Similar to D, the Schwartz functions S has a topology determined by the semi-norms ∥⋅∥k,l. A sequence fn→f in S if and only if for any k,l≥0, ∥fn−f∥k,l→0 when n→∞. Recall that the distributions are “dual objects”, i.e. continuous linear functionals, of D. The dual object of S are tempered distributions.
Similarly, one can show that this definition is equivalent to T being continuous linear functional on S in the sense that for every fn→f in S, T(fn)→T(f). To verify this one can use exactly the same trick as the case of D′.
We have S′⊂D′ because D⊂S. But by the following lemma, a tempered distribution is completely determined by its action on S.
Proof. Let χn,1 be the cut-off function constructed in previous lecture. Let fn(x)=χn,1(x)⋅f(x). Then fn∈D. We claim that fn→f in S, i.e. ∥fn−f∥(k,l)=∥(1−χ1,n)f∥k,l→0 for every k,l.
Then ∥(1−χ1,n)f∥k,l=supn≤∣x∣≤n+1∣xk((1−χ1,n)f)(l)∣≤C′supn≤∣x∣≤n+1∑m=0l∣xkf(x)(m)∣, where C′ is a constant depending on derivatives of χ1,n up to order l. This goes to zero when n→∞ because f∈S. □
Let T be a tempered distribution. Suppose we only know T(φ) for every φ∈D. Then for f∈S, from the lemma we can choose φn∈D such that φn→f in S. Then since T is a tempered distribution, T is continuous, so T(f)=limn→∞T(φn). Note that one can show that the sequence T(φn) is Cauchy so the limit exists.
Any locally integrable function is a distribution of degree 0. Let f be a function on R, it determines a distribution Tf such that (Tf,φ)=∫fφ for every φ∈D. Indeed, for every compact set K, every φ∈CK∞(R), ∣(Tf,φ)∣=∣∫fφ∣≤supx∈K∣φ(x)∣⋅∫K∣f∣.
But a function may not be tempered. For example, ex2 is not a tempered distribution. (Tex2,e−x2)=∫ex2⋅e−x2=∫1=∞.
This example tells us that in order for a function to be tempered distribution, it need some restriction, though not strict, on its growth.
Proposition.(1+∣x∣)−mf is bounded for some m, then Tf is a tempered distribution.
Proof. For g∈S, (Tf,g)=∫fg=∫(1+∣x∣)−m(1+∣x∣)m(1+∣x∣)2(1+∣x∣)−2gf≤∥g∥m+2∫C(1+∣x∣)−2<∞, where C is an upper bound of (1+∣x∣)−mf.
We have studied the Fourier transform works well for Schwartz functions. In particular, we have the shifting theorem, derivative theorem, convolution theorem and inversion theorem, and the Poisson summation formula. We are going to see that these also generalizes to tempered distributions. But first, we need to make sense the operations.
Let T∈D′. The derivative of T is defined by the distribution T′ such that (T′,φ)=−(T,φ′) for any φ∈D. One checks that T′ is also a distribution as follows: for every φ∈CK∞(R),
∣(T′,φ)∣=∣(T,φ′)∣≤C∑0≤k≤N∥φ′∥k=C∑0≤k≤N∥φ∥k+1≤C∑0≤k≤N+1∥φ∥k.
As a motivation for the derivative, let’s consider the case when T is determined a smooth function f, in this case, the derivative of Tf should be Tf′. Then (Tf′,φ)=∫f′φ=−∫fφ′=−(Tf,φ′).
We’ll frequently use the integration by parts formula in the special case when one of the function is compact support.
This allow us to define any derivatives of f∈Lloc1(R) in sense of distribution. Let f∈Lloc1(R), define its k-th order derivative by (Tf(k),φ)=(−1)k(T,φ).
Let T be a tempered distribution, then since S′⊂D′, T is a distribution. Then T has derivative T′ as a distribution. It’s straightforward to verify that T′ is also a tempered distribution. What is (T′,g) for g∈S? We already know if g has compact support then (T′,g)=−(T,g). But by the density lemma, T is completely determined by its action on D.
Let f be a smooth function, T∈D′. We can define a new distribution fT. Again, to find it, we use our “try a function first” principle. If T=Tg, then (fTg,h)=∫fgh=(Tg,fh). So we can define fT by its action (fT,φ)=(T,fφ) for φ∈D. To check that fT is a distribution, for φ∈CK∞(R),
∣(fT,φ)∣=∣(T,fφ)∣≤C∑0≤k≤N∥fφ∥k,K≤C′max0≤k≤N∥f∥k,K∑0≤k≤N∥φ∥k,K. Note that we used the Leibnitz rule to calculate ∥fφ∥k,K.
Similarly, if T∈S′, we can show that fT∈S′ for f∈C∞(R) with moderate growth condition (i.e. f growth like polynomial). Then the density lemma implies
In particular, we have the multiplication T↦2πixT defined.
For T∈S, we’ll define its Fourier transform FT. It should be another tempered distribution, and it should be defined by its action on D. Then what should be (FT,φ) for φ∈D? Still, let’s determine this from our “try a function” principle.
Let f,g∈S. Then FTf should be TFf because tempered distribution is generalization of functions. So we need to determine (FTf,g)=(Ff,g)=(Tf,?).