THESIS LIBRARY Michigan State University This is to certify that the dissertation entitled MIXED NORM GENERHLIEH‘TIONS OF LOEIGHTEb BERGMHA) SPHCES m) HE um BflLL 01: (3 presented by STEVE N mm RLES 614 D 8018 has been accepted towards fulfillment of the requirements for PA. D degreein Haflejmafics flf you I Majorfl pr es 1' Dt (0,2,,375. William T. Sledd ae MS U is an Affirmative Action/Equal Opportunity Institution 0-12771 MSU LIBRARIES m v RETURNING MATERIALS: Place in book drop to remove this checkout from your record. FINES will be charged if book is returned after the date stamped below. MIXED NORM GENERALIZATIONS OF WEIGHTED BERGMAN SPACES IN THE UNIT BALL OF [IN By Steven Charles Gadbois A DISSERTATION Submitted to Michigan State University in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Department of Mathematics 1985 ABSTRACT MIXED NORM GENERALIZATIONS OF WEIGHTED BERGMAN SPACES IN THE UNIT BALL OF It“ By Steven Charles Gadbois Let f be an analytic function in the unit ball B of it” for which the "mixed norm" (I01 (I33 |f(rt)|P dc(t))q/pw(r)r2N-1 dr)"q is finite. Here 0 < p < 00, 0 < q < 0°, 0) is a suitable radial weight function, and o is normalized Lebesgue measure on as. Note that when p = q, because of the "polar coordinates” formula, the space of all such functions is just the Bergman space with weight (0. General mixed norm spaces were studied extensively by Benedek and Panzone. We begin by generalizing a collection of results gotten by Luecking forthe Bergman spaces or the Hardy spaces. Boundedness of certain Bergman projections is proven first, using vector-valued integration and some facts due to Forelli and Rudin. Representation of the dual space of our mixed norm Spaces follows from this. Then a representation of functions in our mixed norm spaces is obtained (by using duality) and several equivalent norms are produced (by refining arguments of Luecking). We also state a general "Carleson measure theorem" for our mixed norm spaces whose proof depends largely on geometry and the connection between Steven Charles Gadbois the nonisotropic metric and the invariant Poisson kernel. Several consequences are noted, including a theorem originally due to Cima and Wogen. Other related methods and results are given, among them a Carleson measure theorem for mixed norm spaces in the polydisc, a generalization of a result of Hastings. To my wife, parents, and family for their patience and love ACKNOWLEDGMENTS I am indebted to my advisor, Professor William Sledd, for his suggestions, support, and patience during my work on this dissertation and the reading that preceded it. I have benefited greatly from his knowledge of the literature and his remarkable intuition. There are many others at Michigan State University whom I must also thank, among them Professors Sheldon Axler, Wade Ramey, and Joel Shapiro, for many inspiring analysis courses and seminars, and Professors Habib Salehi and Lee Sonneborn, for special guidance and advice. TABLE OF CONTENTS INTRODUCTION CHAPTER 1 §1. Notation and Definitions §2. Basic Properties of Ali: §3. The Nonisotropic Metric and the Pseudohyperbolic "Metric" CHAPTER 2 §1. Boundedness of the Bergman Projection on LE5 §2. Representation of the Dual Space of Ali? §3. Two