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Approximation numbers of composition operators on the Hardy space of the ball and of the polydisk
Daniel Li, Hervé Queffélec, Luis Rodríguez-Piazza
To cite this version:
Daniel Li, Hervé Queffélec, Luis Rodríguez-Piazza. Approximation numbers of composition operators
on the Hardy space of the ball and of the polydisk. 2015. �hal-01146030�
Approximation numbers of composition operators on the Hardy space of the ball
and of the polydisk
Daniel Li, Hervé Queffélec, Luis Rodríguez-Piazza ∗
April 27, 2015
Abstract. We give general estimates for the approximation numbers of compo- sition operators on the Hardy space on the ball B d and the polydisk D d . Mathematics Subject Classification 2010. Primary: 47B33 – Secondary:
32A07 – 32A35 – 32A70 – 46E22 – 47B07
Key-words. approximation numbers; bounded symmetric domain; composi- tion operator; Hardy space; polydisk; Reinhardt domain; several complex vari- ables
1 Introduction
This work is an attempt to investigate approximation numbers of compo- sition operators on the Hardy space H 2 (Ω) where Ω is an open subset of C d , i.e. when we work with d complex variables instead of one. In fact, we will essentially consider the two cases when Ω = B d is the unit ball of C d endowed with its usual hermitian norm k z k = P d
j=1 | z j | 2 1/2
and Ω = D d is the unit ball of C d endowed with the sup-norm k z k
∞= sup d j=1 | z j |, that is when Ω is the unit polydisk of C d . In order to treat these two cases jointly, we will work in the setting of bounded symmetric domains.
An interesting feature is that the rate of decay of approximation numbers highly depends on d, becoming slower and slower as d increases, which might lead to think that no compact composition operators exist for truly infinite- dimensional symbols. We will see in the forthcoming paper [17] that this is not the case.
∗
Supported by a Spanish research project MTM 2012-05622.
2 Notations and background
A bounded symmetric domain of C d is an open convex and circled subset Ω of C d such that for every point a ∈ Ω, there is an involutive bi-holomorphic map u: Ω → Ω such that a is an isolated fixed point of σ (equivalently, u(a) = a and u
′(a) = − id (see [21], Proposition 3.1.1). É. Cartan showed that every bounded symmetric domain of C d is homogeneous, i.e. the group of automorphisms of Ω acts transitively on Ω: for every a, b ∈ Ω, there is an automorphism u of Ω such that u(a) = b (see [21], p. 250). The unit ball B d and the polydisk D d are examples of bounded symmetric domains.
The Shilov boundary S Ω of such a domain Ω is the smallest closed set F ⊆ ∂Ω such that sup z
∈Ω | f (z) | = sup z
∈F | f (z) | for every function f holomorphic in some neighborhood of Ω. For example, the Shilov boundary of the bidisk is S
D2= { (z 1 , z 2 ) ∈ C 2 ; | z 1 | = | z 2 | = 1 } , whereas, its usual boundary ∂ D 2 is { (z 1 , z 2 ) ∈ C 2 ; | z 1 | , | z 2 | ≤ 1 and | z 1 | = 1 or | z 2 | = 1 } ; for the unit ball B d , the Shilov boundary is equal to the usual boundary S d
−1 ([7], § 4.1). Equivalently (see [7], Theorem 4.2), S Ω is the set of the extreme points of the convex set Ω.
If σ is the unique probability measure on S Ω invariant by the automorphisms u of Ω such that u(0) = 0, the Hardy space H 2 (Ω) is the space of all complex- valued holomorphic functions f on Ω such that:
k f k H
2(Ω) :=
sup
0<r<1
Z
S
Ω| f (rξ) | 2 dσ(ξ) 1/2
(see [11]). It is a Hilbert space (see [10]).
A Schur map, associated with Ω, will be a non-constant analytic self-map of Ω into itself. It will be called truly d-dimensional if the differential ϕ
′(a) : C d → C d is an invertible linear map for at least one point a ∈ Ω. Then, by the implicit function Theorem, ϕ(Ω) has non-void interior. We say that the Schur map ϕ is a symbol if it defines a bounded composition operator C ϕ : H 2 (Ω) → H 2 (Ω) by C ϕ (f ) = f ◦ ϕ.
