Part 3.II

Distributions and Fourier Transforms

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Problem 3.6.1

Suppose ff is a complex continuous function in Rn\mathbb {R}^{n}, with compact support. Prove that ψPj→f\psi P_{j} \rightarrow f uniformly on Rn\mathbb {R}^{n}, for some ψ∈D\psi \in \mathscr {D} and for some sequence {Pj}\left\{ P_{j}\right\} of polynomials.

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Problem 3.6.2

Show that the metrizable topology for D(Ω)\mathscr {D}(\Omega ) that was rejected in Section 6.2 is not complete for any Ω\Omega.

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Problem 3.6.3

If EE is an arbitrary closed subset of Rn\mathbb {R}^{n}, show that there is an f∈C∞(Rn)f \in C^{\infty }\left(\mathbb {R}^{n}\right) such that f(x)=0f(x) = 0 for every x∈Ex \in E and f(x)>0f(x) > 0 for every other x∈Rnx \in \mathbb {R}^{n}.

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Problem 3.6.4

Suppose Λ∈D′(Ω)\Lambda \in \mathscr {D}^{\prime }(\Omega ) and Λϕ≥0\Lambda \phi \geq 0 whenever ϕ∈D(Ω)\phi \in \mathscr {D}(\Omega ) and ϕ≥0\phi \geq 0. Prove that Λ\Lambda is then a positive measure in Ω\Omega (which is finite on compact sets).

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Problem 3.6.5

Prove that the numbers cαβc_{\alpha \beta } in the Leibniz formula are

cαβ=∏i=1nαi!βi!(αi−βi)! c_{\alpha \beta } = \prod _{i = 1}^{n} \frac{\alpha _{i}!}{\beta _{i}!\left(\alpha _{i}-\beta _{i}\right)!}
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Problem 3.6.6
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(a)

Suppose cm=exp⁡{−(m!)!},m=0,1,2,…c_{m} = \exp \left\{ -(m!)!\right\} , m = 0,1,2, \ldots. Does the series

∑m=0∞cm(Dmϕ)(0) \sum _{m = 0}^{\infty } c_{m}\left(D^{m} \phi \right)(0)

converge for every ϕ∈C∞(R)\phi \in C^{\infty }(R)?

(b)

Let Ω\Omega be open in Rn\mathbb {R}^{n}, suppose Λi∈D′(Ω)\Lambda_{i} \in \mathscr {D}^{\prime }(\Omega ), and suppose that all Λi\Lambda_{i} have their supports in some fixed compact K⊂ΩK \subset \Omega. Prove that the sequence {Λi}\left\{ \Lambda_{i}\right\} cannot converge in D′(Ω)\mathscr {D}^{\prime }(\Omega ) unless the orders of the Λj\Lambda_{j} are bounded. Hint: Use the Banach-Steinhaus theorem.

(c)

Can the assumption about the supports be dropped in (b)?

Problem 3.6.7

Let Ω=(0,∞)\Omega = (0, \infty ). Define

Λϕ=∑m=1∞(Dmϕ)(1m)[ϕ∈D(Ω)] \Lambda \phi = \sum _{m = 1}^{\infty }\left(D^{m} \phi \right)\left(\frac{1}{m}\right) \quad [\phi \in \mathscr {D}(\Omega )]

Prove that Λ\Lambda is a distribution of infinite order in Ω\Omega. Prove that Λ\Lambda cannot be extended to a distribution in RR; that is, there exists no Λ0∈D′(R)\Lambda_{0} \in \mathscr {D}^{\prime }(R) such that Λ0=Λ\Lambda_{0} = \Lambda in (0,∞)(0, \infty ).

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Problem 3.6.8

Characterize all distributions whose supports are finite sets.

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Problem 3.6.9
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(a)

Prove that a set E⊂D(Ω)E \subset \mathscr {D}(\Omega ) is bounded if and only if

sup⁡{∣Λϕ∣:ϕ∈E}<∞ \sup \left\{ \left|\Lambda \phi \right|: \phi \in E\right\} < \infty

for every Λ∈D′(Ω)\Lambda \in \mathscr {D}^{\prime }(\Omega ).

(b)

Suppose {ϕj}\left\{ \phi_{j}\right\} is a sequence in D(Ω)\mathscr {D}(\Omega ) such that {Λϕj}\left\{ \Lambda \phi_{j}\right\} is a bounded sequence of numbers, for every Λ∈D′(Ω)\Lambda \in \mathscr {D}^{\prime }(\Omega ). Prove that some subsequence of {ϕj}\left\{ \phi_{j}\right\} converges, in the topology of D(Ω)\mathscr {D}(\Omega ).

(c)

Suppose {Λj}\left\{ \Lambda_{j}\right\} is a sequence in D′(Ω)\mathscr {D}^{\prime }(\Omega ) such that {Λjϕ}\left\{ \Lambda_{j} \phi \right\} is bounded, for every ϕ∈D(Ω)\phi \in \mathscr {D}(\Omega ). Prove that some subsequence of {Λj}\left\{ \Lambda_{j}\right\} converges in D′(Ω)\mathscr {D}^{\prime }(\Omega ) and that the convergence is uniform on every bounded subset of D(Ω)\mathscr {D}(\Omega ). Hint: By the Banach-Steinhaus theorem, the restrictions of the Λj\Lambda_{j} to DK\mathscr {D}_{K} are equicontinuous. Apply Ascoli's theorem.

Problem 3.6.10

Suppose {fi}\left\{ f_{i}\right\} is a sequence of locally integrable functions in Ω\Omega (an open set in Rn\mathbb {R}^{n}) and

lim⁡i→∞∫K∣fi(x)∣dx=0 \lim _{i \rightarrow \infty } \int _{K}\left|f_{i}(x)\right| d x = 0

for every compact K⊂ΩK \subset \Omega. Prove that then Dαfi→0D^{\alpha } f_{i} \rightarrow 0 in D′(Ω)\mathscr {D}^{\prime }(\Omega ), as i→∞i \rightarrow \infty, for every multi-index α\alpha.

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Problem 3.6.11

Suppose Ω\Omega is open in R2\mathbb {R}^{2}, and {fi}\left\{ f_{i}\right\} is a sequence of harmonic functions in Ω\Omega that converges in the distribution sense to some Λ∈D′(Ω)\Lambda \in \mathscr {D}^{\prime }(\Omega ); explicitly, the assumption is that

Λϕ=lim⁡i→∞∫Ωfi(x)ϕ(x)dx[ϕ∈D(Ω)] \Lambda \phi = \lim _{i \rightarrow \infty } \int _{\Omega } f_{i}(x) \phi (x) d x \quad [\phi \in \mathscr {D}(\Omega )]

Prove then that {fi}\left\{ f_{i}\right\} converges uniformly on every compact subset of Ω\Omega and that Λ\Lambda is a harmonic function. Hint: If ff is harmonic, f(x)f(x) is the average of ff over small circles centered at xx.

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Problem 3.6.12

Recall that δ\delta (the Dirac measure) is the distribution defined by δ(ϕ)=ϕ(0)\delta (\phi ) = \phi (0), for ϕ∈D(R)\phi \in \mathscr {D}(R). For which f∈C∞(R)f \in C^{\infty }(R) is it true that fδ′=0f \delta^{\prime } = 0? Answer the same question for fδ′′f \delta^{\prime \prime }. Conclude that a function f∈C∞(R)f \in C^{\infty }(R) may vanish on the support of a distribution Λ∈D′(R)\Lambda \in \mathscr {D}^{\prime }(R) although fΛ≠0f \Lambda \neq 0.

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Problem 3.6.13

If ϕ∈D(Ω)\phi \in \mathscr {D}(\Omega ) and Λ∈D′(Ω)\Lambda \in \mathscr {D}^{\prime }(\Omega ), does either of the statements

ϕΛ=0,Λϕ=0 \phi \Lambda = 0, \quad \Lambda \phi = 0

imply the other?

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Problem 3.6.14

Suppose KK is the closed unit ball in Rn,Λ∈D′(Rn)\mathbb {R}^{n}, \Lambda \in \mathscr {D}^{\prime }\left(\mathbb {R}^{n}\right) has its support in KK, and f∈C∞(Rn)f \in C^{\infty }\left(\mathbb {R}^{n}\right) vanishes on KK. Prove that fΛ=0f \Lambda = 0. Find other sets KK for which this is true. (Compare with Exercise 12).

