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Function Theory and Operator Theory on the Dirichlet Space

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Function Theory and Operator Theory on the Dirichlet Space Holomorphic Spaces MSRI Publications Volume 33, 1998 Function Theory and Operator Theory on the Dirichlet Space ZHIJIAN WU Abstract. We discuss some recent achievements in function theory and operator theory on the Dirichlet space, paying particular attention to in- variant subspaces, interpolation and Hankel operators. Introduction In recent years the Dirichlet space has received a lot of attention from math- ematicians in the areas of modern analysis, probability and statistical analysis. We intend to discuss some recent achievements in function theory and opera- tor theory on the Dirichlet space. The key references are [Richter and Shields 1988; Richter and Sundberg 1992; Aleman 1992; Marshall and Sundberg 1993; Rochberg and Wu 1993; Wu 1993]. In this introductory section we state the basic results. Proofs will be discussed in the succeeding sections. Denote by D the unit disk of the complex plane. For α 2 R, the space Dα 1 n D consists of all analytic functions f(z) = 0 anz defined on with the norm 1 P 1=2 α 2 kfkα = (n + 1) janj : X0 2 For α = −1 one has D−1 = B, the Bergman space; for α = 0, D0 = H , the Hardy space; and for α = 1, D1 = D, the Dirichlet space. The space Dα is referred to as a weighted Dirichlet space if α > 0, and a weighted Bergman space if α < 0. It is trivial that Dα ⊂ Dβ if α > β. In particular, the Dirichlet space is contained in the Hardy space. For any w 2 D, the point evaluation at w is a bounded linear functional on D. Therefore there is a corresponding reproducing kernel. It is given by 1 1 k (z) = k(z; w) = log : w wz 1 − wz Research supported in part by the NSF Grant DMS-9622890. 179 180 ZHIJIAN WU Let 1 0 2 2 D(f) = jf (z)j dA(z) = n janj ; ZD nX=1 where dA(z) = (1/π) dx dy is normalized Lebesgue measure on D. The square of the norm of a function f in D can be also expressed as 2 2 2 kfk = kfk1 = kfk0 + D(f): Arazy, Fisher and Peetre proved in [Arazy et al. 1988] that the number D(f) is the Hilbert{Schmidt norm of the big Hankel operator on the Bergman spacep (introduced first in [Axler 1986]) with the analytic symbol f. Arazy and Fisher [1985] proved that the Dirichlet space D with the norm k · k = D( · ) is the unique M¨obius invariant Hilbert space on D. A more general resultp in [Arazy et al. 1990] implies that for any Bergman type space B(ν) = L2(D; ν) \ fanalytic functions on Dg, which has a reproducing kernel kν (z; w), one has the formula 2 2 jf(z) − f(w)j jkν (z; w)j dν(z) dν(w) = D(f) for all f 2 D: ZD ZD The operator Mz of multiplication by z on the Dirichlet space, denoted some- times by (Mz; D), is a bounded linear operator. Moreover it is an analytic 2-isometry; that is, 1 2 2 2 2 D nD Mz f − 2 kMzfk + kfk = 0 for all f 2 ; and Mz = f0g: n\=0 Richter [1991] proved that every cyclic analytic 2-isometry can be represented as D multiplication by z on a Dirichlet-type space (µ) with the norm k · kµ defined by 2 2 kfkµ = kfk0 + Dµ(f): Here µ is a nonnegative finite Borel measure on the unit circle @D; the number Dµ(f) is defined by 0 2 Dµ(f) = jf (z)j hµ(z) dA(z); ZD where hµ(z) is the harmonic extension of the measure µ to D, defined as the iθ 2 iθ 2 integral of the Poisson kernel Pz(e ) = (1 − jzj )=je − zj against dµ: 2π 1 iθ hµ(z) = Pz(e ) dµ(θ): 2π Z0 2 2 It is not hard to see that Dµ(f) < 1 implies f 2 H . Therefore D(µ) ⊆ H . Deep results involving D(µ) can be found in [Richter and Sundberg 1991]. A closed subspace N of D is called invariant if Mz maps N into itself. We shall discuss the following two theorems for invariant subspaces. FUNCTION THEORY AND OPERATOR THEORY ON THE DIRICHLET SPACE 181 Theorem 0.1. Let N 6= f0g be an invariant subspace for (Mz; D). Then dim(N zN) = 1; that is, zN is a closed subspace of N of codimension one. For f 2 D, denote by [f] the smallest invariant subspace of D containing f. An analytic function ' defined on D is called a multiplier of D if 'D ⊆ D. The multiplier norm of ' is defined by k'kM = supfk'fk : f 2 D; kfk = 1g: Theorem 