Let us recall that if any Schur function generates a bounded composition operator on H 2 ( D d ) when d = 1, this is no longer the case as soon as d ≥ 2, as shown for example by the Schur map ϕ(z 1 , z 2 ) = (z 1 , z 1 ). Indeed, if say d = 2, taking f (z) = (z 1 + z 2 ) n , we see that
k f k 2 2 = X n
k=0
n k
2
= 2n
n
∼ 4 n
√ πn , while:
k C ϕ f k 2 = k (2z 1 ) n k 2 = 2 n .
The same phenomenon occurs on H 2 (B d ) ([18]; see also [4] and [5]).
If H is a Hilbert space and T : H → H is a bounded linear operator, the approximation numbers of T are defined, for n ≥ 1 by:
(2.1) a n (T ) = inf
rank
R<n k T − R k .
One has k T k = a 1 (T ) ≥ a 2 (T ) ≥ · · · ≥ a n (T ) ≥ a n+1 (T ) ≥ · · · , and T is compact if and only if a n (T) n −→
→∞
0.
The approximation numbers have (obviously) the following ideal property:
for every bounded linear operators S, U : H → H , one has:
a n (ST U ) ≤ k S k k U k a n (T ) , n = 1, 2 . . . .
For an operator T : H 2 (Ω) → H 2 (Ω) with approximation numbers a n (T ) = a n , we will introduce the non-negative numbers 0 ≤ γ d
−(T ) ≤ γ d + (T ) ≤ ∞ defined by:
(2.2) γ
−d (T ) = lim inf
n
→∞log 1/a n
n 1/d and γ d + (T ) = lim sup
n
→∞log 1/a n
n 1/d ·
The relevance of those parameters to the decay of approximation numbers is indicated by the following obvious facts, in which 0 < c ≤ C < ∞ denote constants independent of n:
γ d
−(T ) > 0 ⇐⇒ a n ≤ C e
−c n
1/d, n = 1, 2, . . . (2.3)
γ d + (T) < ∞ ⇐⇒ a n ≥ c e
−Cn
1/d, n = 1, 2, . . . . (2.4)
So, the positivity of γ d
−(T ) indicates that a n is “small” and the finiteness of γ d + (T ) indicates that a n is “big”.
As usual, the notation A . B means that there is a constant c such that A ≤ c B and A ≈ B means that A . B and B . A.
3 Lower bound
The next theorem shows that the approximation numbers of composition op- erators cannot be very small. We have already seen that in the one-dimensional case in [14]. The important fact here is that this lower bound depend highly of the dimension.
Theorem 3.1 Let Ω be a bounded symmetric domain of C d and ϕ: Ω → Ω be a truly d-dimensional Schur map inducing a compact composition operator C ϕ : H 2 (Ω) → H 2 (Ω). Then, for some constants 0 < c ≤ C < ∞ , independent of n, we have:
a n (C ϕ ) ≥ c e
−Cn
1/d, ∀ n ≥ 1, that is
γ d + (C ϕ ) < ∞ .
For proving that, we shall use the following results, the first of which is due
to D. Clahane [6], Theorem 2.1 (and to B. MacCluer [18] in the particular case
of the unit ball B d ).
Theorem 3.2 (D. Clahane) Let Ω be a bounded symmetric domain of C d and ϕ: Ω → Ω be a holomorphic map inducing a compact composition operator C ϕ : H 2 (Ω) → H 2 (Ω). Then ϕ has a unique fixed point z 0 ∈ Ω and the spectrum of C ϕ consists of 0, and all possible products of eigenvalues of the derivative ϕ
′(z 0 ).
When ϕ is truly d-dimensional, 0 cannot be an eigenvalue of C ϕ since if f ◦ ϕ = 0, then f vanishes on ϕ(Ω) which have a non-void interior, and hence f ≡ 0. Note that 1 is an eigenvalue, by taking the product of zero eigenvalue of ϕ
′(z 0 ).
In fact, in our case, we will not need the existence of z 0 , for we will force 0 to be a fixed point by a harmless change of the symbol ϕ.
Lemma 3.3 Let H be a complex Hilbert space and T : H → H be a compact operator with eigenvalues λ 1 , . . . , λ n , . . ., written in non-increasing order and with singular values a n , n = 1, 2, . . . . Then:
(3.1) | λ 2n | 2 ≤ a 1 a n .
Indeed, it suffices to apply an immediate consequence of Weyl’s inequalities, namely | λ n | ≤ (a 1 · · · a n ) 1/n , with n changed into 2n, and square to get
| λ 2n | 2 ≤ (a 1 · · · a 2n ) 1/n ≤ (a n 1 a n n ) 1/n = a 1 a n .