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Problem 3.6.15

Suppose K⊂V⊂Ω,KK \subset V \subset \Omega , K is compact, VV and Ω\Omega are open in Rn,Λ∈D′(Ω)\mathbb {R}^{n}, \Lambda \in \mathscr {D}^{\prime }(\Omega ) has its support in KK, and {ϕi}⊂D(Ω)\left\{ \phi_{i}\right\} \subset \mathscr {D}(\Omega ) satisfies

lim⁡i→∞[sup⁡x∈V∣(Dαϕi)(x)∣]=0(a) \lim _{i \rightarrow \infty }\left[\sup _{x \in V}\left|\left(D^{\alpha } \phi _{i}\right)(x)\right|\right] = 0 \tag {a}

for every multi-index α\alpha. Prove that then

lim⁡t→∞Λ(ϕi)=0 \lim _{t \rightarrow \infty } \Lambda \left(\phi _{i}\right) = 0
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Problem 3.6.16

The preceding statement becomes false if VV is replaced by KK in the hypothesis (a). Show this by means of the following example, in which Ω=R\Omega = R. Choose c1>c2>⋯>0c_{1} > c_{2} > \cdots > 0, such that ∑cj<∞\sum c_{j} < \infty; define

Λϕ=∑j=1∞(ϕ(cj)−ϕ(0))(ϕ∈D(R)) \Lambda \phi = \sum _{j = 1}^{\infty }\left(\phi \left(c_{j}\right)-\phi (0)\right) \quad (\phi \in \mathscr {D}(R))

and consider functions ϕi∈D(R)\phi_{i} \in \mathscr {D}(R) such that ϕi(x)=0\phi_{i}(x) = 0 if x≤ci+1,ϕi(x)=1/ix \leq c_{i+1}, \phi_{i}(x) = 1 / i if ci≤x≤c1c_{i} \leq x \leq c_{1}. Show also that this Λ\Lambda is a distribution of order 1.

However, for certain K,VK, V can be replaced by KK in the hypothesis (a) of Exercise 15. Show that this is so when KK is the closed unit ball of Rn\mathbb {R}^{n}. Find other sets KK for which this is true.

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Problem 3.6.17

If Λ∈D′(R)\Lambda \in \mathscr {D}^{\prime }(R) has order NN, show that Λ=DN+2f\Lambda = D^{N+2} f, for some continuous function ff. If Λ=δ\Lambda = \delta, what are the possibilities for ff?.

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Problem 3.6.18

Express δ∈D′(R2)\delta \in \mathscr {D}^{\prime }\left(\mathbb {R}^{2}\right) in the form given by Theorem 6.27, as explicitly as you can.

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Problem 3.6.19

Suppose Λ∈D′(Ω),ϕ∈D(Ω)\Lambda \in \mathscr {D}^{\prime }(\Omega ), \phi \in \mathscr {D}(\Omega ), and (Dαϕ)(x)=0\left(D^{\alpha } \phi \right)(x) = 0 for every xx in the support of Λ\Lambda and for every multi-index α\alpha. Prove that Λϕ=0\Lambda \phi = 0. Suggestion: Do it first for distributions with compact support, by the method used in Theorem 6.25.

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Problem 3.6.20

Prove that every continuous linear functional on C∞(Ω)C^{\infty }(\Omega ) is of the form f→Λff \rightarrow \Lambda f, where Λ\Lambda is a distribution with compact support in Ω\Omega; this is a converse to (d)(d) of Theorem 6.24.

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Problem 3.6.21

Let C∞(T)C^{\infty }(T) be the space of all infinitely differentiable complex functions on the unit circle TT in C\mathscr {C}. One may regard C∞(T)C^{\infty }(T) as the subspace of C∞(R)C^{\infty }(R) consisting of those functions that have period 2π2 \pi. Suppose

f(z)=∑n=0∞anzn f(z) = \sum _{n = 0}^{\infty } a_{n} z^{n}

converges in the open unit disc UU in C\mathcal{C}. Prove that each of the following three properties of ff implies the other two:

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(a)

There exist p<∞p < \infty and γ<∞\gamma < \infty such that

∣an∣≤γ⋅np(n=1,2,3,…) \left|a_{n}\right| \leq \gamma \cdot n^{p} \quad (n = 1,2,3, \ldots )
(b)

There exist p<∞p < \infty and γ<∞\gamma < \infty such that

∣f(z)∣≤γ⋅(1−∣z∣)−p(z∈U) \left|f(z)\right| \leq \gamma \cdot (1-\left|z\right|)^{-p} \quad (z \in U)
(c)

lim⁡r→1∫−ππf(reiθ)ϕ(eiθ)dθ\lim_{r \rightarrow 1} \int_{-\pi }^{\pi } f\left(r e^{i \theta }\right) \phi \left(e^{i \theta }\right) d \theta exists (as a complex number) for every ϕ∈C∞(T)\phi \in C^{\infty }(T).

Problem 3.6.22

For u∈D′(R)u \in \mathscr {D}^{\prime }(R), show that

u−τxux→Du in D′(R) \frac{u-\tau _{x} u}{x} \rightarrow D u \quad \text{ in } \mathscr {D}^{\prime }(R)

as x→0x \rightarrow 0. (The derivative of uu may thus still be regarded as a limit of quotients).

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Problem 3.6.23

Suppose {fi}\left\{ f_{i}\right\} is a sequence of locally integrable functions in Rn\mathbb {R}^{n}, such that

lim⁡i→∞(fi∗ϕ)(x) \lim _{i \rightarrow \infty }\left(f_{i} * \phi \right)(x)

exists, for each ϕ∈D(Rn)\phi \in \mathscr {D}\left(\mathbb {R}^{n}\right) and each x∈Rnx \in \mathbb {R}^{n}. Prove that then {Da(fi∗ϕ)}\left\{ D^{a}\left(f_{i} * \phi \right)\right\} converges uniformly on compact sets, for each multi-index α\alpha.

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Problem 3.6.24

Let HH be the Heaviside function on RR, defined by

H(x)={1 if x>00 if x≤0 H(x) = \begin{cases} 1 & \text{ if } x > 0 \\ 0 & \text{ if } x \leq 0\end{cases}

and let δ\delta be the Dirac measure.

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(a)

Show that (H∗ϕ)(x)=∫−∞xϕ(s)ds(H * \phi )(x) = \int_{-\infty }^{x} \phi (s) d s, if ϕ∈D(R)\phi \in \mathscr {D}(R).

(b)

Show that δ′∗H=δ\delta^{\prime } * H = \delta.

(c)

Show that 1∗δ′=01 * \delta^{\prime } = 0. (Here 1 denotes the locally integrable function whose value is 1 at every point and which is thought of as a distribution).

(d)

It follows that the associative law fails:

1∗(δ′∗H)=1∗δ=1 1 *\left(\delta ^{\prime } * H\right) = 1 * \delta = 1

but

(1∗δ′)∗H=0∗H=0 \left(1 * \delta ^{\prime }\right) * H = 0 * H = 0
Problem 3.6.25

Here is another characterization of convolutions analogous to Theorem 6.33. Suppose LL is a continuous linear mapping of D\mathscr {D} into C∞C^{\infty } which commutes with every DαD^{\alpha }, that is, (a)

LDαϕ=DαLϕ(ϕ∈D) L D^{\alpha } \phi = D^{\alpha } L \phi \quad (\phi \in \mathscr {D})

Then there is a u∈D′u \in \mathscr {D}^{\prime } such that

Lϕ=u∗ϕ L \phi = u * \phi

Suggestion: Fix ϕ∈D\phi \in \mathscr {D}, put

h(x)=(τ−xLτxϕ)(0)=(Lτxϕ)(x)(x∈Rn) h(x) = \left(\tau _{-x} L \tau _{x} \phi \right)(0) = \left(L \tau _{x} \phi \right)(x) \quad \left(x \in \mathbb {R}^{n}\right)

let DeD_{e} be the directional derivative used in the proof of Theorem 6.30, and show that

(Deh)(x)=(DeLτxϕ)(x)−(LτxDeϕ)(x) \left(D_{e} h\right)(x) = \left(D_{e} L \tau _{x} \phi \right)(x)-\left(L \tau _{x} D_{e} \phi \right)(x)

which is 0 if (a) holds. Thus h(x)=h(0)h(x) = h(0), which implies that τxL=Lτx\tau_{x} L = L \tau_{x}. Can the assumption that the range of LL is in C∞C^{\infty } be weakened?