Norm-Representation Theorems §4. Representation of Ali? Functions CHAPTER 3 §1. Some History §2. Some Estimates §3. A Carleson Measure Theorem §4. Some Corollarles §5. Related Methods and Results BIBLIOGRAPHY Page $030000 10 15 17 22 25 25 27 30 34 36 41 INTRODUCTION Let f be an analytic function in the unit ball B of it” for which the "mixed norm" (I01 (I38 |f(rrc)lp do(‘c))q’pw(r)r2N'1 dr)1/q is finite. Here 0 < p < 00, 0 < q < 00, a) is a suitable radial weight function (e.g., (o(r) = (1 - r2)“ for a > -1), and o is normalized Lebesgue measure on BB. The space of all such functions is denoted by Afi’j. Note that when p = q, because of the "polar coordinates" formula, this is just the weighted Bergman space A50. General mixed norm spaces were studied extensively by Benedek and Panzone in [2]. The preliminaries are taken care of in Chapter 1. All notation and definitions are given, several metrics to be used later are discussed, and ABE is shown to be a Banach space for certain to. Chapter 2 generalizes results gotten by Luecking in [11] for the Bergman spaces Aior the Hardy spaces HP. Boundedness of certain Bergman projections is proven first, using vector-valued integration and some facts due to Forelli and Rudin in [7]. Representation of the dual space of Afj for certain p, q, and (0 follows from this. Then by refining arguments of Luecking a representation of functions in AZ? is obtained (duality is also used) and several equivalent norms are produced. In Chapter 3 we state a general "Carleson measure theorem" for our mixed norm spaces whose proof depends largely on geometry and the connection between the nonisotropic metric and the invariant Poisson kernel. Several consequences are noted, including a theorem originally due to Cima and Wogen in [4]. Other related methods and results are given, among them a Carleson measure theorem for mixed norm spaces in the polydisc which generalizes a result of Hastings in [8]. CHAPTER 1 In section one of this chapter, a mixed norm generalization of the weighted Bergman space in the unit ball of it“ is defined, and notation is set forth. Basic properties of our spaces of functions are given in section two, and the various metrics we will find useful are described in section three. §1 Ngtation and Definitigns The classical Bergman space A9 on the unit ball B = BN in [EN (0 < p < 00) is the set of functions f e H(BN) satisfying (IB |f(z)|F’ dm(z))1/p < oo. Here N is a positive integer, [IN is equipped with the usual inner product defined for z =(21, . . . ,zN) and w = (w,, . . . ,wN) in It” by (z, w) = .51 2in and with the associated norm [2] = (z, z)1/2, H(BN) is the set of holomorphic functions on BN, and m is Lebesgue measure on BN normalized so that m(BN) = 1. Using "polar cooordinatesv. (see [15], 1.4.3), this integral may be written as (2N I! (Is lf(r1:)|P d0(‘t)) rZI‘I'1 dr)1/p where l = [0, 1), S = SN = aBN = {z e (EN | [2| = 1}, and o=oN is the rotation 3 invariant positive Borel measure on SN with C(SN) = 1. We shall study the following weighted "mixed norm" generalizations of the Bergman spaces. If 0 < p, q < 00 and it o) is a nonnegative weight function on [0, 1) satisfying I, (o(r)r2N" dr < 00, define A53 = {t e H(B) | [ltllpm = (II (IS |I(l"c)|p do(t))q/pu)(r)r2N'1 dr)1/q < ea}, Note that when to a 1 and q = p, this is precisely the Bergman space. Also note that ltlpq.