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C. R. Acad. Sci. Paris, Ser. I 335 (2002) 729–732 Analyse mathématique/Mathematical Analysis

Besov spaces and Bergman projections on the ball

H. Turgay Kaptano˘glu

Mathematics Department, Middle East Technical University, Ankara 06531, Turkey Received 2 September 2002; accepted 13 September 2002

Note presented by Jean-Pierre Kahane.

Abstract A class of radial differential operators are investigated yielding a natural classification of diagonal Besov spaces on the unit ball ofCN. Precise conditions are given for the boundedness of Bergman projections from certain Lp spaces onto Besov spaces. Right inverses for these projections are also provided. Applications to complex interpolation are presented. To cite this article: H.T. Kaptano˘glu, C. R. Acad. Sci. Paris, Ser. I 335 (2002) 729–732.

2002 Académie des sciences/Éditions scientifiques et médicales Elsevier SAS

Les espaces de Besov et les projections de Bergman dans la boule

Résumé Nous étudions une class d’opérateurs différentiels radiaux conduisant à une classification

naturelle des espaces de Besov diagonaux dans la boule unité deCN. Nous donnons les conditions précises pour la bornitude des projections de Bergman de certains espaces Lp sur des espaces de Besov. Nous déterminons aussi des inverses à droite pour ces projections.

Nous présentons des applications à l’interpolation complexe. Pour citer cet article : H.T.

Kaptano˘glu, C. R. Acad. Sci. Paris, Ser. I 335 (2002) 729–732.

2002 Académie des sciences/Éditions scientifiques et médicales Elsevier SAS

1. Introduction

LetB denote the unit ball of CN and H (B) the space of holomorphic functions on B. Let ν be the normalized volume measure onB and let dνq(z)= (1 − |z|2)qdν(z). Diagonal Besov spaces BSVvp are defined in one of two ways. One definiton requires an f∈ H (B) to satisfy (1 − |z|2)m−vRmf (z)∈ Lp−1) for some integer m > v, where v is real (see [6]). Here R is the radial derivative; see below. Another requires an f∈ H (B) to satisfy R1+vf (z)∈ Lpp−1), where v > 0, Rvis a v-th-order radial derivative, and p > 1 (see [12]).

The purpose of this Note is to give a new definition that characterizes these spaces using exactly the same parameters as those of the weighted Bergman spaces Apq= Lpq)∩ H (B): p > 0 and q ∈ R. The function whose p-th power is considered is not f any more, but a product of a t -th order radial derivative of f and the t -th power of 1− |z|2. We call the spaces thus defined Bqp, and it turns out that they naturally extend the Apq spaces to all q∈ R while satisfying Apq = Bqpfor q >−1. The value of t turns out to be irrelevant as long as (Re t)p+ q > −1. Eq. (2) summarizes the new classification.

Detailed proofs and further results will be presented elsewhere.

2. Radial differential operators

The radial derivative at z of a holomorphic function f is Rf (z)=

k=1kfk(z), where fk is the k-th term in the homogeneous expansion of f . Following [7], we define some more general linear operators.

E-mail address: kaptan@math.metu.edu.tr (H.T. Kaptano˘glu).

2002 Académie des sciences/Éditions scientifiques et médicales Elsevier SAS. Tous droits réservés

S 1 6 3 1 - 0 7 3 X ( 0 2 ) 0 2 5 5 6 - 6 /FLA

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H.T. Kaptano˘glu / C. R. Acad. Sci. Paris, Ser. I 335 (2002) 729–732

DEFINITION. – Let f ∈ H (B). We define Dstf =

k=0

(s+ t)k

(s)k

fk (s∈ C \ −N, s + t ∈ C \ −N),

where (a)0= 1 and (a)m= a(a + 1) · · ·(a + m − 1) for positive integer m. If, say, s = −m with m ∈ N, we write the corresponding factor as (λ)k, divide it by (−1)m(λ+ m), and then let λ → −m. So

Dstf = f0+ · · · + fm+ 

k=m+1

(t− m)k

m!(1)k−m−1fk (s= −m ∈ −N, s + t ∈ C \ −N).

