Theorem
Smooth vectors of the Schrödinger representation
The smooth-vector space of the Heisenberg Schrödinger representation is Schwartz space, with the same topology.
Statement
For the Schrödinger representation of the real Heisenberg group on , the smooth vectors are precisely
where classes are identified with their smooth representatives. The smooth-vector Fréchet topology equals the usual Schwartz topology.
Why both regularity and decay appear
The infinitesimal translation and modulation operators are and . Their ordered products require all weighted weak derivatives to belong to . The iterated-domain characterization therefore tests both spatial differentiability and decay.
Schwartz bounds imply these bounds by adding a sufficiently high polynomial weight. Conversely, applying one-dimensional Sobolev bounds to each makes it bounded, since it and its derivative lie in . These estimates in both directions identify both the space and its topology. The same statement holds on , with multi-indices and sufficiently high Sobolev order.
Pointwise smoothness is not enough
The function
is smooth and square-integrable, but . It is not in the domain of the modulation generator, so it is not a smooth vector for the Heisenberg representation. Smoothness of a representative function and smoothness of its Hilbert-valued orbit map are different requirements.
The resulting rigging
The space of distribution vectors is the continuous anti-dual . Thus
It is the anti-linear version of the familiar tempered-distribution rigging. Unlike an arbitrary smooth-vector space, Schwartz space is nuclear.
References
- Rahul Garg and Sundaram Thangavelu, On the structure of analytic vectors for the Schrödinger representation. §2, opening identification of smooth vectors with Schwartz space, and Theorem 2.2. The equivalence of topologies follows from the weighted Sobolev estimates above.