=( (.l Hill We art-dove. where, for O s r < 1, fr is the function defined on S by Ir(’t) = f(rt). Using this notation, we also define A? = {t e HIBll iitil..,,,.. = (l. ltiitoaemoN-t dot/o < co}. Ap°°= HP: {fe H(B)| llfllpoo= sup Ilf “9(3) < 0°}. 00"(1 and A°°°° = H°° = {i e H(B )Illfllm— = 3,ng lli noelL < 0°}- The Spaces HID and H°° are the classical Hardy spaces. In the special case that w(r) = (1 - r2)“ with a > -1 [or co 5 1], we write A2? [or APO] instead of A53, and II “pm [or II “qu instead of II “pm. We also write dma(z) = (1 - I212)“ dm(z). The set of (equivalence classes of) measurablefunctions satisfying the integrability condition defining AZ? is denoted by L23. It is easy to check that it + 9|!ng —<. llfllgm + Melitta where S = min{p, q, 1}; thus (A23, ll NEW») and (LEE, ll Ilgfq’w) are metric spaces, and are normed linear spaces if 1 s p, q s 00. The basic reference for mixed norm spaces (including, but not limited to, our spaces LIZ?) is Benedek and Panzone, [2]. We will follow the usual practice of writing c and C for positive constants ("small" and "large" respectively) that may vary from line to line. Dependence on some parameter(s), for example p and N, may be emphasized by writing C = C(p, N). If two positive quantities A(x) and B(x) have ratio bounded above and below as x ranges over some index set X, we say A(x) and B(x) are equivalent, and we write A(x) ~ B(x) for every x e X. For example, (1 - r2) ~ (1 - r) for every 0 s r s 1; this particular fact will be used repeatedly without mention. Note that by two applications of Holder's inequality, Li‘s“ C LE}? ifehher p2 5. p1 and q2 < q1 and (0:1 + 1)/q1 < (a2 + 1)/q‘2 or p2 5 p1 and q2 =q1 and 0:13 a2. In either case, the containment is proper (unless p1 = p2, q1 = q2, and a1 = (12), since then there is some 3 satisfying N/p1 + (or1 + 1)/q1 < s < N/p2 + (ct2 + 1)/q2, and f(2) = (1 - (2, C))'5 (with Ce 8 fixed) defines a function in A5322 not in Alas“: Ilill ‘4 = I. (IS I1 - for every 2 e B for some C independent of f. Prggf : First suppose 0 < p < 00. Since |f|P is subharmonic, for 0 < r < p < 1 and 13 e S we have Ittrolip 5 Is |f(pnll" P((r/p)i:. n) dam) s 2”(p-r)‘NIs |f(pnllpd6m). (2.1) Iiirrliip- W” s Cllfpll Ins, Here P denotes the invariant Poisson kernel defined for z e B and t; e S by Ptz. i.) = ((1 'lZ|2)/|1 -op2~-i up s anti... Letting x = (p - r)/(1 - r), for 1/2 3 r <1 it follows that > |f( row: (1 - r)(N’P+ (Mil/shit, 1 qu/p (1 - x)“ [(1 - r)x + r12N1dx ~ "(mud (1- r)(N/p+ (a+1)q)q J01 qu/p(1_x)a CIX Cllfllpqa so the result follows. If 0 s r < 1/2, the result follows from the maximum modulus theorem. Now suppose p = 00. Then |f(r1:)| s llfpll L°°(S) for 0 s r s p < 1, and the result for 0 < q s 00 is proven by the same procedures. 0 This growth estimate will also be a consequence of Theorem 3.3.1. r ll 1.2.2 : A? is a closed subspace of Li? (0 < p, q s 00, -1 < a), and is hence complete. 