The definition of Dts when s+ t or both s and s + t are nonpositive integers is similar.

It is shown in [5] that Dts is a continuous operator on H (B). If ds,t,k is the coefficient of fk in Dtsf , Stirling’s formula gives ds,t,k∼ kt as k→ ∞. Thus Dts is a radial differential operator of order t ∈ C.

Every Dtsis a bijection on H (B) and thus invertible. A case by case checking reveals that Drs+tDts= Dts+r. Thus (Dts)−1= Ds−t+t for all r, s, t∈ C.

3. Bqpspaces

DEFINITION. – Let q∈ R and 0 < p  ∞ with −qp + q > −1 (read −q > 0 when p = ∞). We define Bqp= Bqp(B) as the space of f ∈ H (B) for which the function (1 − |z|2)−qD−q−qf (z) belongs to Lpq).

The Bqpnorm of f is defined as the Lpq) norm of (1− |z|2)−qD−q−qf (z).

We use the term norm even when 0 < p < 1. More explicitly, Bqp(B) =



f∈ H (B) : f pBp

q =



B

D−q−qf (z)p−qp+q(z) <



(0 < p <∞), Bq(B) =

f ∈ H (B) : f Bq = sup

z∈B

1− |z|2 −qD−q−qf (z)<.

Let us also define Bq0(B) as that subspace of Bq(B) with the same norm consisting of functions f for which (1− |z|2)−q|D−q−qf (z)| belongs to C0(B), continuous functions on B with 0 boundary values. Since every Dts is invertible, there is no nonzero f∈ Bqpfor whichf Bqpis zero.

THEOREM 1. – An f∈ H (B) belongs to Bqpif and only if for some s and t satisfying (Re t)p+ q > −1 (read Re t > 0 when p= ∞) the function (1 − |z|2)tDstf (z) belongs to Lpq). The Lpq) norm of (1− |z|2)tDstf (z) is equivalent to the Bqpnorm of f .

The case q= −(N + 1) is handled in [15,16]. Also, the Bqpspaces are the spaces Ap−qp+q+1,−qof [9], which considers only−qp + q + 1 > 0.

DEFINITION. – Let q∈ R and 0 < p  ∞. We define Bqp= Bqp(B) as the space of f ∈ H (B) for which the function (1− |z|2)tDstf (z) for some s and t satisfying (Re t)p+ q > −1 (read Re t > 0 for p = ∞) belongs to Lpq).

COROLLARY. – The spaces Bqpfor q >−1 and the Bergman spaces Apq coincide.

By Theorem 1, Bqspaces are the same for all q∈ R. This space is the Bloch space B. Similarly, the spaces Bq0are all the same for q∈ R and are the little Bloch space B0. The next result is in [16] for s > N . COROLLARY. – A function f ∈ H (B) belongs to B (resp. B0) if and only if for some s and t with Re t > 0 the function (1− |z|2)tDstf (z) is uniformly bounded onB (resp. belongs to C0(B)).

COROLLARY. – Our space Bqpand the diagonal Besov space BSV−(q+1)/pp coincide.

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To cite this article: H.T. Kaptano˘glu, C. R. Acad. Sci. Paris, Ser. I 335 (2002) 729–732

Thus Bqpspaces for p 1 are Banach spaces. Each Bq2space has several equivalent inner products (f, g)s,t=



B

1− |z|2 t

Dtsf (z)

1− |z|2 t

Dstg(z) dνq(z), (1)

one for each s and each t satisfying 2 Re t+ q > −1. The monomials {zα} form an orthogonal set with respect to each of these inner products.

THEOREM 2. – Each Bq2is a Hilbert space with reproducing kernel Kq(z, w)= (1 − z, w)−(N+1+q) for q >−(N + 1) and

Kq(z, w)= 1 +

k=1

(k− 1)!

