongravitating bath, replica symmetry, analytic continuation, a fixed alpha sector, large NN, a small code subspace, Haar randomness, protected charge, postselection, or atmosphere-scale nonlocality. If changing one reverses the conclusion, the matrix records that dependence rather than averaging it away.

Model-specific evidence must also retain its direction. JT gravity can show how wormholes and an ensemble fit exactly; it cannot establish that every CFT is averaged. Smooth microstate geometries show that rich horizon-scale states exist; they do not establish that known solutions are typical. Explicit nonlocal couplings show consistency targets; they do not supply a microscopic derivation. These boundaries let genuine progress remain visible without premature universality.

Results and open questions through 2026-08-19

Section titled “Results and open questions through 2026-08-19”
Cross-cutting claimAssumptionsControlled resultLimitation or unresolved comparison
Fine-grained Page behavior can arise gravitationally, Almheiri et al. 2020, §§2–6Specified low-dimensional bath model, state, QES candidates, replica saddles, contour, and continuationReproduces a Page-like generalized-entropy turnover in the stated approximationOne-theory amplitudes, contour uniqueness, and broad four-dimensional control remain separate
Interior operators can be redundantly encoded, Dong, Harlow, and Wall 2016, complete Letter and proofFinite regulated code, declared logical algebra and boundary region, and relative-entropy hypothesesEstablishes multiple physical representatives of one logical operator on the codeLarge-domain, nonperturbative, state-overlap, and efficient-decoding questions remain open
Connected topologies reproduce ensemble correlations, Saad, Shenker, and Stanford 2019, §§2–5Perturbative JT topology expansion and a specified double-scaled matrix-integral completionMatches connected topology terms to connected ensemble observables order by orderDoes not make a universal claim about factorization in every fixed boundary theory
Reflection-positive QFT reconstruction, McNamara and Wang 2026, §1.1, Theorem 1.1; §§5.2–5.3, 9, and 11Finite, multiplicative, reflection-positive closed-manifold partition function in the compact source class, with the full charged spectrumReconstructs a unitary compact functorial QFT and attributes apparent Hilbert-space nonfactorization to omitted charged statesApplication to gravity requires proof of every hypothesis and does not construct the gravitational UV completion
Microscopic state counting and geometries, Bena et al. 2022, §§2–8Protected string-theory sectors and explicitly constructed state families or geometriesSupplies protected entropy counts and many nontrivial microstate constructionsTypical-state geometry and generic real-time evaporation remain proposal-dependent
Operational verification is more demanding than recoverability, Harlow 2016, §§5.4–5.7 and Appendix E and Acharya et al. 2020, §§1.3, 4, and 6–7Declared circuit and access model, finite-dimensional state, independent-copy supply, accuracy, and success probabilityComplexity and copy bounds quantify two distinct resource obstructionsNo single theorem closes copies, gates, time, energy, collection, dressing, and backreaction for every protocol

The strongest competing interpretations differ mainly on how far controlled model results can be exported: some view the combined holographic, island, and error-correction picture as a compelling mechanism; others require a fixed- theory Lorentzian observable and nonperturbative errors before making that claim. The full-spectrum reconstruction theorem supplies a third position under formal-QFT hypotheses: apparent nonfactorization can reflect omitted charged states rather than an ensemble. The conclusions could change if such a calculation appears, if an explicit counterexample defeats a central reconstruction or factorization assumption, or if a feasible experiment distinguishes two rows while respecting its own resource and backreaction budget.

A framework has a fixed unitary boundary Hamiltonian and establishes a JLMS-type relative-entropy mismatch ∣ΔJLMS∣=O(1/N)\lvert\Delta_{\mathrm{JLMS}}\rvert=O(1/N) on a declared code. Which matrix cells are supported, and which remain conditional? The relative-entropy statement is derived in Jafferis et al. 2016, §§2–4.

Solution

Fixed-theory unitarity is supported for the boundary state family, and perturbative relative-entropy matching is supported for the stated code, region, regulator, and central data. The raw O(1/N)O(1/N) mismatch does not automatically become an O(1/N)O(1/N) operator-norm reconstruction error. That stronger cell needs a quantitative recovery theorem with fixed complementary data and an explicit conversion to the chosen channel or operator norm. One must still identify the radiation algebra and derive its fine-grained entropy, show the horizon EFT regime, control nonperturbative errors as the code grows, relate the setup to evaporation, and supply a decoder with time, memory, collection, and backreaction costs. Those cells remain conditional or unknown; they are not failures of the two established results.

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