80 A3)? is a Banach space if 1 ._<.. p, q s 00. Prggf : Suppose fn —> f in LES with tn 6 A35. By Proposition 1.2.1 fn is uniformly Cauchy on compact subsets of B, so fn is uniformly convergent on compact subsets of B to some 9 since L3? is complete (see [2], p. 304). But g is analytic _ - p ([15], 1.1.4) and f _ g a.e., so g 6 Ag? and fn —> g in A03. El Prgpgsitign 1.2.3 : If f e Afj (o < p, q < oo), then [iii] llfr-fllp’w = o. This follows immediately from the dominated convergence theorem. (For details, see [16], Proposition 3.3.) So the functions analytic in a neighborhood of B form a dense subset of A23. Th N ni r i M ri n h P h Ii "Metri" There are several notions of "distance" in BN (or B1,, or SN) and each has its own advantages. We will have occasion to use three. The isotropic metric will refer to the usual metric in if“, and B(z, r) will denote a corresponding ball, i.e., B(z, r) = {w 6 (EN | )z - W| < r}. The nonisotropic metric d is defined on B]; by d(z, w) = (1 - (z, w)(1/2. It satisfies the triangle inequality on B7] and is a metric on SN; see [15], 5.1.2. Define 5(0, 5) = SN, and for 5 > o, p e (o, 1), and n e SN, define §(pn, 5) = {1: e SN | (on, n))2 < 5(1 - p)}. Note that oénm, 5) ~ 5N(t - p)”; see [15], 5.1.4. The pseudohyperbolic "metric" p is defined on BN by p(z, w) = |w(z)| where (Dw is the automorphism of BN given for w #5 0 by (r - 21)2 + (1 - r2))z'I?-, i.e., 2r(1 - 82)Re 21 > (r2 - 82) + (1 - 82r2)|z1|2 + (1 - r2)|z'). Now, 4rRe 21 + r212]2 < r2 + 4r|z1| - r2|z1i2 3 4r < 4, so (r2 - 82) + (1 - 82r2))zi2 = ((r2 - 82) + (1 - 82r2)|z1)2 + (1 - r2)lz’(2) + r2(1 - 82)Iz')2 < 2r(1 - 82)(Re 21 + riz')2/2) s 2r(1 - 82)()z1)2 + rlz'IZRe z, + r2lZ'I4/4)“2 < 2r(1 - 82)()z1|2 + )z')2)1/2 = 2r(1 - 82)|zl. Hence ([2], 0') e E(r, 8), and (r - 8)/(1 - r8) < [2) < (r + 8)/(1 + r8). 0 CHAPTER 2 Most of the results of this chapter are generalizations of work of Luecking in [11]. Section one deals with boundedness of the Bergman projection, and this result is used to identify the dual Space of our mixed norm spaces in section two. Sections three and four are concerned with representations of the mixed norms and of functions in the mixed norm spaces. §1 Boundedness of the Bergman Projection on L3? Suppose s > -1. The Bergman kernel Ks is defined by Ks(z. W) = (1 - lWlZIS/(l - <2. W>)N+1+s forz, we BN. Note that: (a) for fixed w e B, Ks( - ,w) 5 Ali? and (b) for fixed 2 e B, Ks(z, - ) 6 L53 if II (1 - r2)$‘lco(r)r2"“'1 dr < 00, 9.9., if co(r) ~ (1 - r2)“ with sq > -(a + 1). (But Ks(z, - ) is not conjugate holomorphic unless s = 0.) Both observations follow because the respective denominators are bounded above and below in B. The Bergman projection Ts is defined by 10 11 Tsf(z) = (N a S) L, Ks(z, w)f(w) dm(w) for z e BN and f for which the integrands are in L‘(dm). In general, the binomial coefficient (N NS) is I‘(N + S + 1)/I‘(N + 1)I‘(s + 1). It is clear that, for fixed S, Tsf is holomorphic when defined. In this section, a condition on s, p, q, and on will be found which ensures that Ts is bounded on LEE; there will be no dependence on p other than p 2 1. In [7], Forelli and Rudin Showed that Ts is bounded on LP(dm) (1 s p < 00) if and only if (s + 1)p > 1. Then Békollé ([1]) showed that Ts is bounded on LP(dma) (1 < p < 00, -1 < a) if and only if (s + 1)p > a + 1. (He actually showed this for more general weights satisfying a ”8,, condition”, a condition analogous to Muckenhoupt's Ap condition introduced in [13].) An important tool will be the following pair of facts due to Forelli and Rudin in [7], Proposition 2.7: (1.1a) I8 |Ks(z, w)|(1 - |w12)‘° dm(w) .