Fourier analysis
Let u∈L2(R) and let us set
U(x,ξ)=∫e−(x+iξ−y)2/2u(y)dy,x,ξ∈R.
Show that U(x,ξ) is well-defined on R2 and that there exists a constant C>0 such that for all u∈L2(R), we have
∬∣U(x,ξ)∣2e−ξ2dxdξ=C∫∣u(y)∣2dy.
Solution.
First, observe that
(x+iξ−y)2=(x−y)2+2i(x−y)ξ−ξ2.
Thus, its real part is (x−y)2−ξ2, which gives the estimate
∣U(x,ξ)∣≤∫e−(x−y)2/2e−ξ2/2∣u(y)∣dy≤(∫e−(x−y)2eξ2dy)1/2∥u∥L2=eξ2/2(∫e−y2dy)1/2∥u∥L2<∞,(Cauchy-Schwarz)(y↦x−y)
since u∈L2 and e−y2∈L1. Thus, U(x,ξ) exists everywhere on R2. For the second part, observe that
∬∣U(x,ξ)∣2e−ξ2dxdξ=∬∣∣∫e−(x−y)2/2ei(x−y)ξeξ2/2u(y)dy∣∣2e−ξ2dxdξ=∬∣∣∫eiyξe−y2/2u(x−y)dy∣∣2dξdx=∬∥∥e−y2/2u(x−y)∥∥L22dx=∫∥∥e−y2/2u(x−y)∥∥L22dx=∬e−y2∣u(x−y)∣2dydx=∫e−y2∫∣u(x−y)∣2dxdy=(∫e−y2dy)(∫∣u(x)∣2dx)=π∫∣u(y)∣2dy,(Fubini-Tonelli)(Plancherel)(Fubini-Tonelli)(x↦x−y)
so C=π.