Skip to content

Quantum-Gravity Claims, Observables, and Evidence

What does a proposed quantum-gravity description actually predict? This chapter teaches you to specify its observables, states, global data, approximation regime, and possible failures before comparing calculations. The same method distinguishes a tested correspondence from a claim about a complete theory.

Begin with Holographic Duality: Claims, Dictionaries, and Regimes to turn a proposed correspondence into a definite statement.

Helpful background. Duality claims supplies the language of dictionaries; gravitational regimes separates fixed-background, semiclassical, and quantum-gravity questions.

  1. Holographic Duality: Claims, Dictionaries, and Regimes — Specify which theories, sectors, and quantities a correspondence identifies.
  2. Observable and Regime Matrix for Quantum Gravity — Match each observable to the regime in which it is defined.
  3. Relational, Boundary, and Asymptotic Observables — Locate events using physical reference systems or boundary data.
  4. Exact Statements, Saddle Expansions, and Conditional Derivations — Separate exact identities from saddle approximations and conditional deductions.
  5. Dictionary Completeness and Global Data — Identify global information that local correlators miss.
  6. Fixed-Theory, Ensemble, and Superselection Claims — Distinguish a state of one theory from an average over theories.
  7. Nonperturbative Definition and Completion Criteria — Ask what exact rules must supplement a perturbative expansion.
  8. Evidence Programs for Holographic Duality — Compare tests of different parts of a proposed dictionary.
  9. Evidence Independence, Circularity, and Double Counting — Determine which agreements share assumptions or calibration data.
  10. Falsifiers, Negative Results, and Counterexamples — Formulate a negative result against a precise proposition.
  11. Assessing Quantum-Gravity Results and Open Questions — Assess how new results change a bounded scientific conclusion.

A duality dictionary and an approximation to its predictions are different ingredients. In the D3-brane construction, the proposed correspondence extends beyond the large-NN, strong-coupling regime in which classical supergravity is useful Maldacena 1998, § 2. A discrepancy outside that regime can invalidate the approximation without disproving the correspondence.

Tests must also be independent in the relevant sense. Fitting a normalization to one observable and recovering that observable checks implementation; predicting another observable without refitting tests additional content. Neither calculation determines global sectors that it never probes.

Compare the assumptions and limits of these representative conclusions.

Scroll horizontally to compare all columns. Use the Left and Right arrow keys when the table region is focused.

Representative claim domains and validity boundaries for Quantum-Gravity Claims, Observables, and Evidence
Claim object State, ensemble, and conventions Approximation, status, and evidence timing Uncertainty and counterevidence Falsifier Failure condition Licensed conclusion
dictionary Declare both theories and parameter map; use the volume conventions unless the page states a local replacement. Dictionary entry or correspondence claim. Control chain: theory pair and global data → state, algebra, and observable → claim class and regime → evidence and falsifier → bounded conclusion. Sources are cited on the destination page; literature checked through 10 August 2026. Track omitted corrections, alternate branches, and competing definitions. A failed “round-trip one protected observable” check is counterevidence to the promoted claim. With both theories and maps fixed, a protected observable gives incompatible values after normalization and any declared corrections are accounted for. Inferring exact equivalence from one successful observable map. a stated map of observables
saddle result Declare state, contour, and expansion order; use the volume conventions unless the page states a local replacement. Model-specific calculation or conditional result. Control chain: theory pair and global data → state, algebra, and observable → claim class and regime → evidence and falsifier → bounded conclusion. Sources are cited on the destination page; literature checked through 10 August 2026. Track omitted corrections, alternate branches, and competing definitions. A failed “vary saddle and limit order” check is counterevidence to the promoted claim. An omitted admitted saddle or remainder contributes at the claimed retained order, defeating the stated asymptotic accuracy in that regime. Promoting a saddle expansion to a nonperturbative completion. an asymptotic result in its regime
phenomenological proposal Declare mechanism, nuisance model, and data; use the volume conventions unless the page states a local replacement. Proposal or conditional construction. Control chain: theory pair and global data → state, algebra, and observable → claim class and regime → evidence and falsifier → bounded conclusion. Sources are cited on the destination page; literature checked through 10 August 2026. Track omitted corrections, alternate branches, and competing definitions. A failed “compare independent alternatives” check is counterevidence to the promoted claim. Independent data reject the specified mechanism beyond the declared nuisance and model errors; an equally successful alternative separately blocks unique identification. Inferring evidence for a unique UV theory from sensitivity, a bound, or an anomaly. a sensitivity, bound, or anomaly

Download the structured table data (JSON).

Two calculations agree after their normalization is fixed by the same two-point function. Does this constitute two independent tests of the full duality?

Solution

No. Both inherit the calibration and any assumptions used to identify the two-point functions. Each may still test additional interactions or kinematic dependence, but the shared input must be separated from new predictions. Untested global sectors and finite-parameter effects remain open.

Continue to Large N and Semiclassical Bulk Criteria to determine when boundary data support a controlled gravitational approximation.