Wigner 3j symbols
E674699
Wigner 3j symbols are mathematical coefficients used in quantum mechanics and angular momentum theory to describe the coupling and recoupling of three angular momenta with well-defined symmetry properties.
All labels observed (2)
| Label | Occurrences |
|---|---|
| Wigner 3j symbols canonical | 2 |
| Wigner 6j symbols | 1 |
How this entity was disambiguated
This entity first appeared as the object of triple T7593279 — 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: Wigner 3j symbols Context triple: [Condon–Shortley phase, relatedTo, Wigner 3j symbols]
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A.
Clebsch–Gordan coefficients
Clebsch–Gordan coefficients are numerical factors in quantum mechanics and representation theory that describe how to combine two angular momenta (or group representations) into a single resultant one.
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B.
Wigner–Eckart theorem
The Wigner–Eckart theorem is a fundamental result in quantum mechanics that factorizes matrix elements of tensor operators into a reduced matrix element and a purely geometric part given by Clebsch–Gordan coefficients, greatly simplifying angular momentum calculations.
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C.
Racah algebra
Racah algebra is a mathematical structure in representation theory and quantum mechanics that encodes the symmetries and coupling properties of angular momenta, particularly through Racah coefficients and related special functions.
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D.
Jacobi polynomials
Jacobi polynomials are a family of classical orthogonal polynomials depending on two parameters, widely used in approximation theory, numerical analysis, and solutions of differential equations.
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E.
Brillouin–Wigner perturbation theory
Brillouin–Wigner perturbation theory is a formulation of quantum mechanical perturbation theory that uses an energy-dependent effective Hamiltonian to obtain improved approximations to eigenvalues and eigenstates.
- F. None of above. chosen
- G. Unsure - the case is ambiguous/there is not enough information to decide.
Target entity: Wigner 3j symbols Target entity description: Wigner 3j symbols are mathematical coefficients used in quantum mechanics and angular momentum theory to describe the coupling and recoupling of three angular momenta with well-defined symmetry properties.
-
A.
Clebsch–Gordan coefficients
Clebsch–Gordan coefficients are numerical factors in quantum mechanics and representation theory that describe how to combine two angular momenta (or group representations) into a single resultant one.
-
B.
Wigner–Eckart theorem
The Wigner–Eckart theorem is a fundamental result in quantum mechanics that factorizes matrix elements of tensor operators into a reduced matrix element and a purely geometric part given by Clebsch–Gordan coefficients, greatly simplifying angular momentum calculations.
-
C.
Racah algebra
Racah algebra is a mathematical structure in representation theory and quantum mechanics that encodes the symmetries and coupling properties of angular momenta, particularly through Racah coefficients and related special functions.
-
D.
Jacobi polynomials
Jacobi polynomials are a family of classical orthogonal polynomials depending on two parameters, widely used in approximation theory, numerical analysis, and solutions of differential equations.
-
E.
Brillouin–Wigner perturbation theory
Brillouin–Wigner perturbation theory is a formulation of quantum mechanical perturbation theory that uses an energy-dependent effective Hamiltonian to obtain improved approximations to eigenvalues and eigenstates.
- F. None of above. chosen
Statements (48)
| Predicate | Object |
|---|---|
| instanceOf |
angular momentum coupling coefficient
ⓘ
mathematical object ⓘ special function ⓘ tensor coupling coefficient ⓘ |
| appearsIn |
Gaunt coefficients
NERFINISHED
ⓘ
addition of spherical harmonics ⓘ evaluation of matrix elements of tensor operators ⓘ multipole expansion of interactions ⓘ spherical tensor operator theory ⓘ |
| belongsTo |
representation theory of SU(2)
ⓘ
theory of angular momentum in quantum mechanics ⓘ |
| definedOver | half-integer and integer angular momentum quantum numbers ⓘ |
| expressibleInTermsOf | Clebsch–Gordan coefficients NERFINISHED ⓘ |
| hasAlternativeFormulation |
group-theoretical coupling coefficients of SU(2)
ⓘ
integrals of three spherical harmonics ⓘ |
| hasComputationalUse |
numerical evaluation of transition amplitudes
ⓘ
symbolic manipulation in computer algebra systems ⓘ tabulation of angular momentum coupling coefficients ⓘ |
| hasNotation | ( j1 j2 j3 ; m1 m2 m3 ) with 3x2 array brackets ⓘ |
| hasProperty |
completeness relations
ⓘ
orthogonality relations ⓘ real values in standard phase convention ⓘ vanish when m quantum numbers do not sum to zero ⓘ vanish when triangle inequalities are violated ⓘ well-defined phase convention ⓘ |
| hasSelectionRule |
j1 j2 j3 satisfy angular momentum addition rules
ⓘ
m1 plus m2 plus m3 equals zero ⓘ parity condition j1 plus j2 plus j3 integer ⓘ triangle condition for j1 j2 j3 ⓘ |
| hasSymmetryProperty |
invariance under even permutations of columns
ⓘ
phase factor under column permutations ⓘ sign change under odd permutations of columns ⓘ |
| namedAfter | Eugene Wigner NERFINISHED ⓘ |
| relatedTo |
Clebsch–Gordan coefficients
NERFINISHED
ⓘ
Racah coefficients NERFINISHED ⓘ Wigner 6j symbols ⓘ Wigner 9j symbols NERFINISHED ⓘ |
| standardReference |
Angular Momentum in Quantum Mechanics by A. R. Edmonds
NERFINISHED
ⓘ
Quantum Theory of Angular Momentum by D. A. Varshalovich et al. NERFINISHED ⓘ |
| usedFor |
coupling of three angular momenta
ⓘ
evaluation of Clebsch–Gordan coefficient symmetries ⓘ recoupling of angular momenta ⓘ |
| usedIn |
angular momentum theory
ⓘ
atomic physics ⓘ molecular spectroscopy ⓘ nuclear physics ⓘ quantum chemistry ⓘ quantum mechanics ⓘ |
How these facts were elicited
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Subject: Wigner 3j symbols Description of subject: Wigner 3j symbols are mathematical coefficients used in quantum mechanics and angular momentum theory to describe the coupling and recoupling of three angular momenta with well-defined symmetry properties.
Referenced by (3)
Full triples — surface form annotated when it differs from this entity's canonical label.