Lemma 3.4 Let N p be the number of multi-indices α = (α 1 , . . . , α d ) such that
| α | = α 1 + · · · + α d ≤ p. Then, as p goes to infinity:
(3.2) N p ∼ p d
d! ·
Proof. Let n k be the number of multi-indices (α 1 , . . . , α d , α d+1 ) such that α 1 + · · · + α d + α d+1 = k. We have (see [13], page 498), classically, for | t | < 1:
X
∞p=0
n p t p = X
∞α
1=0
t α
1· · · X
∞α
d+1t α
d+1= X
∞k=0
t k d+1
= 1
(1 − t) d+1 ; hence
n p = d + p
p
. But N p = n p , and hence:
N p = (d + 1) · · · (d + p)
p! = (d + p)!
p! d! ∼ p d d! ,
by Stirling’s formula for example.
Claim 3.5 We may assume that ϕ(0) = 0 and ϕ
′(0) is invertible.
Proof. Since ϕ is truly d-dimensional, there exists a ∈ Ω such that ϕ
′(a) is invertible. Since Ω is homogeneous, there exist two automorphisms Φ a and Φ ϕ(a) of Ω such that Φ a (0) = a and Φ ϕ(a) [ϕ(a)] = 0. Set ψ = Φ ϕ(a) ◦ ϕ ◦ Φ a . Then ψ(0) = 0. Now, every analytic automorphism Φ of Ω induces a bounded composition operator on H 2 (Ω) and C Φ
−1 = C Φ
−1([6], Theorem 3.1); hence we can write C ψ = C Φ
a◦ C ϕ ◦ C Φ
ϕ(a)and it follows that C ψ , as C ϕ , is compact.
The ideal property of approximation numbers implies that, for n = 1, 2, . . . , one has:
k C Φ
ak k C Φ
ϕ(a)k
−1
a n (C ϕ ) ≤ a n (C ψ ) ≤ k C Φ
ak k C Φ
ϕ(a)k a n (C ϕ ) , so γ d
−(C ψ ) = γ d
−(C ϕ ). Moreover, using the chain rule, we see that ψ
′(0) is
invertible, since ϕ
′(a) is.
Proof of Theorem 3.1. Let µ 1 , . . . , µ d be the eigenvalues of ϕ
′(0) and set min 1
≤j
≤d | µ j | = e
−A > 0. By Theorem 3.2, the eigenvalues λ 1 , . . . , λ n , . . . of C ϕ
are the numbers µ α 1
1· · · µ α d
drearranged in non-increasing order. By definition, we have λ N
p= Q d
j=1 µ α j
jfor some d-tuple α = (α 1 , . . . , α d ) such that | α | ≤ p.
Therefore, | λ N
p| ≥ e
−A
|α
|≥ e
−Ap . If M p = [N p ]/2 where [ . ] stands for the integer part, equation (3.1) gives:
e
−2Ap ≤ | λ N
p| 2 ≤ | λ 2M
p| 2 ≤ a 1 a M
p.
Since M p ∼ C d p d in view of Lemma 3.4, inverting this relation and using the monotonicity of the a n ’s clearly gives the claimed result.
4 An alternative approach for the polydisk and the unit ball
The previous proof of Theorem 3.1 is essentially a “functional analysis” one.
It is interesting to give a proof using complex analysis tools instead of func- tional analysis ones. Moreover, this approach will be useful for the example in Section 6.
In the general case, we are not be able to do that, and we only do it for the polydisk. The same approach works for the unit ball, by using results of B.
Berndtsson in [2]. To save notation, we will give the proof in the case d = 2 but
it clearly works in any dimension d. We will make use of the following theorem
of P. Beurling ([9] p. 285), in which the word interpolation sequence refers to the
space H
∞of bounded analytic functions on Ω (Ω = D or D 2 ), the interpolation
constant M S of the sequence S = (s j ) being the smallest number M such that,
for any sequence (w j ) of data satisfying sup | w j | ≤ 1, there exists f ∈ H
∞(Ω)
such that f (s j ) = w j and k f k
∞≤ M .
Theorem 4.1 (P. Beurling) Let (z j ) be an interpolating sequence in the unit disk D , with interpolation constant M . Then, there exist analytic functions f j , j ≥ 1, on D such that:
f j (z k ) = δ j,k and
X
∞j=1
| f j (z) | ≤ M , ∀ z ∈ D .
