Temperley–Lieb algebra
E911208
The Temperley–Lieb algebra is a diagrammatic algebra arising in statistical mechanics and knot theory, central to the study of exactly solvable models and link invariants.
All labels observed (1)
| Label | Occurrences |
|---|---|
| Temperley–Lieb algebra canonical | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T11205458 — 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.
Target entity: Temperley–Lieb algebra Context triple: [Yang–Baxter equation, relatedTo, Temperley–Lieb algebra]
-
A.
Kauffman polynomial
The Kauffman polynomial is a two-variable knot invariant in knot theory that generalizes and extends the information captured by the Jones polynomial.
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B.
Khovanov homology
Khovanov homology is a powerful link invariant in knot theory that lifts the Jones polynomial to a graded homology theory, providing stronger topological information than the polynomial alone.
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C.
Witten–Reshetikhin–Turaev invariant
The Witten–Reshetikhin–Turaev invariant is a quantum invariant of 3-manifolds and links derived from Chern–Simons theory and quantum groups, playing a central role in low-dimensional topology and quantum topology.
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D.
Jones polynomial
The Jones polynomial is a powerful knot invariant in topology that assigns to each knot or link a Laurent polynomial, enabling the distinction of many knots that are indistinguishable by classical invariants.
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E.
Schur–Weyl duality
Schur–Weyl duality is a fundamental result in representation theory that links representations of the symmetric group and the general linear group via their commuting actions on tensor powers of a vector space.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Temperley–Lieb algebra Target entity description: The Temperley–Lieb algebra is a diagrammatic algebra arising in statistical mechanics and knot theory, central to the study of exactly solvable models and link invariants.
-
A.
Kauffman polynomial
The Kauffman polynomial is a two-variable knot invariant in knot theory that generalizes and extends the information captured by the Jones polynomial.
-
B.
Khovanov homology
Khovanov homology is a powerful link invariant in knot theory that lifts the Jones polynomial to a graded homology theory, providing stronger topological information than the polynomial alone.
-
C.
Witten–Reshetikhin–Turaev invariant
The Witten–Reshetikhin–Turaev invariant is a quantum invariant of 3-manifolds and links derived from Chern–Simons theory and quantum groups, playing a central role in low-dimensional topology and quantum topology.
-
D.
Jones polynomial
The Jones polynomial is a powerful knot invariant in topology that assigns to each knot or link a Laurent polynomial, enabling the distinction of many knots that are indistinguishable by classical invariants.
-
E.
Schur–Weyl duality
Schur–Weyl duality is a fundamental result in representation theory that links representations of the symmetric group and the general linear group via their commuting actions on tensor powers of a vector space.
- F. None of above. chosen
Statements (52)
| Predicate | Object |
|---|---|
| instanceOf |
algebra
ⓘ
associative algebra ⓘ cellular algebra ⓘ diagram algebra ⓘ diagrammatic algebra ⓘ finite-dimensional algebra ⓘ |
| appearsIn |
conformal field theory
NERFINISHED
ⓘ
integrable systems ⓘ |
| arisesIn |
Potts model
NERFINISHED
ⓘ
exactly solvable models ⓘ ice-type models ⓘ lattice models in statistical mechanics ⓘ |
| centralTo |
Jones polynomial
NERFINISHED
ⓘ
planar algebras ⓘ study of link invariants ⓘ subfactor theory ⓘ |
| definedOver |
commutative ring
ⓘ
field ⓘ |
| dependsOn | integer n ⓘ |
| dimensionFormula | Catalan number C_n ⓘ |
| fieldOfStudy |
knot theory
ⓘ
low-dimensional topology ⓘ mathematics ⓘ quantum algebra ⓘ representation theory ⓘ statistical mechanics ⓘ |
| hasBasis |
non-crossing pairings
ⓘ
planar diagrams ⓘ |
| hasMultiplicationDefinedBy | concatenation of diagrams ⓘ |
| hasNotation | TL_n(q) NERFINISHED ⓘ |
| hasParameter | loop parameter q ⓘ |
| hasProperty |
non-semisimple at roots of unity
ⓘ
semisimple for generic q ⓘ |
| hasRelation |
e_i e_j = e_j e_i for |i-j|>1
ⓘ
e_i e_{i\\pm1} e_i = e_i ⓘ e_i^2 = \\delta e_i ⓘ |
| introducedBy |
Elliott Lieb
NERFINISHED
ⓘ
Neville Temperley NERFINISHED ⓘ |
| quotientOf | Hecke algebra of type A NERFINISHED ⓘ |
| relatedTo |
Catalan numbers
ⓘ
Hecke algebra of type A NERFINISHED ⓘ Jones–Wenzl idempotents NERFINISHED ⓘ Kauffman bracket NERFINISHED ⓘ braid group NERFINISHED ⓘ planar non-crossing partitions ⓘ subfactors of type II_1 ⓘ |
| usedFor |
construction of Jones polynomial
ⓘ
exact diagonalization of lattice models ⓘ representation theory of quantum groups ⓘ study of quantum spin chains ⓘ transfer matrices in statistical mechanics ⓘ |
| yearOfIntroduction | 1971 ⓘ |
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Subject: Temperley–Lieb algebra Description of subject: The Temperley–Lieb algebra is a diagrammatic algebra arising in statistical mechanics and knot theory, central to the study of exactly solvable models and link invariants.
Referenced by (1)
Full triples — surface form annotated when it differs from this entity's canonical label.