<. C(1 - (2)2)°°for every 2 e B if 0 < c < 3 +1; (1 .1b) I8 |Ks(z, w)|(1 - (2|2)'° dm(z) 5 C(1 -|w12)cfor every w e B if 0 < c + s < S +1. Theorem 2.1.1 : Ts maps LEE (1 s p s 00, 1 < q < 00, -1 < or) boundedly into AZ? if (s + 1)q > on + 1. Furthermore, Tsf = f and Tsf a f(0) for every f e Afifl. Proof : As noted in [15], Proposition 7.1.2, Tsf = f and TSTEITE) is true for is H°°(B), hence for f e A? by density of H°°(B) in Af’xq, once continuity is vefified. If 1 < p < 00, vector-valued integration and HCIder's inequality yield that H (1.30,“ Lp(S) = CHI] IS Ks(r ' t mepm) dG(TI)p2N-1 deILP(S) 12 s CI. II-Is Ks(r- .Pnlfpm) domilltpapm‘ dp =c I. (IS IIS Kart. Pnlfpm) domll" dott))1’9p2N"dp s C II [IS (IS le(r’c. pnlllfptan dcml) ><(IS IKSUI. on)! d0(n))p’p'd0(t)]“°pz”" do- But 3 IKs(l"l:, pn)| dam) is independent of 1:, so by Fubini's theorem, the expression above is less than cI. [(ISIK.Irr. pn)l d0(n))p""+ 1(IS prmllp do(n))]"ppz”" dp = cl . I lesm. pn)l doth) Iliplltp.s.p2N-‘ do This estimate can also be verified in a similar way if p = 1 or 00. Using this estimate and Ho'lder's inequality, we have ||Tsf|| 3,... = oi. ||(Tsf).|lEp(s)(1 - Wit 3 CI . [I . IS )Ksm, pm) dom) Ilfplle(s)p2N-1 dp]q(. - ,2)a,2N-t d, s cI. (IB IKs(rt. pniiii 12)-.. dm(pn))°/q' ><(IB le(r'r. pn)l(1 -p2>tqlli.,l|Ep.s) dm(pn))(1 - recto“-1 dr. where 8 will be Chosen later. But Is leirr. pnllii - pzl‘i’q' dm(pn) S C(1 - r2)“ by (1.1a), as long as 0 < 8q' < s + 1. Using this and Fubini's theorem, we have llTsill 3..., 13 < cI.( ((1 - r2>-11')1/1'(IBIK.Irt. pn)l(1 -p2>11II1.,IIEp.., dm(pn))(1 - r2)11r2N-1 dr = cI. Ilip ||Epdm(n) 5 C(1 - p2)'('a+5QI = C(1 - p2)a-8q by (1.1b), as long asO<-a+8q+s111p2-=~1dp Cllfllq PQ‘X pq,'o< To choose suitable 3, note that there exists 8 satisfying O<8q'0t+1. [I As in [7], p. 594, we immediately get the following. Qorollam 2.1.2 : For1_<_p<°°,1(or+1)/q - 1. Let u = Refand fix 0 < r, p <1. Then fp = Ts(fp) = Ts(fp + fp) = 2Ts(up), so Is |fp( rt)lpdo() )=2PIST |Ts (r)t|pdo 1:). Thus “I”:q o. =I. (SI Ifp (rt) [9 do“ ))q/p(1 _r2)ar2N-1 dr = 2“ I ( s [Tsup (r1: )|9 do( ))q/p( 1 _ r2) 01er 1 dr =2qllT.U pllq <2‘W‘llup llq PJI‘X- FUN and the result follows upon letting p —> 1. Cl The "inner norm" LP(S) was not critical in Theorem 2.1.1. If N = 1, the Bergman kernel satisfies Ks(re‘°, pelt) = Ks(rei(e ' (P), p) and a change of variables is possible, so LP(S.) may be replaced by any Banach space X on 81 satisfying || FeIIX s CH F||X for all 6 e [0, 21:) and for all F e X. (Here, and only here, we write Fe forthe function defined on S1 by Fe(ei‘P) = F(ei(‘p ' 9)). No confusion with fr should result.) The beginning of the proof is then ”In K. Ire" pe‘111.I e19) dellx= llIn Ks(r. pate-111N211) dellx =||InK.( Krpei1)I1...)I (e') dHX< <0lli.llxI..IK.Ir.pe11)Id

