Let FF be a number field, FvF_v its completions, and S(Fv)\mathcal S(F_v) the local . Put F=vFvF_\infty=\prod_{v\mid\infty}F_v, and let S(F)\mathcal S(F_\infty) be the completed nuclear tensor product of the archimedean local Schwartz spaces. For each finite place set ev=1Ove_v=1_{\mathcal O_v}. The restricted tensor product of the local is

S(F)^ ⁣vS(Fv)=colimS(S(F)^vSS(Fv))(vvSCev),\mathcal S(F_\infty)\,\widehat\otimes\! \bigotimes_{v\nmid\infty}'\mathcal S(F_v) =\underset{S}{\mathop{\mathrm{colim}}}\, \left(\mathcal S(F_\infty)\widehat\otimes \bigotimes_{v\in S}\mathcal S(F_v)\right) \otimes\left(\bigotimes_{\substack{v\nmid\infty\\v\notin S}} \mathbb C e_v\right),

where SS ranges over finite sets of finite places. The vectors eve_v are part of the definition.

Canonical realization

An elementary tensor determines a function on the restricted product AF=vFv\mathbb A_F=\prod_v'F_v by

x=(xv)vvfv(xv).x=(x_v)_v\longmapsto\prod_v f_v(x_v).

Only finitely many factors differ from 1Ov1_{\mathcal O_v}, and an adele lies in Ov\mathcal O_v at almost every finite place, so this product is well defined. Finite sums of completely separated local functions realize a dense algebraic subspace of the adelic test-function space. They need not exhaust S(F)\mathcal S(F_\infty) when there is more than one archimedean place.

Topology

For a fixed finite SS, the unrestricted factors form a completed nuclear test-function tensor product, while factors outside SS remain fixed. The adelic Schwartz topology is the standard locally convex inductive-limit (LF) topology over these finite sets. Completely separated elementary tensors are dense in each archimedean completion and hence in the resulting adelic space.

Dependence on distinguished vectors

A restricted tensor product is not determined by the spaces S(Fv)\mathcal S(F_v) alone; the vectors eve_v are part of its data. For the additive adeles, 1Ov1_{\mathcal O_v} is the standard unramified choice. Replacing finitely many eve_v gives the same restricted tensor-product space up to its evident canonical identification, whereas changing infinitely many can produce a different restricted product.

References
  1. André Weil, Basic Number Theory, 2nd ed., Springer, 1973. DOI record. Relevant: Chapter II, “Adeles,” restricted products and adelic test functions.
  2. Daniel Bump, Automorphic Forms and Representations, Cambridge University Press, 1997. DOI record. Relevant: Chapter 3, restricted tensor products in adelic harmonic analysis.