- Stone's theorem on one-parameter unitary groups
In
mathematics , Stone's theorem on one-parameterunitary group s is a basic theorem offunctional analysis which establishes aone-to-one correspondence betweenself-adjoint operator s on aHilbert space "H" and one-parameter families ofunitary operators :
which are strongly continuous, that is
:
and are homomorphisms:
:
Such one-parameter families are ordinarily referred to as strongly continuous one-parameter unitary groups. The theorem is named after
Marshall Stone who formulated and proved this theorem in1932 .Formal statement
Let "U" be a strongly continuous 1-parameter unitary group, then there exists a unique self-adjoint operator "A" such that
:
Conversely, let "A" be a self-adjoint operator on a Hilbert space "H". Then
:
is a strongly continuous one-parameter family of unitary operators.
The infinitesimal generator of {"U""t"}"t" is the operator . This mapping is a bijective correspondence. "A" will be a bounded operator
iff the operator-valued function is norm continuous.Example
The family of translation operators
:
is a one-parameter unitary group of unitary operators; the infinitesimal generator of this family is an extension of the differential operator
:
defined on the space of complex-valued continuously differentiable functions of
compact support on R. Thus:
Applications and generalizations
Stone's theorem has numerous applications in
quantum mechanics . For instance, given an isolated quantum mechanical system, with Hilbert space of states "H",time evolution is a strongly continuous one-parameter unitary group on "H". The infinitesimal generator of this group is the system Hamiltonian.The
Hille–Yosida theorem generalizes Stone's theorem to strongly continuous one-parameter semigroups ofcontraction s onBanach space s.References
* M. H. Stone, "On one-parameter unitary groups in Hilbert Space", Annals of Mathematics 33, 643-648, (1932).
* K. Yosida, "Functional Analysis", Springer-Verlag, (1968)
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