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Fourier transform acts continuously on Schwartz space

Statement

Assume countable choice. The negative-sign, 2π-normalized Fourier transform is continuous F:SS, and F(αf)(ξ)=(2πiξ)αf^(ξ),βf^=F((2πix)βf).

Facts & Assumptions

Given: Countable choice (The Axiom of Countable Choice (ACω)) for the integral and integration-by-parts interfaces. Euler's formula and the sine/cosine derivatives give the derivative of eit (The derivatives of sine and cosine are cosine and minus sine, exp(x+iy)=ex(cosy+isiny), exp(x+iy)=ex, and eiπ+1=0).

[F1]

Polynomial multiplication and differentiation are continuous on Schwartz space (Basic operations are continuous on Schwartz space).

[F2]

Every weighted Schwartz derivative is integrable with a finite-seminorm norm bound (Schwartz derivatives are integrable).

[F3]

The integral Fourier transform is bounded continuous with supremum at most its input norm (The L1 transform is bounded and uniformly continuous).

[F4]

Dominated convergence applies (Dominated convergence).

[F5]

Absolute integrability permits Fubini (Fubini's theorem for L^1 functions on a sigma-finite product).

[F6]

Whole-line complex integration by parts holds when both derivative products are integrable and the endpoint products vanish (Complex integration by parts on intervals and decaying lines).

Proof

technique · direct
1.1

The interval FTC for eit gives eit1t. Thus the difference quotient in frequency coordinate j is dominated in absolute value by 2πxjf(x), integrable by [F2]. By [F4] its limit is F(2πixjf). The convergence for arbitrary real increments follows either directly from the dominated estimate by truncating the majorant to a finite box and using uniform convergence there, or by the sequential criterion under the stated countable choice. The derivative is continuous by [F3]. Repeating for each weighted function, which remains Schwartz by [F1], proves all ordered derivatives and the second formula.

F1F2F3F4F6given
1.2

Fix the other coordinates and integrate in coordinate j. For u=f restricted to this line and v=e2πixξ, both uv and uv are integrable on the line: multiply u,u by 1+xj2 and use their bounded Schwartz seminorms. Also uv0 at both ends, since xju is bounded. [F6] therefore gives the derivative identity in that coordinate. Integrating over the other coordinates is legitimate by [F2] and [F5], since the full integrals of jf and f are finite. Iteration using [F1] proves the first formula, including zero components of ξ without division by them.

F1F2F5F6given
2.1

Combine the two identities to obtain ξαβf^=(2πi)αF(α((2πix)βf)). By [F3], its supremum is at most (2π)αα((2πix)βf)1. By [F2] and the explicit operation bounds in [F1], this is a finite linear combination of input Schwartz seminorms. Thus every output seminorm is finite, and the finite-neighbourhood definition proves continuity.

step 1.1step 1.2F1F2F3

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