Clebsch–Gordan coefficients
E262449
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.
All labels observed (4)
| Label | Occurrences |
|---|---|
| Clebsch–Gordan coefficients canonical | 5 |
| Clebsch–Gordan constraints | 1 |
| Clebsch–Gordan decomposition | 1 |
| Wigner 3-j symbols | 1 |
Statements (50)
| Predicate | Object |
|---|---|
| instanceOf |
mathematical concept
ⓘ
quantum mechanics concept ⓘ representation theory concept ⓘ |
| appearsIn |
addition of spin-1/2 systems
ⓘ
coupling of orbital and spin angular momentum in atoms ⓘ quantum theory of angular momentum ⓘ |
| canBeExpressedAs | square root factors times factorials and sums ⓘ |
| canBeTabulated | finite tables for small j values ⓘ |
| computedBy |
computer algebra systems
ⓘ
explicit closed-form formulas ⓘ recursive relations ⓘ |
| definedFor |
magnetic quantum numbers m1 and m2
ⓘ
pairs of angular momentum quantum numbers j1 and j2 ⓘ resultant angular momentum quantum number J ⓘ resultant magnetic quantum number M ⓘ |
| field |
angular momentum theory
ⓘ
group theory ⓘ quantum mechanics ⓘ representation theory ⓘ |
| hasProperty |
depend on phase conventions
ⓘ
real in standard phase conventions ⓘ symmetric up to phase factors under interchange of j1 and j2 ⓘ vanish when selection rules are not satisfied ⓘ |
| namedAfter |
Alfred Clebsch
ⓘ
Paul Gordan ⓘ |
| relatedTo |
rotation group SO(3)
ⓘ
surface form:
SO(3) Lie group
rotation group SU(2) ⓘ
surface form:
SU(2) Lie group
Wigner 3j symbols ⓘ Wigner 3j symbols ⓘ
surface form:
Wigner 6j symbols
Wigner–Eckart theorem ⓘ spherical harmonics ⓘ |
| satisfies |
completeness relations
ⓘ
orthogonality relations ⓘ selection rule absolute value of j1 minus j2 lessOrEqual J lessOrEqual j1 plus j2 ⓘ selection rule m1 plus m2 equals M ⓘ triangle inequality for angular momenta ⓘ |
| usedFor |
adding quantum angular momenta
ⓘ
calculations in atomic physics ⓘ calculations in nuclear physics ⓘ calculations in particle physics ⓘ changing basis between coupled and uncoupled angular momentum states ⓘ combining two angular momenta ⓘ computing selection rules in spectroscopy ⓘ constructing total angular momentum eigenstates ⓘ coupling spin and orbital angular momentum ⓘ decomposing SO(3) representations ⓘ decomposing SU(2) representations ⓘ decomposing tensor products of representations ⓘ evaluating matrix elements of tensor operators ⓘ spectroscopic term coupling ⓘ |
Referenced by (8)
Full triples — surface form annotated when it differs from this entity's canonical label.
this entity surface form:
Clebsch–Gordan decomposition
this entity surface form:
Wigner 3-j symbols
this entity surface form:
Clebsch–Gordan constraints