Section 12.3

Hilbert–Schmidt theorem

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Problem 12.78

Prove Theorem 12.3.

Theorem 12.3 (D. Hilbert, 1906; E. Schmidt, 1907): Let HH be an infinite-dimensional separable Hilbert space and A=A∗∈K(H)A = A^{*} \in \mathcal{K}(H). Then there exists an orthonormal basis {en}n=1∞\left\{ e_{n}\right\}_{n = 1}^{\infty } of HH consisting of eigenvectors of AA: Aen=λnenA e_{n} = \lambda_{n} e_{n}. The nonzero eigenvalues are real and can be numbered in nonincreasing order of absolute value: ∣λ1∣⩾∣λ2∣⩾…⩾∣λn∣⩾…\left|\lambda_{1}\right| \geqslant \left|\lambda_{2}\right| \geqslant \ldots \geqslant \left|\lambda_{n}\right| \geqslant \ldots, and moreover ∣λ1∣=∥A∥\left|\lambda_{1}\right| = \left\| A\right\| and lim⁡n→∞λn=0\lim_{n \rightarrow \infty } \lambda_{n} = 0.

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Problem 12.79

(D. Hilbert, 1906; E. Schmidt, 1907). Prove that in a separable Hilbert space a compact operator can be represented in the form

Ax=∑i=1Nsi(A)(x,ψi)φi A x = \sum _{i = 1}^{N} s_{i}(A)\left(x, \psi _{i}\right) \varphi _{i}

where N⩽∞,{ψi}N \leqslant \infty ,\left\{ \psi_{i}\right\} is an orthonormal basis, {φi}\left\{ \varphi_{i}\right\} is an orthonormal system.

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Problem 12.80

Let HH be a separable Hilbert space, A∈K(H)A \in \mathcal{K}(H). Prove that the numbers sk(A)s_{k}(A) are the distances from the operator AA to the set of all (k−1)(k-1)-dimensional operators, i.e.,

sk(A)=inf⁡rank⁡Pk=k−1∥A−Pk∥ s_{k}(A) = \inf _{\operatorname {rank} P_{k} = k-1}\left\| A-P_{k}\right\|

In particular, s1=∥A∥s_{1} = \left\| A\right\|.

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Problem 12.81

(Courant-Fischer variational principle). Prove that for every compact self-adjoint nonnegative operator AA in a Hilbert space HH the equalities

λn=min⁡{max⁡{(Ax,x):x⊥X,∥x∥=1}:dim⁡X=n−1} \lambda _{n} = \min \left\{ \max \left\{ (A x, x): x \perp X,\left\| x\right\| = 1\right\} : \operatorname {dim} X = n-1\right\}

hold, where λn\lambda_{n} are the eigenvalues of the operator AA, numbered in non-increasing order counting multiplicity, and the minimum is taken over all subspaces of dimension n−1n-1.

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Problem 12.82

Let AA and BB be compact self-adjoint operators in a Hilbert space and 0⩽A⩽B0 \leqslant A \leqslant B. Prove that λn(A)⩽λn(B)\lambda_{n}(A) \leqslant \lambda_{n}(B), where λn\lambda_{n} are the eigenvalues, numbered in non-increasing order counting multiplicity.

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Problem 12.83

Let AA and BB be compact operators in a Hilbert space HH, with Im⁡A⊂Im⁡B\operatorname {Im} A \subset \operatorname {Im} B. Prove that there exists a number C>0C > 0 such that sn(A)⩽Csn(B)s_{n}(A) \leqslant C s_{n}(B) for all n∈Nn \in \mathbb {N}.

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Problem 12.84

Let A∈B(L2[0,1])A \in \mathcal{B}\left(L_{2}[0,1]\right) and Im⁡A⊂W˙21[0,1]\operatorname {Im} A \subset \dot{W}_{2}^{1}[0,1]. Prove that A∈K(L2[0,1])A \in \mathcal{K}\left(L_{2}[0,1]\right) and sn(A)⩽Cn−1s_{n}(A) \leqslant C n^{-1} for some C>0C > 0 and every n∈Nn \in \mathbb {N}.

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Problem 12.85

Given a sequence sk⩾0,sk↘0s_{k} \geqslant 0, s_{k} \searrow 0. Prove that there exists an operator A∈K(l2)A \in \mathcal{K}\left(l_{2}\right) such that sk(A)=sks_{k}(A) = s_{k} for every k⩾1k \geqslant 1.