As a consequence, if A = (a j ) and B = (b k ) are interpolation sequences of D with respective interpolation constants M A and M B , their “cartesian product”
(p j,k ) j,k = (a j , b k )
j,k is an interpolation sequence, with respect to H
∞( D 2 ), with interpolation constant ≤ M A M B .
The consequence was observed in the paper [3]. Indeed, if (f j ) and (g k ) are P. Beurling’s functions associated to A and B respectively, any sequence (w j,k ) with sup j,k | w j,k | ≤ 1 can be interpolated by the bounded analytic function
f (z, w) = X
j,k
≥1
w j,k f j (z) g k (w)
which satisfies k f k
∞≤ M A M B .
Alternatively, in the sequel, we might use the result of [3] on the sufficiency of Carleson’s condition on products of Gleason distances in the case of several variables. But we will stick to the previous approach. We now make use of the following lemma of [15] which was enunciated in the one-dimensional case, but whose proof works word for word in our new setting; indeed, the space of multipliers of H 2 ( D 2 ) is (isometrically) H
∞( D 2 ) and then one shows that the unconditionality constant of the sequence (K s
j) 1
≤j
≤n of reproducing kernels associated to a finite sequence S = (s j ) 1
≤j
≤n is less than M u (see also [14]).
Also note that he reproducing kernel of H 2 ( D 2 ) is now, for a = (a 1 , a 2 ) ∈ D 2 : K a (z 1 , z 2 ) = 1
(1 − a 1 z 1 )(1 − a 2 z 2 ) , with k K a k 2 = [(1 − | a 1 | 2 )(1 − | a 2 | 2 )]
−1 .
Lemma 4.2 Let ϕ: D 2 → D 2 be a symbol inducing a compact composition operator C ϕ : H 2 ( D 2 ) → H 2 ( D 2 ). Let u = (u 1 , . . . , u N ) be a finite sequence of distinct points of D 2 with interpolation constant M u and let v j = ϕ(u j ), 1 ≤ j ≤ N . Let M v be the interpolation constant of v = (v 1 , . . . , v N ). Then, setting:
µ 2 N = inf
1
≤j
≤N
| K v
j| 2
| K u
j| 2 = inf
1
≤j
≤N
(1 − | u j,1 | 2 )(1 − | u j,2 | 2 ) (1 − | v j,1 | 2 )(1 − | v j,2 | 2 ) , with u j = (u j,1 , u j,2 ) and v j = (v j,1 , v j,2 ), one has:
(4.1) a N (C ϕ ) ≥ c
′µ N M u
−1 M v
−1 ≥ c
′µ N M v
−2 .
The last inequality M u ≤ M v is proved as follows: let sup | w j | ≤ 1 and choose f ∈ H
∞such that f (v j ) = w j and k f k
∞≤ M v ; then g = f ◦ ϕ ∈ H
∞and satisfies k g k
∞≤ M v and g(u j ) = f (v j ) = w j . It remains to choose u and v and to estimate the parameters of the lemma.
As in the first proof, we may assume that ϕ(0) = 0 and that the differential ϕ
′(0) is invertible.
Since ϕ
′(0) is invertible, the set ϕ( D 2 ) contains a closed polydisk of radius 0 < r < 1 with center 0. We then take for v the sequence v j,k = (rω j , rω k ) where ω is a primitive nth-root of unity, e.g. ω = e 2iπ/n . We have v = A × A where A = (rω, rω 2 , . . . , rω n ) so that the sequence v has length N = n 2 . We know ([9], p. 284) that M A = r 1
−n , so that Theorem 4.1 gives us M v ≤ r 2
−2n . We now write v j = ϕ(u j ) with | u j | ≤ r, which is always possible by decreasing r if necessary (this r can be ridiculously small, but remains positive). Finally,
k K v
jk 2
k K u
jk 2 ≥ (1 − | u j,1 | 2 )(1 − | u j,2 | 2 ) ≥ (1 − r 2 ) 2 . Collecting all those estimates and using (4.1), we obtain:
a n
2(C ϕ ) ≥ (1 − r 2 ) 2 r 4n
−4 ≥ c r 4n .
Interpolating an arbitrary integer m between two consecutive squares, we clearly obtain Theorem 3.1 for D 2 (note that in dimension d a factor (1 − r 2 ) d instead
of (1 − r 2 ) 2 shows up).
5 An upper bound
Though the result of this section is undoubtedly true in the general setting of bounded symmetric domains, we are not familiar enough with complex analysis in several variables to work it out. Therefore, we will assume in this section that:
(5.1) Ω = B l
1× · · · × B l
N, with l 1 + · · · + l N = d
is the product of N unit balls. That covers the case of the unit ball of C d (N = 1) and the case of the polydisk of C d (N = d and l 1 = · · · = l N = 1). To save notations, we will assume in the sequel with N = 2.
