Kondo lattice model
E1372793
UNEXPLORED
The Kondo lattice model is a theoretical framework in condensed matter physics that describes conduction electrons interacting with a periodic array of localized magnetic moments, often used to study heavy-fermion behavior and related correlated electron phenomena.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Kondo lattice model canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T19377088 — resolving that mention is where its identity was fixed. The disambiguator weighed these candidate entities and picked the highlighted one (or “None”, minting a new entity). This is how homonymy is resolved: the same surface form can point to different entities.
NED1
Entity disambiguation (via context triple)
gpt-5-mini-2025-08-07
Target entity: Kondo lattice model Context triple: [Dynamical Mean-Field Theory, appliesTo, Kondo lattice model]
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A.
Anderson impurity model
The Anderson impurity model is a theoretical framework in condensed matter physics that describes a localized electronic state (impurity) with Coulomb interactions hybridizing with a continuum of conduction electrons, central to understanding phenomena like the Kondo effect.
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B.
t-J model
The t-J model is a theoretical framework in condensed matter physics used to describe strongly correlated electrons on a lattice, particularly in the study of high-temperature superconductivity.
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C.
Hubbard model
The Hubbard model is a fundamental theoretical model in condensed matter physics that describes interacting electrons on a lattice and is widely used to study phenomena such as magnetism, metal–insulator transitions, and high-temperature superconductivity.
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D.
Dynamical Mean-Field Theory
Dynamical Mean-Field Theory is a non-perturbative theoretical approach in condensed matter physics that captures local electronic correlations by mapping lattice models onto self-consistent quantum impurity problems, enabling the study of phenomena such as the Mott metal–insulator transition.
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E.
Luttinger liquid theory
Luttinger liquid theory is a framework describing the collective, non-Fermi-liquid behavior of interacting electrons in one-dimensional conductors, where excitations are best understood as bosonic density waves rather than quasiparticles.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
NED2
Entity disambiguation (via description)
gpt-5-mini-2025-08-07
Target entity: Kondo lattice model Target entity description: The Kondo lattice model is a theoretical framework in condensed matter physics that describes conduction electrons interacting with a periodic array of localized magnetic moments, often used to study heavy-fermion behavior and related correlated electron phenomena.
-
A.
Anderson impurity model
The Anderson impurity model is a theoretical framework in condensed matter physics that describes a localized electronic state (impurity) with Coulomb interactions hybridizing with a continuum of conduction electrons, central to understanding phenomena like the Kondo effect.
-
B.
t-J model
The t-J model is a theoretical framework in condensed matter physics used to describe strongly correlated electrons on a lattice, particularly in the study of high-temperature superconductivity.
-
C.
Hubbard model
The Hubbard model is a fundamental theoretical model in condensed matter physics that describes interacting electrons on a lattice and is widely used to study phenomena such as magnetism, metal–insulator transitions, and high-temperature superconductivity.
-
D.
Dynamical Mean-Field Theory
Dynamical Mean-Field Theory is a non-perturbative theoretical approach in condensed matter physics that captures local electronic correlations by mapping lattice models onto self-consistent quantum impurity problems, enabling the study of phenomena such as the Mott metal–insulator transition.
-
E.
Luttinger liquid theory
Luttinger liquid theory is a framework describing the collective, non-Fermi-liquid behavior of interacting electrons in one-dimensional conductors, where excitations are best understood as bosonic density waves rather than quasiparticles.
- F. None of above. chosen
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.