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Problem 3.6.26

If f∈L1((−∞,−δ)∪(δ,∞))f \in L^{1}((-\infty ,-\delta ) \cup (\delta , \infty )) for every δ>0\delta > 0, define its principal value integral to be

PV∫−∞∞f(x)dx=lim⁡δ→0(∫−∞−δ+∫δ∞)f(x)dx P V \int _{-\infty }^{\infty } f(x) d x = \lim _{\delta \rightarrow 0}\left(\int _{-\infty }^{-\delta }+\int _{\delta }^{\infty }\right) f(x) d x

if the limit exists. For ϕ∈D(R)\phi \in \mathscr {D}(R), put

Λϕ=∫−∞∞ϕ(x)log⁡∣x∣dx \Lambda \phi = \int _{-\infty }^{\infty } \phi (x) \log \left|x\right| d x

Show that

Λ′ϕ=PV∫−∞∞ϕ(x)dxxΛ′′ϕ=−PV∫−∞∞ϕ(x)−ϕ(0)x2dx \begin{aligned} & \Lambda ^{\prime } \phi = P V \int _{-\infty }^{\infty } \phi (x) \frac{d x}{x} \\ & \Lambda ^{\prime \prime } \phi = -P V \int _{-\infty }^{\infty } \frac{\phi (x)-\phi (0)}{x^{2}} d x \end{aligned}
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Problem 3.6.27

Find all distributions u∈D′(Rn)u \in \mathscr {D}^{\prime }\left(\mathbb {R}^{n}\right) that satisfy at least one of the following two conditions:

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(a)

τxu=u\tau_{x} u = u for every x∈Rnx \in \mathbb {R}^{n},

(b)

Dαu=0D^{\alpha } u = 0 for every α\alpha with ∣α∣=1\left|\alpha \right| = 1.

Problem 3.7.1

Suppose AA is an invertible linear operator on Rn,f∈L1(Rn)\mathbb {R}^{n}, f \in L^{1}\left(\mathbb {R}^{n}\right), and g(x)=f(Ax)g(x) = f(A x). Express g^\hat{g} in terms of f^\hat{f}. This generalizes (d)(d) of Theorem 7.2.

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Problem 3.7.2

Is the topology of Sn\mathscr {S}_{n} induced by some invariant metric which turns the Fourier transform into an isometry of Sn\mathscr {S}_{n} onto Sn\mathscr {S}_{n}?

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Problem 3.7.3

Suppose f(x)=ex,g(x)=excos⁡(ex)f(x) = e^{x}, g(x) = e^{x} \cos \left(e^{x}\right), on the real line. Show that gg is a tempered distribution but that ff is not.

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Problem 3.7.4

By Exercise 3 there exist distributions in Rn\mathbb {R}^{n} which are not tempered. Such distributions are continuous linear functionals on D(Rn)\mathscr {D}\left(\mathbb {R}^{n}\right) which have no continuous linear extension to Sn\mathscr {S}_{n}. Explain why this does not contradict the Hahn-Banach theorem.

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Problem 3.7.5
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(a)

Construct a sequence in D(Rn)\mathscr {D}\left(\mathbb {R}^{n}\right) which converges to 0 in the topology of Sn\mathscr {S}_{n} but not in that of D(Rn)\mathscr {D}\left(\mathbb {R}^{n}\right).

(b)

Construct a sequence of polynomials which converges in the topology of D′(R1)\mathscr {D}^{\prime }\left(\mathbb {R}^{1}\right) but not in that of S1′\mathscr {S}_{1}^{\prime }.

Problem 3.7.6

Prove that the operations listed in Theorem 7.13 are continuous mappings of Sn′\mathscr {S}_{n}^{\prime } into Sn′\mathscr {S}_{n}^{\prime }.

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Problem 3.7.7

If u∈Sn′u \in \mathscr {S}_{n}^{\prime }, prove that

(τxu)∧=e−xu^ and (exu)∧=τxu^ \left(\tau _{x} u\right)^{\wedge } = e_{-x} \hat{u} \quad \text{ and } \quad \left(e_{x} u\right)^{\wedge } = \tau _{x} \hat{u}

for every x∈Rnx \in \mathbb {R}^{n}.

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Problem 3.7.8

Suppose f∈L1(Rn),f≠0,λf \in L^{1}\left(\mathbb {R}^{n}\right), f \neq 0, \lambda is a complex number, and f^=λf\hat{f} = \lambda f. What can you say about λ\lambda?

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Problem 3.7.9

Prove (a) of Theorem 7.8 directly (without using Fourier transforms).

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Problem 3.7.10

The Fourier transform of a complex Borel measure μ\mu on Rn\mathbb {R}^{n} is customarily defined to be the function μ^\hat{\mu } given by

μ^(x)=∫Rne−ix⋅tdμ(t)(x∈Rn) \hat{\mu }(x) = \int _{\mathbb {R}^{n}} e^{-i x \cdot t} d \mu (t) \quad \left(x \in \mathbb {R}^{n}\right)

Of course, μ\mu is also a tempered distribution, and as such its Fourier transform was defined in Section 7.14. Show that these two definitions are consistent. Prove that each μ^\hat{\mu } is bounded and uniformly continuous.

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Problem 3.7.11

Suppose Λ:Sn→C(Rn)\Lambda : \mathscr {S}_{n} \rightarrow C\left(\mathbb {R}^{n}\right) is continuous, linear, and τxΛ=Λτx\tau_{x} \Lambda = \Lambda \tau_{x} for every x∈Rnx \in \mathbb {R}^{n}. Does it follow that there exists u∈Sn′u \in \mathscr {S}_{n}^{\prime } such that

Λϕ=u∗ϕ \Lambda \phi = u * \phi

for every ϕ∈Sn\phi \in \mathscr {S}_{n}?

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Problem 3.7.12

If {hj}\left\{ h_{j}\right\} is an approximate identity, as in Definition 6.31, and u∈Sn′u \in \mathscr {S}_{n}^{\prime }, does it follow that u∗hj→uu * h_{j} \rightarrow u as j→∞j \rightarrow \infty, in the weak*-topology of Sn′\mathscr {S}_{n}^{\prime }?

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Problem 3.7.13

Suppose XX and YY are complete metric spaces, AA is dense in X,f:A→YX, f: A \rightarrow Y is uniformly continuous.

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(a)

Prove that ff has a unique continuous extension F:X→YF: X \rightarrow Y.

(b)

If ff is an isometry, prove that the same is true of FF, and prove that F(X)F(X) is closed in YY. (This was used in the proof of the Plancherel theorem; see also Exercise 19, Chapter 1).

Problem 3.7.14

Suppose FF is an entire function in Cn\mathbb {C}^{n}, and suppose that to each ε>0\varepsilon > 0 there correspond an integer N(ε)N(\varepsilon ) and a constant γ(ε)<∞\gamma (\varepsilon ) < \infty such that

∣F(z)∣≤γ(ε)(1+∣z∣)N(ε)eε∣Im(z)∣(z∈Cn) \left|F(z)\right| \leq \gamma (\varepsilon )\left(1+\left|z\right|\right)^{N(\varepsilon )} e^{\varepsilon \left|\mathrm{Im}\left(z\right)\right|} \quad \left(z \in \mathbb {C}^{n}\right)

Prove that FF is a polynomial.