A point z = (z j ) 1
≤j
≤d ∈ Ω is of the form z = (u, v) with u = (u j ) 1
≤j
≤l
1, v = (v j ) l
1<j
≤d and P l
1j=1 | u j | 2 < 1, P d
j=l
1+1 | v j | 2 < 1. We see that Ω is the unit ball of C d equipped with the following norm:
(5.2) |k z k| = max X l
1j=1
| u j | 2 1/2
, X d
j=l
1+1
| v j | 2 1/2
,
where z = (u, v) with u ∈ C l
1and v ∈ C l
2.
The Shilov boundary of Ω is S Ω = S l
1× S l
2and the normalized invariant measure on S Ω is σ = σ l
1⊗ σ l
2where σ l
1and σ l
2denote respectively the area measure on the hermitian spheres S l
1and S l
2.
The following is in Rudin ([19] p. 16).
Lemma 5.1 The monomials e α , with e α (z) = z α , form an orthogonal basis of H 2 (Ω). Moreover if α = (β, γ) with β = (α 1 , . . . , α l
1) and γ = (α l
1+1 , . . . , α d ), then writing z = (u, v) we have:
k e α k 2 = Z
S
l1×S
l2| u β | 2 | v γ | 2 dσ l
1(u) dσ l
2(v) = (l 1 − 1)! β!
(l 1 − 1 + | β | )!
(l 2 − 1)! γ!
(l 2 − 1 + | γ | )! · Therefore, if f = P
α c α e α ∈ H 2 (Ω), one has:
k f k 2 = X
α
| c α | 2 (l 1 − 1)! β ! (l 1 − 1 + | β | )!
(l 2 − 1)! γ!
(l 2 − 1 + | γ | )! ·
We can now state the main result of that section, in which we set k ϕ k
∞:=
sup z
∈Ω |k ϕ(z) k| .
Theorem 5.2 Let Ω = B l
1× B l
2, d = l 1 + l 2 , and ϕ: Ω → Ω be a truly d- dimensional Schur map, inducing a compact composition operator C ϕ : H 2 (Ω) → H 2 (Ω). Then, if k ϕ k
∞< 1, one has γ d
−(C ϕ ) > 0, that is there exist some constants 0 < c ≤ C < ∞ , independent of n, such that:
(5.3) a n (C ϕ ) ≤ C e
−cn
1/d, n = 1, 2, . . . . Proof. Let us set r = k ϕ k
∞< 1. Let f = P
c α e α ∈ H 2 (Ω) with (5.4) c α = f b (α) and k f k 2 = X
α
| c α | 2 k e α k 2 ≤ 1 . Then C ϕ f = P
c α ϕ α .
We approximate C ϕ by the N n -rank operator R defined by Rf = X
|
α
|≤n
c α ϕ α
and we set g = C ϕ (f ) − R(f ) as well as α = (β, γ) and z = (u, v). We begin with observing that (l (l
11−−1+p)! 1)!p! ≤ (p + 1) l
1−1 and (l (l
22−−1+q)! 1)!q! ≤ (q + 1) l
2−1 . Since
| c α | ≤ k e α k
−1 , we get by Lemma 5.1 and the multinomial formula:
(5.5) X
|
β
|=p
p!
β! | ϕ β (u) | 2 = X l
1j=1
| ϕ j (u) | 2
p
and a similar formula with | γ | = q that, setting p + q = N:
X
|
β
|=p
|
γ
|=q
k e α k
−2 | ϕ α (z) | 2 = X
|
β
|=p
|
γ
|=q
(l 1 − 1 + p)!
β!(l 1 − 1)!
(l 2 − 1 + q)!
γ!(l 2 − 1)! | ϕ β (u) | 2 | ϕ γ (v) | 2
≤ (p + 1) l
1−1 (q + 1) l
2−1 X l
1j=1
| ϕ j (u) | 2
p X d j=l
1+1
| ϕ j (v) | 2 q
≤ (p + 1) l
1−1 (q + 1) l
2−1 r 2p r 2q ≤ (N + 1) l
1+l
2−2 r 2N . We thus have for z ∈ Ω the pointwise estimate (where we used (5.4) and the Cauchy-Schwarz inequality):
| g(z) | 2 ≤ X
|