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Problem 12.86

Let HH be an infinite-dimensional separable Hilbert space, A∈K(H),{sk}1∞A \in \mathcal{K}(H),\left\{ s_{k}\right\}_{1}^{\infty } the ss-numbers of the operator A,{en}1∞A,\left\{ e_{n}\right\}_{1}^{\infty } an arbitrary orthonormal basis in HH. Prove that ∑k=1∞sk2=∑n=1∞∥Aen∥2\sum_{k = 1}^{\infty } s_{k}^{2} = \sum_{n = 1}^{\infty }\left\| A e_{n}\right\|^{2} (i.e., either both series diverge, or both series converge and their sums are equal).

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Problem 12.87

Let H1H_{1} and H2H_{2} be separable Hilbert spaces, A∈K(H1,H2),{en}1∞A \in \mathcal{K}\left(H_{1}, H_{2}\right),\left\{ e_{n}\right\}_{1}^{\infty } an orthonormal basis in H1H_{1}. Prove that ∥A∥2⩽∑n=1∞∥Aen∥2\left\| A\right\|^{2} \leqslant \sum_{n = 1}^{\infty }\left\| A e_{n}\right\|^{2}.

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Problem 12.88

Let H1H_{1} and H2H_{2} be separable Hilbert spaces, A∈B(H1,H2),{en}1∞A \in \mathcal{B}\left(H_{1}, H_{2}\right),\left\{ e_{n}\right\}_{1}^{\infty } an orthonormal basis in H1H_{1}. Prove that if the series ∑n=1∞∥Aen∥2\sum_{n = 1}^{\infty }\left\| A e_{n}\right\|^{2} converges, then AA is compact.

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Problem 12.89

Let HH be an infinite-dimensional separable Hilbert space, A∈K(H)A \in \mathcal{K}(H). Prove the equivalence of the following statements:

  1. A∈S2(H)A \in \mathcal{S}_{2}(H), i.e., the series ∑k=1∞sk2(A)\sum_{k = 1}^{\infty } s_{k}^{2}(A) converges;

  2. for some orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } in the space HH the series ∑n=1∞∥Aen∥2\sum_{n = 1}^{\infty }\left\| A e_{n}\right\|^{2} converges;

  3. for every orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } in the space HH the series ∑n=1∞∥Aen∥2\sum_{n = 1}^{\infty }\left\| A e_{n}\right\|^{2} converges;

  4. for the matrix entries ajk=(Aej,ek)a_{j k} = \left(A e_{j}, e_{k}\right) of the operator AA in some orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } of the space HH the inequality ∑j,k=1∞∣ajk∣2<∞\sum_{j, k = 1}^{\infty }\left|a_{j k}\right|^{2} < \infty holds;

  5. for the matrix entries ajk=(Aej,ek)a_{j k} = \left(A e_{j}, e_{k}\right) of the operator AA in an arbitrary orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } of the space HH the inequality ∑j,k=1∞∣ajk∣2<∞\sum_{j, k = 1}^{\infty }\left|a_{j k}\right|^{2} < \infty holds. Prove that if the operator AA satisfies these conditions, then the sums of all the indicated series coincide.

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Problem 12.90

Let HH be a separable infinite-dimensional Hilbert space. Prove that the set S2(H)\mathcal{S}_{2}(H) is a non-closed (in the norm of B(H)\mathcal{B}(H)) linear subspace of the space K(H)\mathcal{K}(H).

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Problem 12.91

Let HH be a separable infinite-dimensional Hilbert space. Prove that the norm in S2(H)\mathcal{S}_{2}(H) is generated by the inner product

(A,B)S2(H)=∑j,k=1∞ajkbˉjk (A, B)_{\mathcal{S}_{2}(H)} = \sum _{j, k = 1}^{\infty } a_{j k} \bar{b}_{j k}

where ajk=(Aej,ek)a_{j k} = \left(A e_{j}, e_{k}\right) and bjk=(Bej,ek)b_{j k} = \left(B e_{j}, e_{k}\right) are the matrix entries of the operators AA and BB in an arbitrary orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } of the space HH. Prove that the same inner product can be given by the rule

(A,B)S2(H)=∑k=1∞sk(A∗B) (A, B)_{\mathcal{S}_{2}(H)} = \sum _{k = 1}^{\infty } s_{k}\left(A^{*} B\right)
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Problem 12.92

Let HH be a separable Hilbert space. Prove that S2(H)\mathcal{S}_{2}(H) is a Hilbert space with the inner product defined in the previous problem.