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Problem 3.7.15

Suppose ff is an entire function in Cn,N\mathbb {C}^{n}, N is a positive integer, r≥0r \geq 0, and

∣f(z)∣≤(1+∣z∣)Ner∣Im(z)∣ for all z∈Cn∣f(x)∣≤1 for all x∈Rn \begin{array}{ll} \left|f(z)\right| \leq \left(1+\left|z\right|\right)^{N} e^{r\left|\mathrm{Im}\left(z\right)\right|} & \text{ for all } z \in \mathbb {C}^{n} \\ \left|f(x)\right| \leq 1 & \text{ for all } x \in \mathbb {R}^{n} \end{array}

Prove that then

∣f(z)∣≤er∣Im(z)∣ for all z∈Cn \left|f(z)\right| \leq e^{r\left|\mathrm{Im}\left(z\right)\right|} \quad \text{ for all } z \in \mathbb {C}^{n}

Suggestion: Fix z=x+iy∈Cnz = x+i y \in \mathbb {C}^{n}; define

gs(λ)=(1−isλ)−N−1eir∣y∣λf(x+λy) g_{s}(\lambda ) = (1-i s \lambda )^{-N-1} e^{i r\left|y\right| \lambda } f(x+\lambda y)

for λ∈C,s>0\lambda \in \mathcal{C}, s > 0, and apply the maximum modulus theorem to a large semicircular region in the upper half-plane to deduce that ∣gs(i)∣<1\left|g_{s}(i)\right| < 1. Let s→0s \rightarrow 0.

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Problem 3.7.16

In (b) of Theorem 7.23 it is not asserted that uu has order NN. The following example shows that this is not always true.

Let μ\mu be the Borel probability measure on R3\mathbb {R}^{3} which is concentrated on the unit sphere S2S^{2} and which is invariant under all rotations of S2S^{2}. Compute (by using spherical coordinates) that

μ^(x)=sin⁡∣x∣∣x∣(x∈R3) \hat{\mu }(x) = \frac{\sin \left|x\right|}{\left|x\right|} \quad \left(x \in \mathbb {R}^{3}\right)

Put u=D1μu = D_{1} \mu. Then

∣u^(x)∣=∣x1μ^(x)∣≤1(x∈R3) \left|\hat{u}(x)\right| = \left|x_{1} \hat{\mu }(x)\right| \leq 1 \quad \left(x \in \mathbb {R}^{3}\right)

Deduce from Exercise 15 that

∣u(e−z)∣≤γe∣Im(z)∣(z∈C3) \left|u\left(e_{-z}\right)\right| \leq \gamma e^{\left|\mathrm{Im}\left(z\right)\right|} \quad \left(z \in \mathbb {C}^{3}\right)

although uu is not a distribution of order 0. (Its order is 1). Find an explicit formula for the entire function u(e−z),z∈C3u\left(e_{-z}\right), z \in \mathbb {C}^{3}.

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Problem 3.7.17

Suppose uu is a distribution in Rn\mathbb {R}^{n}, with compact support KK, whose Fourier transform u^\hat{u} is a bounded function on Rn\mathbb {R}^{n}.

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(a)

Assume n=1n = 1 or n=2n = 2, and prove that ψu=0\psi u = 0 for every ψ∈C∞(Rn)\psi \in C^{\infty }\left(\mathbb {R}^{n}\right) that vanishes on KK.

(b)

Assume n=2n = 2, and assume that there is a real polynomial PP, in two variables, that vanishes on KK. Prove that Pu=0P u = 0 and that u^\hat{u} therefore satisfies the partial differential equation P(−D)u^=0P(-D) \hat{u} = 0. For example, when KK is the unit circle, then

u^+Δu^=0 \hat{u}+\Delta \hat{u} = 0

where Δ=∂2/∂x12+∂2/∂x22\Delta = \partial^{2} / \partial x_{1}^{2}+\partial^{2} / \partial x_{2}^{2} is the Laplacian.

(c)

Show, with the aid of Exercise 16 and the polynomial 1−x12−x22−x321-x_{1}^{2}-x_{2}^{2}-x_{3}^{2}, that (b)(b), hence also (a)(a), becomes false with n=3n = 3 in place of n=2n = 2.

(d)

Assume n=1,f∈L1(R),f^=0n = 1, f \in L^{1}(\mathbb {R}), \hat{f} = 0 on KK, and f^\hat{f} satisfies a Lipschitz condition of order 12\frac{1}{2}, that is, ∣f^(t)−f^(s)∣≤C∣t−s∣1/2\left|\hat{f}(t)-\hat{f}(s)\right| \leq C\left|t-s\right|^{1 / 2}. Prove that then

∫−∞∞f(x)u^(x)dx=0 \int _{-\infty }^{\infty } f(x) \hat{u}(x) d x = 0

Suggestion: For any nn, let HεH_{\varepsilon } be the set of all points outside KK whose distance from KK is less than ε>0\varepsilon > 0. Let {hε}\left\{ h_{\varepsilon }\right\} be an apprcximate identity, as in the proof of (b)(b) of Theorem 7.23, use the Plancherel theorem to obtain

∥u∗hε∥2≤∥u^∥∞ε−π/2∥h1∥2 \left\| u * h_{\varepsilon }\right\| _{2} \leq \left\| \hat{u}\right\| _{\infty } \varepsilon ^{-\pi / 2}\left\| h_{1}\right\| _{2}

and show that therefore

∣u(ϕ)∣≤∥u^∥∞∥h1∥2lim inf⁡ε→0{ε−n∫Hε∣ϕ∣2dmn}1/2 \left|u(\phi )\right| \leq \left\| \hat{u}\right\| _{\infty }\left\| h_{1}\right\| _{2} \liminf _{\varepsilon \rightarrow 0}\left\{ \varepsilon ^{-n} \int _{H_{\varepsilon }}\left|\phi \right|^{2} d m_{n}\right\} ^{1 / 2}

for any ϕ∈D(Rn)\phi \in \mathscr {D}\left(\mathbb {R}^{n}\right) that vanishes on KK. This yields (a). A slight modification yields (d); (b) follows from (a).

Problem 3.7.18

Was it necessary to introduce the function ψ\psi into the proof of Theorem 7.25? Could the proof have been simplified by setting F(x)=f(x)F(x) = f(x) on K,F(x)=0K, F(x) = 0 off K?

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Problem 3.7.19

Show that the hypotheses of Theorem 7.25 imply that DαfD^{\alpha } f is locally L2L^{2} for every multi-index α\alpha with ∣α∣≤r\left|\alpha \right| \leq r.

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Problem 3.7.20

Let f∈L2(R2)f \in L^{2}\left(\mathbb {R}^{2}\right) be the continuous function whose Fourier transform is

f^(y)=(1+∣y∣)−4{log⁡(2+∣y∣)}−1(y∈R2) \hat{f}(y) = (1+\left|y\right|)^{-4}\left\{ \log (2+\left|y\right|)\right\} ^{-1} \quad \left(y \in \mathbb {R}^{2}\right)

Since ∣y∣3f^(y)\left|y\right|^{3} \hat{f}(y) is in L2(R2)L^{2}\left(\mathbb {R}^{2}\right), Theorem 7.25 implies that f∈C(1)(R2)f \in C^{(1)}\left(\mathbb {R}^{2}\right). Show that the stronger conclusion f∈C(2)(R2)f \in C^{(2)}\left(\mathbb {R}^{2}\right) is false, by proving that

f(h,0)+f(−h,0)−2f(0,0)h2→−∞ as h→0 \frac{f(h, 0)+f(-h, 0)-2 f(0,0)}{h^{2}} \rightarrow -\infty \text{ as } h \rightarrow 0

This shows that >> cannot be replaced by ≥\geq in (1) of Theorem 7.25.

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Problem 3.7.21

Suppose uu is a distribution in Rn\mathbb {R}^{n} whose first derivatives D1u,…,DnuD_{1} u, \ldots , D_{n} u are functions in L2(Rn)L^{2}\left(\mathbb {R}^{n}\right). Prove that uu is also a function and that uu is locally L2L^{2}. (Show that "locally" cannot be omitted in the conclusion). Hint: uu is in fact the sum of an L2L^{2}-function and an entire function.

When n=1n = 1, show that uu is actually a continuous function. Show that this stronger conclusion is false when n=2n = 2. For example, the gradient of the function

u(reiθ)=log⁡log⁡(2+1r) u\left(r e^{i \theta }\right) = \log \log \left(2+\frac{1}{r}\right)

is in L2(R2)L^{2}\left(\mathbb {R}^{2}\right). See Exercise 11, Chapter 8, for the same result under weaker hypotheses.

