Stone's theorem on one-parameter unitary groups
In mathematics, Stone's theorem on one-parameter unitary groups is a basic theorem of functional analysis that establishes a one-to-one correspondence between self-adjoint operators on a Hilbert space Template:Mvar and one-parameter families
and are homomorphisms, i.e.,
Such one-parameter families are ordinarily referred to as strongly continuous one-parameter unitary groups.
The theorem was proved by Template:Harvs, and Template:Harvtxt showed that the requirement that be strongly continuous can be relaxed to say that it is merely weakly measurable, at least when the Hilbert space is separable.
Conversely, let Template:Mvar be a (not necessarily bounded) self-adjoint operator on a Hilbert space Template:Mvar. Then the one-parameter family of unitary operators defined by (using the Spectral Theorem for Self-Adjoint Operators)
is a strongly continuous one-parameter group.
The infinitesimal generator of is defined to be the operator iA. This mapping is a bijective correspondence. Furthermore, Template:Mvar will be a bounded operator if and only if the operator-valued mapping t ↦ Ut is norm-continuous.
Stone's Theorem can be recast using the language of the Fourier transform. The real line R is a locally compact abelian group. Non-degenerate *-representations of the group C*-algebra C∗(R) are in one-to-one correspondence with strongly continuous unitary representations of R, i.e., strongly continuous one-parameter unitary groups. On the other hand, the Fourier transform is a *-isomorphism from C∗(R) to C0(R), the C*-algebra of complex-valued continuous functions on the real line that vanish at infinity. Hence, there is a one-to-one correspondence between strongly continuous one-parameter unitary groups and *-representations of C0(R). As every *-representation of C0(R) corresponds uniquely to a self-adjoint operator, Stone's Theorem holds.
Therefore, the procedure for obtaining the infinitesimal generator of a strongly continuous one-parameter unitary group is as follows.
- Let be a strongly continuous unitary representation of R on a Hilbert space Template:Mvar.
- Integrate this unitary representation to yield a non-degenerate *-representation Template:Mvar of C∗(R) on Template:Mvar by first defining
- and then extending Template:Mvar to all of C∗(R) by continuity.
- Use the Fourier transform to obtain a non-degenerate *-representation Template:Mvar of C0(R) on Template:Mvar.
- By the Riesz-Markov Theorem, Template:Mvar gives rise to a projection-valued measure on R that is the resolution of the identity of a unique self-adjoint operator Template:Mvar, which may be unbounded.
- Then iA is the infinitesimal generator of .
The precise definition of C∗(R) is as follows. Consider the *-algebra Cc(R), the complex-valued continuous functions on R with compact support, where the multiplication is given by convolution. The completion of this *-algebra with respect to the L1-norm is a Banach *-algebra, denoted by . Then C∗(R) is defined to be the enveloping C*-algebra of , i.e., its completion with respect to the largest possible C*-norm. It is a non-trivial fact that, via the Fourier transform, C∗(R) is isomorphic to C0(R). A result in this direction is the Riemann-Lebesgue Lemma, which says that the Fourier transform maps L1(R) to C0(R).
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
In other words, motion on the line is generated by the momentum operator.
Stone's theorem has numerous applications in quantum mechanics. For instance, given an isolated quantum mechanical system, with Hilbert space of states Template:Mvar, time evolution is a strongly continuous one-parameter unitary group on Template:Mvar. The infinitesimal generator of this group is the system Hamiltonian.
The Stone–von Neumann theorem generalizes Stone's theorem to a pair of self-adjoint operators, Q, P satisfying the canonical commutation relation, and shows that these are all unitarily equivalent to the position operator and momentum operator on L2(R).
- K. Yosida, Functional Analysis, Springer-Verlag, (1968)