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Problem 12.93

Prove that an operator AA in the space L2[0,1]L_{2}[0,1] is a Hilbert-Schmidt operator if and only if

(Ax)(t)=∫01K(t,s)x(s)ds (A x)(t) = \int _{0}^{1} K(t, s) x(s) d s

where K∈L2([0,1]2)K \in L_{2}\left([0,1]^{2}\right). Prove that the map A↦KA \mapsto K is a unitary isomorphism of the spaces S2(L2[0,1])\mathcal{S}_{2}\left(L_{2}[0,1]\right) and L2([0,1]2)L_{2}\left([0,1]^{2}\right) (in particular, ∥A∥S2(L2[0,1])2=∫01∫01∣K(x,t)∣2dxdt\left\| A\right\|_{\mathcal{S}_{2}\left(L_{2}[0,1]\right)}^{2} = \int_{0}^{1} \int_{0}^{1}|K(x, t)|^{2} d x d t).

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Problem 12.94

Prove that every bounded linear operator in the space L2[0,1]L_{2}[0,1] has the form

(Ax)(t)=ddt∫01K(t,s)x(s)ds (A x)(t) = \frac{d}{d t} \int _{0}^{1} K(t, s) x(s) d s

for some function K∈L2([0,1]2)K \in L_{2}\left([0,1]^{2}\right).

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Problem 12.95

Prove that the class Sp⁡(X)\operatorname {Sp}(X) of nuclear operators in a Banach space XX (see Definition 11.2) coincides with the class S1(H)\mathcal{S}_{1}(H), if the space X=HX = H is Hilbert.

Definition 11.2: Let XX and YY be Banach spaces. An operator A∈B(X,Y)A \in \mathcal{B}(X, Y) is called nuclear, or a trace-class operator (A∈Sp⁡(X,Y)A \in \operatorname {Sp}(X, Y)), if there exist one-dimensional operators Ak∈B(X,Y)A_{k} \in \mathcal{B}(X, Y) such that A=∑k=1∞AkA = \sum_{k = 1}^{\infty } A_{k}, where the series converges absolutely in B(X,Y)\mathcal{B}(X, Y).

Here (Definition 12.7), for A∈K(H)A \in \mathcal{K}(H) the ss-numbers of AA are sn(A):=λn(A∗A)s_{n}(A) := \sqrt{\lambda_{n}\left(A^{*} A\right)}, n=1,2,…n = 1,2, \ldots (numbered in nonincreasing order, counting multiplicity), and A∈S1(H)A \in \mathcal{S}_{1}(H) if {sn}n=1∞∈l1\left\{ s_{n}\right\}_{n = 1}^{\infty } \in l_{1}.

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Problem 12.96

Let HH be a separable Hilbert space and A∈S1(H)A \in \mathcal{S}_{1}(H). Prove that for an arbitrary orthonormal basis {ek}k=1∞\left\{ e_{k}\right\}_{k = 1}^{\infty } the series ∑k=1∞(Aek,ek)\sum_{k = 1}^{\infty }\left(A e_{k}, e_{k}\right) converges, and its sum does not depend on the choice of the basis {ek}k=1∞\left\{ e_{k}\right\}_{k = 1}^{\infty }.

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Problem 12.97

Prove that for an operator A∈S1(H)=Sp⁡(H)A \in \mathcal{S}_{1}(H) = \operatorname {Sp}(H) the equalities

∥A∥Sp⁡(H)=∑k=1∞sk(A)=sup⁡U− unitary (∑k=1∞(UAek,ek)), \left\| A\right\| _{\operatorname {Sp}(H)} = \sum _{k = 1}^{\infty } s_{k}(A) = \sup _{U-\text{ unitary }}\left(\sum _{k = 1}^{\infty }\left(U A e_{k}, e_{k}\right)\right),

hold, where {ek}k=1∞\left\{ e_{k}\right\}_{k = 1}^{\infty } is an arbitrary orthonormal basis (for the definition of ∥A∥Sp(H)\left\| A\right\|_{\mathrm{Sp}(H)} see problem 11.27).

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Problem 12.98

Let HH be a separable Hilbert space. Prove that Sp(H)\mathcal{S}_{p}(H) are linear subspaces of K(H)\mathcal{K}(H) and of B(H)\mathcal{B}(H). Prove that Sp(H)\mathcal{S}_{p}(H) are non-closed two-sided ideals in B(H)\mathcal{B}(H).

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Problem 12.99

Let A,B∈S2(H)A, B \in \mathcal{S}_{2}(H). Prove that AB∈S1(H)A B \in \mathcal{S}_{1}(H).