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Problem 3.7.22

Periodic distributions, or distributions on a torus TnT^{n}, have Fourier series whose theory is somewhat simpler than that of Fourier transforms. This is mainly due to the compactness of TnT^{n} : Every distribution on TnT^{n} has compact support. In particular, tempered distributions are nothing special.

Prove the various assertions made in the following basic outline:

Tn={(eix1,…,eixn):xj real } T^{n} = \left\{ \left(e^{i x_{1}}, \ldots , e^{i x_{n}}\right): x_{j} \text{ real }\right\}

Functions ϕ\phi on TnT^{n} can be identified with functions ϕ~\tilde{\phi } on Rn\mathbb {R}^{n} that are 2π2 \pi-periodic in each variable, by setting

ϕ~(x1,…,xn)=ϕ(eix1,…,eixn) \tilde{\phi }\left(x_{1}, \ldots , x_{n}\right) = \phi \left(e^{i x_{1}}, \ldots , e^{i x_{n}}\right)

Zn\mathbb {Z}^{n} is the set (or additive group) of nn-tuples k=(k1,…,kn)k = \left(k_{1}, \ldots , k_{n}\right) of integers kjk_{j}. For k∈Znk \in \mathbb {Z}^{n}, the function eke_{k} is defined on TnT^{n} by

ek(eix1,…,eixn)=eik⋅x=exp⁡{i(k1x1+⋯+knxn)} e_{k}\left(e^{i x_{1}}, \ldots , e^{i x_{n}}\right) = e^{i k \cdot x} = \exp \left\{ i\left(k_{1} x_{1}+\cdots +k_{n} x_{n}\right)\right\}

σn\sigma_{n} is the Haar measure of TnT^{n}. If ϕ∈L1(σn)\phi \in L^{1}\left(\sigma_{n}\right), the Fourier coefficients of ϕ\phi are

ϕ^(k)=∫Tne−kϕdσn(k∈Zn) \hat{\phi }(k) = \int _{T^{n}} e_{-k} \phi d \sigma _{n} \quad \left(k \in \mathbb {Z}^{n}\right)

D(Tn)\mathscr {D}\left(T^{n}\right) is the space of all functions ϕ\phi on TnT^{n} such that ϕ~∈C∞(Rn)\tilde{\phi } \in C^{\infty }\left(\mathbb {R}^{n}\right). If ϕ∈D(Tn)\phi \in \mathscr {D}\left(T^{n}\right) then

{∑k∈Zn(1+k⋅k)N∣ϕ^(k)∣2}1/2<∞ \left\{ \sum _{k \in \mathbb {Z}^{n}}(1+k \cdot k)^{N}\left|\hat{\phi }(k)\right|^{2}\right\} ^{1 / 2} < \infty

for N=0,1,2,…N = 0,1,2, \ldots These norms define a Fréchet space topology on D(Tn)\mathscr {D}\left(T^{n}\right), which coincides with the one given by the norms

max⁡∣α∣≤Nsup⁡x∈Rn∣(Dαϕ~)(x)∣(N=0,1,2,…) \max _{\left|\alpha \right| \leq N} \sup _{x \in \mathbb {R}^{n}}\left|\left(D^{\alpha } \tilde{\phi }\right)(x)\right| \quad (N = 0,1,2, \ldots )

D′(Tn)\mathscr {D}^{\prime }\left(T^{n}\right) is the space of all continuous linear functionals on D(Tn)\mathscr {D}\left(T^{n}\right); its members are the distributions on TnT^{n}. The Fourier coefficients of any u∈D′(Tn)u \in \mathscr {D}^{\prime }\left(T^{n}\right) are defined by

u^(k)=u(e−k)(k∈Zn) \hat{u}(k) = u\left(e_{-k}\right) \quad \left(k \in \mathbb {Z}^{n}\right)

To each u∈D′(Tn)u \in \mathscr {D}^{\prime }\left(T^{n}\right) correspond an NN and a CC such that

∣u^(k)∣≤C(1+∣k∣)N(k∈Zn) \left|\hat{u}(k)\right| \leq C(1+\left|k\right|)^{N} \quad \left(k \in \mathbb {Z}^{n}\right)

Conversely, if gg is a complex function on ZnZ^{\mathbf{n}} that satisfies ∣g(k)∣≤C(1+∣k∣)N\left|g(k)\right| \leq C(1+\left|k\right|)^{N} for some CC and NN, then g=u^g = \hat{u} for some u∈D′(Tn)u \in \mathscr {D}^{\prime }\left(T^{n}\right).

There is thus a linear one-to-one correspondence between distributions on TnT^{n}, on one hand, and functions of polynomial growth on Zn\mathbb {Z}^{n}, on the other.

If E1⊂E2⊂E3⊂⋯E_{1} \subset E_{2} \subset E_{3} \subset \cdots are finite sets whose union is Zn\mathbb {Z}^{n}, and if u∈D′(Tn)u \in \mathscr {D}^{\prime }\left(T^{n}\right), the "partial sums"

∑k∈Eju^(k)ek \sum _{k \in E_{j}} \hat{u}(k) e_{k}

converge to uu as j→∞j \rightarrow \infty, in the weak*-topology of D′(Tn)\mathscr {D}^{\prime }\left(T^{n}\right). The convolution u∗vu * v of u∈D′(Tn)u \in \mathscr {D}^{\prime }\left(T^{n}\right) and v∈D′(Tn)v \in \mathscr {D}^{\prime }\left(T^{n}\right) is most easily defined as having Fourier coefficients u^(k)v^(k)\hat{u}(k) \hat{v}(k). The analogues of Theorems 6.30 and 6.37 are true; the proofs are much simpler.

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Problem 3.7.23

Modify the proof of Theorem 7.25 so that Fourier series are used in place of Fourier transforms, by replacing FF by a suitable periodic function.

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Problem 3.7.24

Put c=(2/π)1/2c = (2 / \pi )^{1 / 2}. For j=1,2,3,…j = 1,2,3, \ldots, define gjg_{j} on the real line by

g(t)={c/t if 1/j<∣t∣<j0 otherwise  g(t) = \begin{cases} c / t & \text{ if } 1 / j < \left|t\right| < j \\ 0 & \text{ otherwise }\end{cases}

Prove that {g^j}\left\{ \hat{g}_{j}\right\} is a uniformly bounded sequence of functions which converges pointwise, as j→∞j \rightarrow \infty. If f∈L2(R1)f \in L^{2}\left(\mathbb {R}^{1}\right), it follows that f∗gjf * g_{j} converges, in the L2L^{2} metric, to a function Hf∈L2H f \in L^{2}. This is the Hilbert transform of ff; formally,

(Hf)(x)=1π∫−∞∞f(t)x−tdt (H f)(x) = \frac{1}{\pi } \int _{-\infty }^{\infty } \frac{f(t)}{x-t} d t

(The integral exists, in the principal value sense, for almost every xx, but this is not so easy to prove; if ff satisfies a Lipschitz condition of order 1, for instance, the proof is trivial). Prove that

∥Hf∥2=∥f∥2 and H(Hf)=−f \left\| H f\right\| _{2} = \left\| f\right\| _{2} \quad \text{ and } \quad H(H f) = -f

for every f∈L2(R1)f \in L^{2}\left(\mathbb {R}^{1}\right). Thus HH is an L2L^{2}-isometry, of period 4. Is it true that Hf∈S1H f \in \mathscr {S}_{1} if f∈S1f \in \mathscr {S}_{1}?

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Problem 3.8.1

The following simple properties of holomorphic functions of several variables were tacitly used in this chapter. Prove them.

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(a)

If ff is entire in Cn\mathbb {C}^{n}, if w∈Cnw \in \mathbb {C}^{n}, and if ϕ(λ)=f(λw)\phi (\lambda ) = f(\lambda w), then ϕ\phi is an entire function of one complex variable.

(b)

If PP is a polynomial in Cn\mathbb {C}^{n} and if

∫Tn∣P∣dσn=0 \int _{T^{n}}\left|P\right| d \sigma _{n} = 0

then PP is identically 0. Hint: Compute ∫Tn∣P∣2dσn\int_{T^{n}}\left|P\right|^{2} d \sigma_{n}.