1,this can be imitated to some extent. Write e1 = (1 , 0, . . . ,0) 6 SN. For 16 8, let III be a unitary transformation on S (i.e., (11111., [11112) = (n1, n2) for every 711,112 15 S) with [1181 = 1:. So 15 I S K.(ri. ptlfphil don) = Is K.(rl1."1:. pu."vlf.(v) don) = IS K.Ire.. pnli.Iu.n> doInl where n = 11.47. If X is a Banach space on SN satisfying (1.2) II F(u,n)II X s CII F(-)IIX for every n 6 SN and every F e x, then III. K.Ir- . pvl1.Ivl doIvlllx s C "1.1). I. lK.Ire.. pnll dam). The inequality (1.2) is trivial when X = C(SN) for any N. When N = 2, we may take ‘1 “‘2 “1: = .. T2 ”‘1 A computation then shows that It. - 1:2] = “‘11“ - [.1121] I for every 1:1, 12, n e 82, so that (1.2) holds when x = LipaSZ, o < a s 1. (Recall that Lipa82= {fe C(82) I "(1:1) -f(1:2)I/II1- tzla < K(f) < 00 for all 11, 1:26 82 with 11¢12}.) §2 Representation of the Dual eeeee (21A;q Representation of the dual space of AI”: will follow from boundedness of the Bergman projection (Theorem 2.1.1). The case N = 1, ct = 0 was handled by Shapiro in [16], Corollary 3.6. In [11], Theorem 2.1, Luecking identified the dual space of Ag using the boundedness of the Bergman projection on A: and P ANN”. - p’cl’ leen 9 e Autioq’f Lgf = (f, g) = I315 dm for f e AE’Xq. By two applications of Hb'lder's inequality, I define the linear functional Lg on A2? by 16 KI: g>I S IIfIIp,q,aIIgIIp',q',a(1-q°)' Theorem 2.2.1 : Suppose that -1 < or, 1 < p < 00, and max{1, a + 1} < q < 00., Then the map taking 9 to L9 is a linear homeomorphism of Agg:q,)onto the m dual space of A,x . Emof : As noted above, any 9 e Azgjqqdefines a bounded linear functional Lg on Afij, with I LgII .<. “9 up...“1 _q.,. Now take any L e (Agjf. Extend to L e (Eff by the Hahn-Banach theorem. Write 03(r) = (1 - r2)“, and note thatj e Leo if and only if j/oa”q 6 LEE. So define A e (qu). by A] = L(j/m"q); then there exists some k e U” such that A] = I B jk dm. (See [2], Theorem 3.1 forthe generalized representation theorem.) Let h = REST/'5. We have h e Lg’gfq,)and Lf = (f, h) for all f e LEE. Since K0(z, w) = Ko(w, z), Fubini's theorem implies that (2.1) (101., 12) = (f., Tofz) for 111 6 LE:1 0 L2 and 12 e Lg’gfq,)n L2. (To justify the application of Fubini's theorem, note that Tot1 and Tot2 are in L2 since f1 and 12 are, either by Theorem 2.1.1 or by Békollé’s result.) Now, q > at + 1 and q' > a(1 - q') + 1, so by Theorem 2.1.1, To is bounded on La? and Liam By continuity of To and density of the respective spaces ([2], p. 308), (2.1) is also true for f1 6 LIZ? and (2 E [$ng Let g = Toh. 80 g e Agar” and forfe Ali? we have Lf = (f, h) = (Tot, h) = (f, Toh) = (f, 9), Le, L = Lg. If g e Ai’giqqdetines the zero functional, then since Ko(z, -) e A? for any fixed 2 e B, we have 0 = (Ko (2, -), g) = To g(z) = 97?), Le, g a 0. So the map taking 9 to L9 is a one-to-one, continuous, linear transformation of Agfiiqqonto 17 (Af’xqf. By the open mapping theorem, the map is actually a linear homeomorphism. Cl One can use other 0.9., weighted) duality pairings (and other kernels) to - PR get other representations of (Au) §3 Two Norm-Reoreeentetion Theoreme In [11], Theorem 5.1, Luecking shows that km II‘IIIHp ~ (sup kZ:1|f(amk)IP(1 - rm)N)1/P for all f e H9 where 0 s r0 < r1 < . . . —> 1 and {amk} satisfies (1)1amk|= rmforeach m=0, 1,2,. . .and each k= 1, 2, . . . ,km, (2) rmSN C LkJE(amk, 8) for each m for some 8 = 8(p) sufficiently small, and (3) E(amk, e) n E(amkv, e) = o for each m and each k¢ k' for some 0 < e < 8. Such a set {amk} will be called an 15-8 lattice; notice that this differs slightly