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Problem 12.100

Let TT be an integral operator in the space L2[0,1]L_{2}[0,1], (Tx)(t)=∫01K(t,s)x(s)ds(T x)(t) = \int_{0}^{1} K(t, s) x(s) d s, where K(⋅,⋅)∈L2([0,1]2)K(\cdot , \cdot ) \in L_{2}\left([0,1]^{2}\right) and for almost every s∈[0,1]s \in [0,1] the function t↦K(t,s)t \mapsto K(t, s) satisfies the Lipschitz condition: ∣K(t2,s)−K(t1,s)∣⩽C(s)∣t2−t1∣\left|K\left(t_{2}, s\right)-K\left(t_{1}, s\right)\right| \leqslant C(s)\left|t_{2}-t_{1}\right| for all t1,t2∈[0,1]t_{1}, t_{2} \in [0,1], where the function C(⋅)∈L2[0,1]C(\cdot ) \in L_{2}[0,1]. Prove that TT is a nuclear operator. Prove that if the function KK is moreover continuous on the square [0,1]2[0,1]^{2}, then tr⁡(T)=∫01K(t,t)dt\operatorname {tr}(T) = \int_{0}^{1} K(t, t) d t.

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Problem 12.101

(T. Carleman's example). Give an example of a non-nuclear integral operator in the space L2[0,1]L_{2}[0,1] with continuous kernel.

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Problem 12.102

Do there exist:

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(a)

a nuclear operator AA and an orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } in a Hilbert space such that ∑n=1∞∥Aen∥=+∞\sum_{n = 1}^{\infty }\left\| A e_{n}\right\| = +\infty;

(b)

a bounded but non-nuclear operator AA and an orthonormal basis {en}1∞\left\{ e_{n}\right\}_{1}^{\infty } such that (Aen,en)=0\left(A e_{n}, e_{n}\right) = 0 for all n∈Nn \in \mathbb {N} and hence ∑n=1∞(Aen,en)<∞\sum_{n = 1}^{\infty }\left(A e_{n}, e_{n}\right) < \infty?

Problem 12.103

Let HH be a separable Hilbert space and A∈K(H),A⩾0A \in \mathcal{K}(H), A \geqslant 0. Let λk(A)\lambda_{k}(A) be the eigenvalues of the operator AA, numbered in non-increasing order. Prove that λk(A)=sk(A)\lambda_{k}(A) = s_{k}(A).

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Problem 12.104

Let AA and BB be compact operators in a Hilbert space HH, with Im⁡A⊂Im⁡B\operatorname {Im} A \subset \operatorname {Im} B. Prove that if B∈Sp(H)B \in \mathcal{S}_{p}(H), then A∈Sp(H)A \in \mathcal{S}_{p}(H) as well.

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Problem 12.105

Find the norm of the integration operator

(Ax)(t)=∫0tx(s)ds (A x)(t) = \int _{0}^{t} x(s) d s

in L2[0,1]L_{2}[0,1]:

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(a)

using problem 12.80;

(b)

by expanding the function x(s)x(s) in a series with respect to the system {cos⁡(π(k−1/2)s)}1∞\left\{ \cos (\pi (k-1 / 2) s)\right\}_{1}^{\infty } (see problem 3.50).

Problem 12.106

Find the polar decomposition A=WSA = W S for the operator from problem 12.105.

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Problem 12.107

Find the norms of the operators in L2[−b,b]L_{2}[-b, b]:

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(a)

(Ax)(t)=∫−btx(s)ds(A x)(t) = \int_{-b}^{t} x(s) d s;

(b)

(Ax)(t)=∫tbx(s)ds(A x)(t) = \int_{t}^{b} x(s) d s;

(c)

(Ax)(t)=∫0tx(s)ds(A x)(t) = \int_{0}^{t} x(s) d s.

Problem 12.108

Find the spectrum of the integral operators in L2[0,π]L_{2}[0, \pi ] with kernel

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(a)

K(t,s)=∑n=1∞2−nsin⁡ntsin⁡nsK(t, s) = \sum_{n = 1}^{\infty } 2^{-n} \sin n t \sin n s;

(b)

K(t,s)=∑n=0∞2−ncos⁡ntcos⁡nsK(t, s) = \sum_{n = 0}^{\infty } 2^{-n} \cos n t \cos n s;

(c)

K(t,s)=∑n=1∞2−ncos⁡ntcos⁡nsK(t, s) = \sum_{n = 1}^{\infty } 2^{-n} \cos n t \cos n s.

Problem 12.109

Find the spectrum of the integral operators in L2[0,1]L_{2}[0,1] with kernel

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(a)

K(t,s)=min⁡(t,s)K(t, s) = \min (t, s);

(b)

K(t,s)=max⁡(t,s)K(t, s) = \max (t, s) (compare with problem 11.96). Determine to which Neumann-Schatten classes these operators belong.