Wigner’s theorem on symmetry transformations
E98262
Wigner’s theorem on symmetry transformations is a fundamental result in quantum mechanics stating that any symmetry of transition probabilities is represented by either a unitary or antiunitary operator on the system’s Hilbert space.
All labels observed (3)
| Label | Occurrences |
|---|---|
| Wigner’s theorem on symmetry transformations canonical | 2 |
| Wigner’s theorem | 1 |
| Wigner’s theorem on degeneracies | 1 |
Statements (47)
| Predicate | Object |
|---|---|
| instanceOf |
result in mathematical physics
ⓘ
theorem in quantum mechanics ⓘ |
| appliesTo |
pure states in quantum mechanics
ⓘ
rays in Hilbert space ⓘ |
| assumes | symmetry preserves transition probabilities ⓘ |
| characterizes |
automorphisms of the projective Hilbert space preserving transition probabilities
ⓘ
projective symmetries of Hilbert space ⓘ |
| clarifies | why quantum symmetries are represented by unitary or antiunitary operators ⓘ |
| concerns |
Hilbert space structure of quantum states
ⓘ
symmetry transformations in quantum mechanics ⓘ transition probabilities in quantum theory ⓘ |
| domain | Hilbert space of a quantum system ⓘ |
| ensures |
symmetry transformations preserve absolute values of inner products
ⓘ
symmetry transformations preserve transition probabilities between pure states ⓘ |
| field |
functional analysis
ⓘ
mathematical physics ⓘ quantum mechanics ⓘ |
| formalizes | connection between physical symmetries and linear operators on Hilbert space ⓘ |
| hasConsequence |
internal symmetries are represented by unitary operators
ⓘ
spatial rotations are represented by unitary operators ⓘ time-reversal symmetry is represented by an antiunitary operator in many systems ⓘ |
| historicalPeriod | 20th century ⓘ |
| implies |
symmetry transformations act by unitary or antiunitary operators on Hilbert space
ⓘ
symmetry transformations are isometries of projective Hilbert space ⓘ |
| influenced |
axiomatic approaches to quantum mechanics
ⓘ
modern representation theory of quantum symmetries ⓘ quantum information theory treatments of symmetry ⓘ |
| language | mathematical physics terminology ⓘ |
| mathematicalFormulation | bijections of the projective Hilbert space preserving transition probabilities are induced by unitary or antiunitary operators ⓘ |
| namedAfter | Eugene Wigner ⓘ |
| relatedConcept |
Gleason’s theorem
ⓘ
Stone’s theorem on one-parameter unitary groups ⓘ projective Hilbert space ⓘ quantum state space as rays ⓘ |
| relatesTo |
Born rule in quantum mechanics
ⓘ
surface form:
Born rule for transition probabilities
antiunitary operators ⓘ projective representations of groups ⓘ ray representations of symmetry groups ⓘ unitary operators ⓘ |
| requires | complex Hilbert space structure ⓘ |
| statesThat | any symmetry of transition probabilities is implemented by a unitary or antiunitary operator ⓘ |
| typeOf | structure theorem for symmetry transformations ⓘ |
| usedIn |
analysis of parity and charge-conjugation symmetries
ⓘ
analysis of time-reversal symmetry ⓘ classification of quantum symmetries ⓘ derivation of projective unitary representations of symmetry groups ⓘ foundations of quantum theory ⓘ |
Referenced by (4)
Full triples — surface form annotated when it differs from this entity's canonical label.
Longuet-Higgins theorem in molecular symmetry
→
relatedTo
→
Wigner’s theorem on symmetry transformations
ⓘ
this entity surface form:
Wigner’s theorem on degeneracies
this entity surface form:
Wigner’s theorem