Statement

For the of the on H=L2(R)H=L^2(\mathbb R), the are precisely

H∞=S(R),H^\infty=\mathcal S(\mathbb R),

where L2L^2 classes are identified with their smooth representatives. The equals the usual .

Why both regularity and decay appear

The infinitesimal translation and modulation operators are d/dxd/dx and ixix. Their ordered products require all weighted weak derivatives xaf(b)x^a f^{(b)} to belong to L2L^2. The therefore tests both spatial differentiability and decay.

Schwartz bounds imply these L2L^2 bounds by adding a sufficiently high polynomial weight. Conversely, applying one-dimensional to each xaf(b)x^a f^{(b)} makes it bounded, since it and its derivative lie in L2L^2. These estimates in both directions identify both the space and its topology. The same statement holds on Rn\mathbb R^n, with multi-indices and sufficiently high Sobolev order.

Pointwise smoothness is not enough

The function

f(x)=(1+x2)−1/2f(x)=(1+x^2)^{-1/2}

is smooth and square-integrable, but xf∉L2xf\notin L^2. It is not in the domain of the , 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 is the continuous anti-dual S(R)×\mathcal S(\mathbb R)^\times. Thus

S(R)↪L2(R)↪S(R)×.\mathcal S(\mathbb R)\hookrightarrow L^2(\mathbb R) \hookrightarrow\mathcal S(\mathbb R)^\times.

It is the anti-linear version of the familiar tempered-distribution rigging. Unlike an arbitrary smooth-vector space, Schwartz space is nuclear.

References
  1. 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.