AdS/CMT Correspondence¶

Model selected observables of a strongly coupled condensed-matter quantum field theory with a tractable higher-dimensional gravitational system, using an explicit bulk-boundary dictionary and carrying predictions back only within the holographic model's declared validity envelope.

Version: v2 · 2026-09-06 · History
Domain-specific #: 1246
Origin domain: theoretical physics
Subdomain: holographic condensed matter
Aliases: Anti-de Sitter/condensed matter theory correspondence, Anti-de Sitter condensed matter correspondence, Holographic condensed matter

Core Idea¶

AdS/CMT correspondence is a holographic modeling framework for selected strongly coupled condensed-matter systems. It begins with a quantum field theory or low-energy many-body target for which ordinary quasiparticle or perturbative methods are inadequate, chooses a higher-dimensional asymptotically anti-de Sitter gravitational model, fixes a bulk-boundary dictionary between fields and operators, solves the bulk boundary-value problem, and translates the result back into boundary thermodynamics, correlation functions, phases, or transport. Its point is not that a literal laboratory material is secretly a black hole. Its point is that gauge/gravity duality can turn certain strong-coupling questions into classical or semiclassical gravitational calculations in a controlled model.

Scope of Application¶

AdS/CMT lives in theoretical condensed-matter physics at the interface with quantum field theory and gravitational holography. Its scope is broad within that interface but bounded by the availability and credibility of a holographic model.

Quantum critical matter. Finite-temperature dynamics and transport near scale-invariant strongly coupled fixed points can be encoded by black-brane backgrounds and their perturbations.
Compressible quantum matter. Bulk gauge fields and charged horizons model systems at nonzero density, including candidate non-Fermi-liquid and strange-metal regimes.
Superconductors and superfluids. Charged bulk matter can condense below a critical temperature, yielding a boundary order parameter and characteristic conductivity response.
Hydrodynamics and transport. Horizon regularity, conserved fluxes, and linear response give diffusion, viscosity, electric, thermal, and thermoelectric coefficients in declared models.
Translation breaking and momentum relaxation. Lattices, disorder, axion fields, or other deformations can remove the infinite translationally invariant DC response and expose finite transport.
Nonequilibrium dynamics. Time-dependent geometries can model quenches, thermalization, and relaxation when the bulk initial-boundary problem is well posed.
Entanglement and information-sensitive probes. Geometric prescriptions can be used to study entanglement structure, although that wider holographic program is not exhausted by AdS/CMT.

Clarity¶

Clarity begins by separating four levels.

The boundary target is the field theory or many-body phenomenon of interest.
The bulk model is the gravitational representation selected to calculate it.
The dictionary says what bulk variables mean on the boundary.
The material interpretation says whether the result is exact for a specified theory, generic across a class, qualitatively suggestive, or compared with a real system.

Manages Complexity¶

Strongly interacting quantum matter has too many coupled degrees of freedom for a simple quasiparticle description. AdS/CMT manages that complexity by replacing a boundary many-body calculation with a geometric boundary-value problem. Symmetry, conservation laws, temperature, density, and operator content become choices of bulk fields, action terms, geometry, and boundary conditions. The resulting model can reduce a difficult correlation problem to solving coupled ordinary or partial differential equations.

Abstract Reasoning¶

The central move is solve on the tractable side, interpret on the target side. Let \(Z_{\mathrm{QFT}}[\phi_{(0)}]\) be the boundary generating functional with source \(\phi_{(0)}\). In the classical gravity regime,

\[ Z_{\mathrm{QFT}}[\phi_{(0)}]\approx \exp\!\left[-S^{\mathrm{ren}}_{\mathrm{bulk,on\text{-}shell}}[\phi\to\phi_{(0)}]\right]. \]

Knowledge Transfer¶

Within holographic many-body physics, the whole mechanism transfers literally. One can change the boundary phase, dimension, density, symmetry, or observable while retaining the same role package: choose a bulk model, define the dictionary, impose boundary/horizon conditions, solve, extract, and audit validity. That is why the node is a reusable domain abstraction rather than one black-hole example.

Relationships to Other Abstractions¶

Current abstraction AdS/CMT Correspondence Domain-specific

Parents (2) — more general patterns this builds on

AdS/CMT Correspondence is a kind of Representation Prime

AdS/CMT Correspondence instantiates Representation. The boundary theory is the target, the gravitational bulk is the representing medium, the dictionary states which structure is preserved, and the validity ledger supplies the.
AdS/CMT Correspondence presupposes Duality Prime

AdS/CMT Correspondence instantiates Representation. The boundary theory is the target, the gravitational bulk is the representing medium, the dictionary states which structure is preserved, and the validity ledger supplies the.

Hierarchy paths (2) — routes to 2 parentless roots

AdS/CMT Correspondence → Representation → Abstraction

Show alternative path (1)

Neighborhood in Abstraction Space¶

AdS/CMT Correspondence sits in a sparse region of the domain-specific corpus (86^th percentile for distinctiveness): few abstractions share its structure, so a faithful description tends to retrieve it precisely.

Family — Unclustered & Miscellaneous (1565 abstractions)

Nearest neighbors

Computed from structural-signature embeddings · 2026-09-08