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.
Aliases (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
NERFINISHED
→
|
| relatedConcept |
Gleason’s theorem
NERFINISHED
→
Stone’s theorem on one-parameter unitary groups NERFINISHED → projective Hilbert space → quantum state space as rays → |
| relatesTo |
Born rule for transition probabilities
NERFINISHED
→
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 (2)
| Subject (surface form when different) | Predicate |
|---|---|
|
Eugene Wigner
→
|
knownFor |
|
Longuet-Higgins theorem in molecular symmetry
("Wigner’s theorem on degeneracies")
→
|
relatedTo |