(−N − q)kz, wk

for q −(N + 1); in particular, K−(N+1)(z, w)= 1 − log(1 − z, w).

Similar descriptions in [13] and [2] led the author to this research. In fact, the spaces in Theorem 2 are known as Dirichlet-type spaces, B−(N+1)2 being the Dirichlet spaceD and B−12 being the Hardy space H2. The space B−N2 attracts a lot of attention in operator theory (see [3] and [8]) due to the universal property of its kernel in Nevanlinna–Pick interpolation (see [1]) and is denotedP here. Another description of Bq2

spaces for q −(N + 1) without any derivatives is given in [4]. The same reference contains an example that shows that the inclusion Bqp1⊂ Bqp2 for q1< q2is proper for q −(N + 1), which actually works for all real q .

Let 0 < p1< 1 < p2< 2 < p3and q1<−(N + 1) < −N < q2<−1 < 0 < q3. Then

... ... ... ... ... ...

· · · Aqp31 ⊃ A1q3 ⊃ Aqp32 ⊃ A2q3⊃ Apq33 ⊃ B q3= q

∪ ∪ ∪ ∪ ∪ 

· · · Ap1 ⊃ A1 ⊃ Ap2 ⊃ A2 ⊃ Ap3 ⊃ B 0= q

∪ ∪ ∪ ∪ ∪ 

· · · B−1p1 B−11 B−1p2 H2 B−1p3 B −1 = q

∪ ∪ ∪ ∪ ∪ 

· · · Bqp21 Bq1

2 Bqp2

2 Bq2

2 Bqp3

2 B q2= q

∪ ∪ ∪ ∪ ∪ 

· · · B−Np1 B−N1 B−Np2 P B−Np3 B −N = q

∪ ∪ ∪ ∪ ∪ 

· · · B−(N+1)p1 M ⊂ B−(N+1)p2 ⊂ D ⊂ B−(N+1)p3 ⊂ B −(N +1)=q

∪ ∪ ∪ ∪ ∪ 

· · · Bqp11 Bq1

1 Bqp2

1 Bq2

1 Bqp3

1 B q1= q

... ... ... ... ... ...

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The inclusions of the level q= −(N + 1) follow from their Möbius invariance and are in [10] for p > 1.

Further, B−(N+1)1 is the minimal Möbius-invariant spaceM; see [11]. Thus also M ⊂ B−(N+1)p2 . 4. Bergman projections

We restrict ourselves to 1 p  ∞ from now on. Bergman projections are the linear operators Ps with s∈ C defined by

Psf (z)= C



B

(1− |w|2)s

(1− z, w)N+1+sf (w) dν(w) (z∈ B)

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H.T. Kaptano˘glu / C. R. Acad. Sci. Paris, Ser. I 335 (2002) 729–732

for f ∈ L1s). It is clear that Psf ∈ H (B). The coefficient C is a normalization constant. The following theorem appears in [11] for real s >−1.

THEOREM 3. – Let 1 p < ∞ and q  −1. The Bergman projection Ps maps Lpq) boundedly onto Bqp if and only if q+ 1 < p(Re s + 1) and N + 1 + s is not a nonpositive integer. Given such an s, if t satisfies (Re t)p+ q > −1, then Ps((1− |z|2)tDNt +1+sf (z))= Cf (z) for all f ∈ Bqp.

COROLLARY. – The Bergman projection Ps maps Lq)= L(ν) boundedly ontoB and each of C(B) and C0(B) onto B0 if and only if Re s > −1. Given such an s, if t satisfies Re t > 0, then Ps[(1 − |z|2)tDNt +1+sf (z)] = Cf (z) for all f ∈ B and hence for all f ∈ B0too.

5. Duality and interpolation

THEOREM 4. – Let 1 p < ∞ and q  −1. The dual space (Bqp)can be identified with Bqp under the pairing (·, ·)N+1,−qof (1), where 1/p+ 1/p= 1. In particular, the Bloch space B is the dual space of all Bq1. The dual spaceB0can be identified with each of Bq1under the pairings (·, ·)N+1,−qof (1).