(c)

If PP is a polynomial (not identically 0) and gg is an entire function in Cn\mathbb {C}^{n}, then there is at most one entire function ff that satisfies Pf=gP f = g. Find generalizations of these three properties.

Problem 3.8.2

Prove the statement about convex hulls made in the last sentence of the proof of Theorem 8.4.

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Problem 3.8.3

Find a fundamental solution for the operator ∂2/∂x1∂x2\partial^{2} / \partial x_{1} \partial x_{2} in R2\mathbb {R}^{2}. (There is one that is the characteristic function of a certain subset of R2\mathbb {R}^{2}).

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Problem 3.8.4

Show that the equation

∂2u∂x12−∂2u∂x22=0 \frac{\partial ^{2} u}{\partial x_{1}^{2}}-\frac{\partial ^{2} u}{\partial x_{2}^{2}} = 0

is satisfied (in the distribution sense) by every locally integrable function uu of the form

u(x1,x2)=f(x1+x2) or u(x1,x2)=f(x1−x2) u\left(x_{1}, x_{2}\right) = f\left(x_{1}+x_{2}\right) \quad \text{ or } \quad u\left(x_{1}, x_{2}\right) = f\left(x_{1}-x_{2}\right)

and that even classical solutions (i.e., twice continuously differentiable functions) need not be in C∞C^{\infty }. Note the contrast between this and the Laplace equation.

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Problem 3.8.5

For x∈R3x \in \mathbb {R}^{3}, define f(x)=(1+∣x∣2)−1f(x) = \left(1+\left|x\right|^{2}\right)^{-1}. Show that f∈L2(R3)f \in L^{2}\left(\mathbb {R}^{3}\right) and that f^\hat{f} is a fundamental solution of the operator I−ΔI-\Delta in R3\mathbb {R}^{3}. Find f^\hat{f}, by direct computation and also by the following reasoning:

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(a)

Since ff is a radial function (i.e., one that depends only on the distance from the origin) the same is true of f^\hat{f}; see Exercise 1 of Chapter 7.

(b)

Away from the origin, (I−Δ)f^=0(I-\Delta ) \hat{f} = 0, and f^∈C∞\hat{f} \in C^{\infty }.

(c)

If F(∣y∣)=f^(y)F(\left|y\right|) = \hat{f}(y), (b) implies that FF satisfies an ordinary differential equation in (0,∞)(0, \infty ) that can easily be solved explicitly. Ans. f^(y)=(π/2)1/2∣y∣−1exp⁡(−∣y∣)\hat{f}(y) = (\pi / 2)^{1 / 2}\left|y\right|^{-1} \exp (-\left|y\right|). Do the same with Rn\mathbb {R}^{n} in place of R3\mathbb {R}^{3}; you will meet Bessel functions.

Problem 3.8.6

For 0<λ<n0 < \lambda < n and x∈Rnx \in \mathbb {R}^{n}, define

Kλ(x)=∣x∣−λ K_{\lambda }(x) = \left|x\right|^{-\lambda }

Show that

K^λ(y)=c(n,λ)Kn−λ(y)(y∈Rn)(a) \hat{K}_{\lambda }(y) = c(n, \lambda ) K_{n-\lambda }(y) \quad \left(y \in \mathbb {R}^{n}\right) \tag {a}

where

c(n,λ)=2n/2−λΓ[(n−λ)/2]Γ(λ/2) c(n, \lambda ) = \frac{2^{n / 2-\lambda } \Gamma [(n-\lambda ) / 2]}{\Gamma (\lambda / 2)}

Suggestion: If n<2λ<2n,Kλn < 2 \lambda < 2 n, K_{\lambda } is the sum of an L1L^{1}-function and an L2L^{2}-function. For these λ\lambda, Equation (a) can be deduced from the homogeneity condition

Kλ(tx)=t−λKλ(x)(x∈Rn,t>0) K_{\lambda }(t x) = t^{-\lambda } K_{\lambda }(x) \quad \left(x \in \mathbb {R}^{n}, t > 0\right)

The case 0<2λ<n0 < 2 \lambda < n follows from the inversion theorem (for tempered distributions). A passage to the limit gives the case 2λ=n2 \lambda = n. The constants c(n,λ)c(n, \lambda ) can be computed from ∫fϕ^=∫δ^ϕ\int f \hat{\phi } = \int \hat{\delta } \phi, with ϕ(x)=exp⁡(−∣x∣2/2)\phi (x) = \exp \left(-\left|x\right|^{2} / 2\right).

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Problem 3.8.7

Take n≥3n \geq 3 and λ=2\lambda = 2 in Exercise 6, and deduce that −c(n,2)Kn−2-c(n, 2) K_{n-2} is a fundamental solution of the Laplacian Δ\Delta in Rn\mathbb {R}^{n}. For example, if vv has compact support in R3\mathbb {R}^{3}, show that a solution of Δu=v\Delta u = v is given by

u(x)=−14π∫R3∣x−y∣−1v(y)dy u(x) = -\frac{1}{4 \pi } \int _{\mathbb {R}^{3}}\left|x-y\right|^{-1} v(y) d y
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Problem 3.8.8

Identify R2\mathbb {R}^{2} and C\mathbb {C} (so that z=x1+ix2z = x_{1}+i x_{2}); put

∂=∂∂x1−i∂∂x2,∂ˉ=∂∂x1+i∂∂x2 \partial = \frac{\partial }{\partial x_{1}}-i \frac{\partial }{\partial x_{2}}, \quad \bar{\partial } = \frac{\partial }{\partial x_{1}}+i \frac{\partial }{\partial x_{2}}

Show that the Fourier transform of 1/z1 / z (regarded as a tempered distribution) is −i/z-i / z. Show that this result is equivalent to the Cauchy formula

ϕ(z)=∫R2(∂ˉϕ)(w)dm2(w)w−z[ϕ∈D(R2)] \phi (z) = \int _{\mathbb {R}^{2}}(\bar{\partial } \phi )(w) \frac{d m_{2}(w)}{w-z} \quad \left[\phi \in \mathscr {D}\left(\mathbb {R}^{2}\right)\right]

Since ∂log⁡∣w∣=1/w\partial \log \left|w\right| = 1 / w and Δ=∂∂ˉ\Delta = \partial \bar{\partial }, deduce that

ϕ(z)=∫R2(Δϕ)(w)log⁡∣w−z∣dm2(w)[ϕ∈D(R2)] \phi (z) = \int _{\mathbb {R}^{2}}(\Delta \phi )(w) \log \left|w-z\right| d m_{2}(w) \quad \left[\phi \in \mathscr {D}\left(\mathbb {R}^{2}\right)\right]

Thus log⁡∣z∣\log \left|z\right| is a fundamental solution of the Laplacian in R2\mathbb {R}^{2}.

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Problem 3.8.9

Use Exercise 6 to compute that

lim⁡ε→0[ε−1−b−K^2−ε(y)]=log⁡∣y∣(y∈R2) \lim _{\varepsilon \rightarrow 0}\left[\varepsilon ^{-1}-b-\hat{K}_{2-\varepsilon }(y)\right] = \log \left|y\right| \quad \left(y \in \mathbb {R}^{2}\right)

where bb is a certain constant. Show that this leads to another proof of the last statement in Exercise 8.

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Problem 3.8.10

Suppose P(D)=D2+aD+bIP(D) = D^{2}+a D+b I. (We are now in the case n=1n = 1). Let ff and gg be solutions of P(D)u=0P(D) u = 0 which satisfy

f(0)=g(0) and f′(0)−g′(0)=1 f(0) = g(0) \quad \text{ and } \quad f^{\prime }(0)-g^{\prime }(0) = 1

Define

G(x)={f(x) if x≤0g(x) if x>0 G(x) = \begin{cases} f(x) & \text{ if } x \leq 0 \\ g(x) & \text{ if } x > 0\end{cases}

and put

Λϕ=−∫−∞∞ϕ(x)G(x)dx[ϕ∈D(R)] \Lambda \phi = -\int _{-\infty }^{\infty } \phi (x) G(x) d x \quad [\phi \in \mathscr {D}(R)]

Prove that Λ\Lambda is a fundamental solution of P(D)P(D).

