Stone’s theorem on one-parameter unitary groups

E443147

Stone’s theorem on one-parameter unitary groups is a fundamental result in functional analysis and quantum mechanics that characterizes strongly continuous one-parameter unitary groups as being generated by unique self-adjoint operators.

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Statements (48)

Predicate Object
instanceOf mathematical theorem ⓘ
result in operator theory ⓘ
result in quantum mechanics ⓘ
theorem in functional analysis ⓘ
appliesTo self-adjoint operators on a Hilbert space ⓘ
strongly continuous one-parameter unitary groups on a Hilbert space ⓘ
assumes real parameter t in R for the one-parameter group ⓘ
characterizes self-adjoint operators as generators of unitary groups ⓘ
strongly continuous one-parameter unitary groups ⓘ
classificationRole classifies strongly continuous one-parameter unitary groups by their self-adjoint generators ⓘ
concerns densely defined self-adjoint operator A ⓘ
one-parameter unitary group {U(t)}_{t in R} ⓘ
converseStatement If A is a self-adjoint operator on a Hilbert space H, then U(t)=exp(itA) defines a strongly continuous one-parameter unitary group ⓘ
domain Hilbert spaces ⓘ
ensuresProperty the generator of a strongly continuous one-parameter unitary group is closed ⓘ
the generator of a strongly continuous one-parameter unitary group is densely defined ⓘ
field functional analysis ⓘ
mathematical physics ⓘ
operator theory ⓘ
quantum mechanics ⓘ
formalStatement If {U(t)}_{t in R} is a strongly continuous one-parameter unitary group on a Hilbert space H, then there exists a unique self-adjoint operator A such that U(t)=exp(itA) for all real t ⓘ
generalizationOf finite-dimensional diagonalization of normal matrices to continuous unitary flows ⓘ
generatorDefinition the generator A is defined by Aψ = i lim_{t→0} (U(t)ψ − ψ)/t on its domain ⓘ
historicalPeriod 20th century ⓘ
implies the generator of a strongly continuous one-parameter unitary group is self-adjoint ⓘ
the time evolution in quantum mechanics is governed by a self-adjoint Hamiltonian ⓘ
importance links self-adjointness with physical observables in quantum mechanics ⓘ
provides rigorous foundation for Schrödinger time evolution ⓘ
mathematicalArea C*-algebras and unitary representations of groups ⓘ
namedAfter Marshall Harvey Stone ⓘ
linked to: Marshall H. Stone
relatedTo Hille–Yosida theorem ⓘ
Stone–von Neumann theorem ⓘ
spectral theorem ⓘ
relatesConcept one-parameter group ⓘ
self-adjoint operator ⓘ
strong continuity ⓘ
unitary group ⓘ
requiresCondition U(0)=I, the identity operator ⓘ
group property U(t+s)=U(t)U(s) ⓘ
strong continuity of the unitary group ⓘ
statesThat every self-adjoint operator generates a strongly continuous one-parameter unitary group ⓘ
every strongly continuous one-parameter unitary group is generated by a unique self-adjoint operator ⓘ
typicalNotation U(t)=e^{itA} ⓘ
usedIn construction of unitary groups from self-adjoint Hamiltonians ⓘ
description of time evolution of quantum states ⓘ
mathematical formulation of quantum mechanics ⓘ
usesConcept spectral theorem for self-adjoint operators ⓘ
strong operator topology ⓘ

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Full triples — surface form annotated when it differs from this entity's canonical label.

Wigner’s theorem on symmetry transformations → relatedConcept → Stone’s theorem on one-parameter unitary groups ⓘ
Marshall H. Stone → notableWork → Spectral theorem for one-parameter unitary groups ⓘ
linked to: Stone’s theorem on one-parameter unitary groups