THEOREM 5. – Suppose 1 p0< p < p1 ∞ with 1/p = (1 − θ)/p0+ θ/p1 for some θ ∈ (0, 1).

Then the complex interpolation space[Bqp0, Bqp1]θis Bqp.

The case q= −(N + 1) of Theorem 4 is in [15]. For the definitions on complex interpolation, see [14].

Let ψ be a holomorphic automorphism ofB. It is shown in [9] using (1) that the Bergman spaces Apq for 0 < p ∞ and q > −1 are invariant under each of the isometries

Uψp,qf (z)= f ψ(z) 

J ψ(z) (2/p)(1+q/(N+1)).

THEOREM 6. – Suppose 2 p  ∞, −(N + 1) < q  −1, and ψ as above. Then Uψp,q is a bounded linear transformation on Bqp.

Acknowledgements. The author expresses his gratitude to Daniel Alpay of Ben-Gurion University of the Negev for his extensive support and getting him involved in the spaceP.

References

[1] J. Agler, J.E. McCarthy, Complete Nevanlinna–Pick kernels, J. Funct. Anal. 175 (2000) 111–124.

[2] D. Alpay, H.T. Kaptano˘glu, Integral formulas for a sub-Hardy Hilbert space on the ball with complete Nevanlinna–

Pick reproducing kernel, C. R. Acad. Sci. Paris, Série I 333 (2001) 285–290.

[3] D. Alpay, H.T. Kaptano˘glu, Some-finite dimensional backward-shift-invariant subspaces in the ball and a related interpolation problem, Integral Equations Operator Theory 42 (2002) 1–21.

[4] D. Alpay, H.T. Kaptano˘glu, Gleason’s problem and homogeneous interpolation in Hardy and Dirichlet-type spaces of the ball, J. Math. Anal. Appl., 2002, to appear.

[5] J. Arazy, Boundedness and compactness of generalized Hankel operators on bounded symmetric domains, J. Funct. Anal. 137 (1996) 97–151.

[6] J. Arazy, S.D. Fisher, S. Janson, J. Peetre, Membership of Hankel operators on the ball in unitary ideals, J. London Math. Soc. 43 (1991) 485–508.

[7] J. Arazy, H. Upmeier, Invariant inner product in spaces of holomorphic functions on bounded symmetric domains, Doc. Math. 2 (1997) 213–261.

[8] J.A. Ball, T. Trent, V. Vinnikov, Interpolation and commutant lifting for multipliers on reproducing kernel Hilbert spaces, in: Oper. Theory Adv. Appl., Vol. 122, Birkhäuser, Basel, 2001, pp. 89–138.

[9] F. Beatrous, J. Burbea, Holomorphic Sobolev spaces on the ball, Dissertationes Math. 276 (1989).

[10] K.T. Hahn, E.H. Youssfi, Möbius invariant Besov p-spaces and Hankel operators in the Bergman space on the ball inCn, Complex Variables Theory Appl. 17 (1991) 89–104.

[11] M.M. Peloso, Möbius invariant spaces on the unit ball, Michigan Math. J. 39 (1992) 509–536.

[12] K.E. Shaw, Tangential limits and exceptional sets for holomorphic Besov functions in the unit ball ofCn, Illinois J. Math. 37 (1993) 171–185.

[13] Z. Yan, Invariant differential operators and holomorphic function spaces, J. Lie Theory 10 (2000) 1–31.

[14] K. Zhu, Operator Theory in Function Spaces, Dekker, New York, 1990.

[15] K. Zhu, Holomorphic Besov spaces on bounded symmetric domains, I, Quart. J. Math. Oxford 46 (1995) 239–256.

[16] K. Zhu, Holomorphic Besov spaces on bounded symmetric domains, II, Indiana Univ. Math. J. 44 (1995) 1017–

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