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Problem 3.8.11

Suppose uu is a distribution in Rn\mathbb {R}^{n} whose first derivatives D1u,…,DnuD_{1} u, \ldots , D_{n} u are locally L2L^{2}. Prove that uu is then locally L2L^{2}. Hint: If ψ∈D(Rn)\psi \in \mathscr {D}\left(\mathbb {R}^{n}\right) is 1 in a neighborhood of the origin and if ΔE=δ\Delta E = \delta, then Δ(ψE)−δ∈D(Rn)\Delta (\psi E)-\delta \in \mathscr {D}\left(\mathbb {R}^{n}\right). Hence

u−∑i=1n(Diu)∗Di(ψE) u-\sum _{i = 1}^{n}\left(D_{i} u\right) * D_{i}(\psi E)

is in C∞(Rn)C^{\infty }\left(\mathbb {R}^{n}\right). Each Di(ψE)D_{i}(\psi E) is an L1L^{1}-function with compact support.

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Problem 3.8.12

Suppose uu is a distribution in Rn\mathbb {R}^{n} whose Laplacian Δu\Delta u is a continuous function. Prove that uu is then a continuous function. Hint: As in Exercise 11,

u−(ψE)∗(Δu)∈C∞(Rn) u-(\psi E) *(\Delta u) \in C^{\infty }\left(\mathbb {R}^{n}\right)
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Problem 3.8.13

Prove analogues of Exercises 11 and 12, with Rn\mathbb {R}^{n} replaced by an arbitrary open set Ω\Omega.

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Problem 3.8.14

Show, under the hypotheses of Exercise 12, that

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(a)

∂2u/∂x12\partial^{2} u / \partial x_{1}^{2} is locally L2L^{2}, but

(b)

∂2u/∂x12\partial^{2} u / \partial x_{1}^{2} need not be a continuous function.

Outline of (b)(b) for periodic distributions in R2\mathbb {R}^{2} (Exercise 22, Chapter 7): If g∈C(T2)g \in C\left(T^{2}\right) has Fourier coefficients g^(m,n)\hat{g}(m, n) and if ff is defined by

f^(m,n)=(1+m2+n2)−1g^(m,n) \hat{f}(m, n) = \left(1+m^{2}+n^{2}\right)^{-1} \hat{g}(m, n)

then f∈C(T2)f \in C\left(T^{2}\right) and Δf=f−g∈C(T2)\Delta f = f-g \in C\left(T^{2}\right), since ∑∣f^(m,n)∣<∞\sum \left|\hat{f}(m, n)\right| < \infty. The Fourier coefficients of ∂2f/∂x12\partial^{2} f / \partial x_{1}^{2} are −m2f^(m,n)-m^{2} \hat{f}(m, n). If ∂2f/∂x12\partial^{2} f / \partial x_{1}^{2} were continuous for every g∈C(T2)g \in C\left(T^{2}\right), then (∂2f/∂x12)(0,0)\left(\partial^{2} f / \partial x_{1}^{2}\right)(0,0) would be a continuous linear functional of gg. Hence there would be a complex Borel measure μ\mu on T2T^{2}, with Fourier coefficients

μ^(m,n)=m21+m2+n2 \hat{\mu }(m, n) = \frac{m^{2}}{1+m^{2}+n^{2}}

The next exercise shows that no such measure exists.

Problem 3.8.15

If μ\mu is a complex Borel measure on T2T^{2}, and if

γ(A,B)=1(2A+1)(2B+1)∑n=−AA∑m=−BBμ^(m,n) \gamma (A, B) = \frac{1}{(2 A+1)(2 B+1)} \sum _{n = -A}^{A} \sum _{m = -B}^{B} \hat{\mu }(m, n)

prove that

lim⁡A→∞[lim⁡B→∞γ(A,B)]=lim⁡B→∞[lim⁡A→∞γ(A,B)] \lim _{A \rightarrow \infty }\left[\lim _{B \rightarrow \infty } \gamma (A, B)\right] = \lim _{B \rightarrow \infty }\left[\lim _{A \rightarrow \infty } \gamma (A, B)\right]

Suggestion: If DA(t)=(2A+1)−1∑−AAeintD_{A}(t) = (2 A+1)^{-1} \sum_{-A}^{A} e^{i n t}, then DA(x)=1D_{A}(x) = 1 if x=0x = 0, DA(x)→0D_{A}(x) \rightarrow 0 otherwise, and

γ(A,B)=∫T2DA(x)DB(y)dμ(x,y) \gamma (A, B) = \int _{T^{2}} D_{A}(x) D_{B}(y) d \mu (x, y)

Conclude that each of the two iterated limits exists and that both are equal to μ({0,0})\mu (\left\{ 0,0\right\} ).

If μ\mu were as in Exercise 14, one of the iterated limits would be 1, the other 0.

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Problem 3.8.16

Suppose LL is an elliptic linear operator in some open set Ω⊂Rn\Omega \subset \mathbb {R}^{n}, and suppose that the order of LL is odd.

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(a)

Prove that then n=1n = 1 or n=2n = 2.

(b)

If n=2n = 2, prove that the coefficients of the characteristic polynomial of LL cannot all be real.

In view of (a), the Cauchy-Riemann operator is not a very typical example of an elliptic operator.

Problem 3.9.1

Prove the theorem of Tauber stated in Section 9.1.

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Problem 3.9.2

Suppose ϕ∈L∞(Rn)\phi \in L^{\infty }\left(\mathbb {R}^{n}\right) and the support of the distribution ϕ^\hat{\phi } consists of kk distinct points s1,…,sks_{1}, \ldots , s_{k}. Construct suitable functions ψ1,…,ψk\psi_{1}, \ldots , \psi_{k} such that (ϕ∗ψj)∧\left(\phi * \psi_{j}\right)^{\wedge } has the singleton {sj}\left\{ s_{j}\right\} as support, and conclude that ϕ\phi is a trigonometric polynomial, namely,

ϕ(x)=a1eis1⋅x+⋯+akeisk⋅x (a.e).  \phi (x) = a_{1} e^{i s_{1} \cdot x}+\cdots +a_{k} e^{i s_{k} \cdot x} \quad \text{ (a.e). }

(The case k=1k = 1 is done in the proof of Theorem 9.13).

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Problem 3.9.3

Suppose YY is a closed translation-invariant subspace of L1(Rn)L^{1}\left(\mathbb {R}^{n}\right) such that Z(Y)Z(Y) consists of kk distinct points. (The notation is as in Theorem 9.3). Use Exercise 2 to prove that YY has codimension kk in L1(Rn)L^{1}\left(\mathbb {R}^{n}\right), and conclude from this that YY consists of exactly those f∈L1(Rn)f \in L^{1}\left(\mathbb {R}^{n}\right) whose Fourier transforms are 0 at every point of Z(Y)Z(Y).

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Problem 3.9.4

Prove the following analogue of (a) of Theorem 9.7: If ϕ∈L∞(Rn)\phi \in L^{\infty }\left(\mathbb {R}^{n}\right), and if to every t∈Rnt \in \mathbb {R}^{n} corresponds a function Kt∈L1(Rn)K_{t} \in L^{1}\left(\mathbb {R}^{n}\right) such that K^t(t)≠0\hat{K}_{t}(t) \neq 0 and (Kt∗ϕ)(x)→0\left(K_{t} * \phi \right)(x) \rightarrow 0 as ∣x∣→∞\left|x\right| \rightarrow \infty, then (f∗ϕ)(x)→0(f * \phi )(x) \rightarrow 0 as ∣x∣→∞\left|x\right| \rightarrow \infty, for every f∈L1(Rn)f \in L^{1}\left(\mathbb {R}^{n}\right).

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Problem 3.9.5

Assume K∈L1(Rn)K \in L^{1}\left(\mathbb {R}^{n}\right) and K^\hat{K} has at least one zero in Rn\mathbb {R}^{n}. Show that then there exists ϕ∈L∞(Rn)\phi \in L^{\infty }\left(\mathbb {R}^{n}\right) such that (K∗ϕ)(x)=0(K * \phi )(x) = 0 for every x∈Rnx \in \mathbb {R}^{n}, although ϕ\phi does not satisfy the conclusion of (a) of Theorem 9.7.