0.2. Every nonzero invariant subspace N of (Mz; D) has the form N = ['] = 'D(m'); iθ 2 where ' 2 N zN is a multiplier of D, and dm' = j'(e )j dθ=2π. The codimension-one property for invariant subspaces of the Dirichlet space was first proved in [Richter and Shields 1988]. Another proof that works for the more general operators (Mz; D(µ)) and gives more information can be found in [Richter and Sundberg 1992]. Aleman [1992] generalized the argument in [Richter and Sundberg 1992] so that it works for the weighted Dirichlet spaces Dα for 0 < α ≤ 1 (α > 1 is trivial). Recently, Aleman, Richter, and Ross provided another approach to the codimension-one property which is good for a large class of weighted Dirichlet spaces and certain Banach spaces. Part of Theorem 0.2 was proved in [Richter 1991]. That the generator ' is a multiplier of D was proved in [Richter and Sundberg 1992]. (The result there is for the operator (Mz; D(µ))). Carleson [1958] proved that, for a disjoint sequence fzng ⊂ D, the interpola- tion problem '(zn) = wn; for n = 1; 2; 3; : : : (0{1) 1 1 has a solution ' 2 H for every given fwng 2 ` if and only if there are a δ > 0 and a C < 1 such that z − z n m ≥ δ for all n 6= m 1 − z¯ z n m and 2 (1 − jznj ) ≤ C jIj for all arcs I ⊂ @D: znX2S(I) Here jIj is the arc length of I and S(I) is the Carleson square based on I, defined as S(I) = z 2 D : z=jzj 2 I and jzj > 1 − jIj=2π : Let MD denote the space of multipliers of D. It is clear that MD is an algebra 1 1 and MD ⊂ H . We remark that H is in fact the space of all multipliers of H2. 182 ZHIJIAN WU A sequence fzng ⊂ D is called an interpolating sequence for MD if, for each bounded sequence of complex numbers fwng, the interpolation problem (0{1) has a solution ' in MD. By the closed graph theorem, we know that if fzng is an interpolating sequence for MD then there is a constant C < 1 so that the inter- M polation can be done with a function ' 2 D satisfying k'kM ≤ C kfwngk`1 . Axler [1992] proved that any sequence fzng ⊂ D with jznj ! 1 contains a subsequence that is an interpolating sequence for MD. Marshall and Sundberg [1993] gave the following necessary and sufficient conditions for an interpolating sequence for MD. Theorem 0.3. A sequence fzng is an interpolating sequence for MD if and only if there exist a γ > 0 and a C0 < 1 such that 2 z − z γ 1 − n m ≤ (1 − jz j2) for all n 6= m (0{2) 1 − z¯ z n n m and 1 −1 1 −1 log 2 ≤ C log : (0{3) 1 − jznj Cap Ij zn2[XS(Ij ) S Here fIj g is any finite collection of disjoint arcs on @D. Bishop also proved this theorem independently. Sundberg told me that a similar M result for Dα with 0 < α < 1 is also true. Condition (0{3) is a geometric condition for a Carleson measure for D. Car- leson measures for Dα were first characterized by Stegenga [1980]. His result says that a nonnegative measure µ on D satisfies 2 2 D jg(z)j dµ(z) ≤ C kgkα for all g 2 α ZD (in other words, is a Carleson measure for Dα) if and only if µ S(Ij ) ≤ C Capα Ij [ [ D for any finite collection of disjoint arcs fIj g on @ . Here Capα( · ) denotes an appropriate Bessel capacity depending on α. When α = 1, the usual logarithmic capacity may be used for Cap1( · ). Using Stegenga's theorem, condition (0{3) can be replaced by −1 1 D log 2 δzn is a Carleson measure for : (0{4) X 1 − jznj Hankel operators (small and big) on the Hardy and the Bergman spaces have been studied intensively in the past fifteen years. We refer the reader to [Luecking 1992; Peller 1982; Rochberg 1985; Zhu 1990] and references therein for more in- 2 2 formation. Denote by PH2 the orthogonal projection from L (@D) onto H . On the Hardy space, the Hankel operator with symbol b 2 L2(@D) can be written as 1 (I − PH2 )(¯bg) for g 2 H : FUNCTION THEORY AND OPERATOR THEORY ON THE DIRICHLET SPACE 183 Another existing definition is 1 PH2 (bg¯) for g 2 H : In fact, if f¯bng is the sequence of Fourier coefficients of b, the two operators above correspond to the Hankel matrices fb1; b2; b3; : : :g and fb0; b1; b2; : : :g, respectively. In more general spaces, these expressions define two different op- erators, called big Hankel and small Hankel, respectively.
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