LiouvilleCFT — model index

Non-compact Liouville CFT (Polyakov 1981) at coupling b > 0. The canonical self-dual point b = 1 (background charge Q = 2, c = 25) is used as the default. The b ↔ 1/b self-duality leaves both Q and c invariant.

Provisional v2 view — RES not wired

Generated by docs/atlas/generate.jl — a pure VIEW over the *_registry.jl claims + the static test/INVENTORY.jsonl AST scan. No test is executed and no src is run; test/INVENTORY.jsonl is regenerated in-place (idempotently) from that static scan; fetch/@register untouched. Assurance labels are PROVISIONAL: residuals / confidence are not shown yet (RES not wired). Badges reflect the committed test AST, not the latest CI run — a hub can read green while its @test is red between regenerations. @sweep = a graceful regime-resolution gap, not card omission.

All (Quantity, BC) hubs src claims for LiouvilleCFT. Cells link to the per-hub card; = not yet implemented at that BC. The shape of the matrix is the gap visualisation: empty cells are where physics could be added next.

Convention

FieldValue
Hamiltoniansee file-header description above
Observableper src/core/quantities.jl (matches the dispatch tag)
Referencedocs/src/conventions.md (project-wide convention policy)
STATUSbackfilled by PR (audit gate); per-field domain content

Coverage

LevelCount
🟣 universality-corroborated0
🟢 corroborated-at-p2
🔵 coherent0
⚪ cited-only0
🟠 uncorroborated-but-feasible0
total claimed hubs2

Methods (from @register, derived): analytic

Quantity × BC matrix

QuantityInfinite
CentralCharge🟢 hub
ConformalWeights🟢 hub

References

Papers cited by this model's @register cards. The full numbered list is on the Reference List.

[65]
A. Polyakov. Quantum geometry of bosonic strings. Physics Letters B 103, 207–210 (1981).
[66]
A. Zamolodchikov and A. Zamolodchikov. Conformal bootstrap in Liouville field theory. Nuclear Physics B 477, 577–605 (1996).

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