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Problem 3.9.6

If ϕ(x)=sin⁡(x2),−∞<x<∞\phi (x) = \sin \left(x^{2}\right),-\infty < x < \infty, show that

lim⁡∣x∣→∞(f∗ϕ)(x)=0 \lim _{\left|x\right| \rightarrow \infty }(f * \phi )(x) = 0

for every f∈L1(R)f \in L^{1}(\mathbb {R}), although the conclusion of (b)(b) of Theorem 9.7 does not hold.

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Problem 3.9.7

For α>0\alpha > 0, let fαf_{\alpha } be the characteristic function of the interval [0,α][0, \alpha ]. Define fβf_{\beta } in the same way; put g=fα+fβg = f_{\alpha }+f_{\beta }. Prove that the set of all finite linear combinations of translates of gg is dense in L1(R)L^{1}(\mathbb {R}) if and only if β/α\beta / \alpha is irrational.

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Problem 3.9.8

If α>0\alpha > 0 and αx=1\alpha x = 1, prove that

1−α<α[x]≤1 1-\alpha < \alpha [x] \leq 1

and deduce from this that exK(x)e^{x} K(x) is bounded, as asserted in the proof of Theorem 9.12.

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Problem 3.9.9

Let QQ denote the set of all rational numbers. Let μ\mu be a probability measure on RR that is concentrated on QQ, and let ϕ\phi be the characteristic function of QQ. Show that ϕ(x)=(ϕ∗μ)(x)\phi (x) = (\phi * \mu )(x) for every x∈Rx \in R, although ϕ\phi is not constant. (Compare with Theorem 9.13). What other sets could be used in place of QQ to achieve the same effect?

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Problem 3.9.10

Special cases of the following facts were used in Theorem 9.15. Prove them.

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(a)

If ϕ∈L∞(Rn)\phi \in L^{\infty }\left(\mathbb {R}^{n}\right) and k∈L1(Rn)k \in L^{1}\left(\mathbb {R}^{n}\right), then k∗ϕk * \phi is uniformly continuous.

(b)

If {ϕj}\left\{ \phi_{j}\right\} is a sequence of slowly oscillating functions on Rn\mathbb {R}^{n} that converges uniformly to a function ϕ\phi, then ϕ\phi is slowly oscillating.

(c)

If μ\mu and λ\lambda are complex Borel measures on Rn\mathbb {R}^{n}, then

∥(μ∗λ)s∥≤∥μs∥∥λs∥ \left\| (\mu * \lambda )_{s}\right\| \leq \left\| \mu _{s}\right\| \left\| \lambda _{s}\right\|
Problem 3.9.11

Put ψ(x)=cos⁡(∣x∣1/3)\psi (x) = \cos \left(\left|x\right|^{1 / 3}\right) and define

f(x)=ψ(x)−12∫−11ψ(x−y)dy(−∞<x<∞) f(x) = \psi (x)-\frac{1}{2} \int _{-1}^{1} \psi (x-y) d y \quad (-\infty < x < \infty )

Prove that f∈(L1∩C0)(R)f \in \left(L^{1} \cap C_{0}\right)(R) but that no bounded solution of the equation

ϕ(x)−12∫−11ϕ(x−y)dy=f(x) \phi (x)-\frac{1}{2} \int _{-1}^{1} \phi (x-y) d y = f(x)

has limits at +∞+\infty or at −∞-\infty. (This illustrates the relevance of the condition M≠0M \neq 0 in Theorem 9.15).

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Problem 3.9.12

Let μ\mu be a probability measure concentrated on the integers. Prove that every function ϕ\phi on RR which is periodic with period 1 satisfies ϕ−ϕ∗μ=0\phi -\phi * \mu = 0. (This is relevant to Theorems 9.13 and 9.15).

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Problem 3.9.13

Assume ϕ∈L∞(0,∞)\phi \in L^{\infty }(0, \infty ),

∫0∞∣K(x)∣dxx<∞,∫0∞∣H(x)∣dxx<∞∫0∞K(x)x−itdxx≠0 for −∞<t<∞ \begin{array}{ll} \int _{0}^{\infty }\left|K(x)\right| \frac{d x}{x} < \infty , & \int _{0}^{\infty }\left|H(x)\right| \frac{d x}{x} < \infty \\ \int _{0}^{\infty } K(x) x^{-i t} \frac{d x}{x} \neq 0 & \text{ for }-\infty < t < \infty \end{array}

and

lim⁡x→∞∫0∞K(xu)ϕ(u)duu=0 \lim _{x \rightarrow \infty } \int _{0}^{\infty } K\left(\frac{x}{u}\right) \phi (u) \frac{d u}{u} = 0

Prove that

lim⁡x→∞∫0∞H(xu)ϕ(u)duu=0 \lim _{x \rightarrow \infty } \int _{0}^{\infty } H\left(\frac{x}{u}\right) \phi (u) \frac{d u}{u} = 0

This is an analogue of (a) of Theorem 9.7. How would "slowly oscillating" have to be defined to obtain the corresponding analog of (b) of Theorem 9.7?

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Problem 3.9.14

Complete the details in the following outline of Wiener's proof of Littlewood's theorem. Assume ∣nan∣≤1,f(r)=∑0∞anrn\left|n a_{n}\right| \leq 1, f(r) = \sum_{0}^{\infty } a_{n} r^{n}, and f(r)→0f(r) \rightarrow 0 as r→1r \rightarrow 1. If sn=a0+⋯+ans_{n} = a_{0}+\cdots +a_{n}, it is to be proved that sn→0s_{n} \rightarrow 0 as n→∞n \rightarrow \infty.

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(a)

∣sn−f(1−1/n)∣<2\left|s_{n}-f(1-1 / n)\right| < 2. Hence {sn}\left\{ s_{n}\right\} is bounded.

(b)

If ϕ(x)=sn\phi (x) = s_{n} on [n,n+1)[n, n+1) and 0<x<y0 < x < y, then

∣ϕ(y)−ϕ(x)∣≤y+1−xx \left|\phi (y)-\phi (x)\right| \leq \frac{y+1-x}{x}
(c)

∫0∞xe−xtϕ(t)dt=f(e−x)→0\int_{0}^{\infty } x e^{-x t} \phi (t) d t = f\left(e^{-x}\right) \rightarrow 0 as x→0x \rightarrow 0. Hence

lim⁡x→∞∫0∞K(xu)ϕ(u)duu=0 \lim _{x \rightarrow \infty } \int _{0}^{\infty } K\left(\frac{x}{u}\right) \phi (u) \frac{d u}{u} = 0

if

K(x)=(1x)exp⁡(−1x) K(x) = \left(\frac{1}{x}\right) \exp \left(-\frac{1}{x}\right)
(d)

∫0∞K(x)x−itdxx=Γ(1+it)≠0\int_{0}^{\infty } K(x) x^{-i t} \frac{d x}{x} = \Gamma (1+i t) \neq 0 if tt is real.

(e)

Put H(x)=1/(εx)H(x) = 1 /(\varepsilon x) if (1+ε)−1<x<1,H(x)=0(1+\varepsilon )^{-1} < x < 1, H(x) = 0 otherwise. Conclude that

lim⁡x→∞1εx∫x(1+ε)xϕ(y)dy=0 \lim _{x \rightarrow \infty } \frac{1}{\varepsilon x} \int _{x}^{(1+\varepsilon ) x} \phi (y) d y = 0
(f)

By (b) and (e), lim⁡x→∞ϕ(x)=0\lim_{x \rightarrow \infty } \phi (x) = 0. Note: If nan→0n a_{n} \rightarrow 0 is assumed to hold, then a modification of step (a)(a) is all that is needed for the proof.

Problem 3.9.15

Let YY be a closed subspace of L1(Rn)L^{1}\left(\mathbb {R}^{n}\right). Prove that YY is translation-invariant if and only if f∗g∈Yf * g \in Y whenever f∈Yf \in Y and g∈L1(Rn)g \in L^{1}\left(\mathbb {R}^{n}\right).

The closed translation invariant subspaces of L1(Rn)L^{1}\left(\mathbb {R}^{n}\right) are thus exactly the same as the closed ideals in the convolution algebra L1(Rn)L^{1}\left(\mathbb {R}^{n}\right).

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