from Luecking's use of the term, for he requires the condition BN = knJLkJE(amk, 8) instead of (2). A close analysis of Luecking's proof yields the following. Theorem 2.3.1 : Fix 0 < p < 00, 0 < q < 00, and -1< on. Let rm =1 - 2"“ for m = 0, 1, 2, . . . and suppose {amk} is an c-8 lattice for 8 = 8(p, q, or) sufficiently small. Then 18 00 Ilfllp’q’a~ ( Z (k )i(amk)lp2-mN)q/22-m<2+1l)1/1i for everyte AEE. Proof : Write Emk = E(amk,s 6,) Am = UE(amk,e e),r me- =(rm + c)/(1 + r me) and m. = [(rm - e)/(1 - rme), (rm + e)/(1 + rme)). Then by subharmonicity of IfIP, the separation property (3), and Lemma 1.3.1, §|f(rna k-)|22 111“ <2 mN(z C Em k 1112 dm /m(E Emk)) s 02 mN2m1N+1l gIEmk IfIP dm = C2111IAm IfIF’ dm = C2mIlm8 (IS |f(r1c)||° d1, (2) {am} is an e-8 lattice for some a and 8 sufficiently small (8 = 8(p, q, K) where K is as in (6) below), (3 (4 ( (rm +1)/2 < r "HM for each m = 0, 1, 2, . . .for some integer M, |(rm -rm -r m rm)| >Syforeach m¢m' forsomeO -1. Conditions (3) and (4) say that rm —> 1 "not too slowly", while condition (6) says that rrn —-> 1 "not too quickly", at least for weights 0) with suitably controlled growth. Theorem 2.3.2 Szuppose 0 < p < q < 00, conditions (1 )- (7 ) hold, and UUE(a 5)c G c 8. Then IIfII amk, ~ IIfoIID'q’m for every fe ASE. moo fleet : Since we may assume that y < 1/3, condition (3) yields rmM_2rm -1 <(rm -y)/ (1 -r mm1y)<(r +y)/(1+rmy)S(rm+1)/2.<_rm+M. Then, as noted in the proof of Theorem 2.3.1, Luecking actually shows that cllfrmll to... s 061111....” It... +5 |f(amkllp(1 -r...lN so CR ”Inn“ EPIs)w(rmlrm2”“(rm - in.-.) ‘- 05? IIfrm+MIIEP(S)m(rm)rm2N'1(rm - n.-.) + 2 (§( |f( amkllpU - r...)N)“’F’co(rm)rmZN'l(rrn - rm) < K0511: ”frmllq M90) m), m2N-1(rm _ rm) “1% (E213 |f( amkllpU ' r...)"’)“’pcn(rm)rm2""1(rm - rm_1 ) by condition (6). Thus for 8 small, 21 Z IIfrmIILP(3)(°(rm Irmz NIIm " r"1.1) s 05 (.2111 2....ll1I1 - r...) '1rl11wtmirmZN-1Irm - r...) (The reverse inequality is also true but is not needed here.) Write lnn = [rm, rm“), Emk = E(amk, 7), Am = 9513111“): and my = [(rrn - y)/(1 - rmy), (rm + y)/(1 + rm'y)). Then using condition (5) and the above estimate, lili..= .2. 1.11 l1 .npeo 21-1 S 0:50 IIffm+1IILP(S)w(rm+1)rm+12N-1(rm+1 - Irm) s cg (g |f(amk)|P(1 - rm))N)2/po(rm)rm2N-1(rm - rm). By subharmonicity of mi), disjointness of the Emk's, and condition (7), the above sum is less than cg (g (1 - rm NI Em, 11111 dm /m(Emk))q/Pco(rm)rm2N'1(rm - rm_1) s cg(( (1-r M)-1I rnmr|i|r>dm)11/i>ro(r) rmZN-1Irm-rm_,) $02 (I IS II(f’t) Ip xAm(rt) do(1: ) (It)(r)lrr2""1 dr)q/P. Finally, using Jensen's inequality (since q/p 2 1) and disjointness of the les (condition (4)). this is dominated by 0% I I (IS |f(r1c)|p )(Am(r1:) do(i:))‘i’pco(r)r2”1 dr 5 cg I lm.(Is |f(rt)|p xenon) do(t))q/pro(r)r2N-1 dr 5 CII (IS II(l"t)Ip xG(r1:) do(1r))‘i’po)(r)r‘ZN'1 dr 22 Luecking shows in [10] that IIIIIW ~ II foII p,a for every f 6 Ag if and only if (3.1) ma([D n B) ~ ma(G n B) for every isotropic ball B centered on li when N = 1, p = q, and (00') = (1 - r2)01 with or > -1. (He also gives a more general result of the same nature in [11].) In this case we can also show directly that conditions (1) - (7) along with LIA) E(a 8) C G imply (3.1). The key is the mk1 geometric estimate km 2 C(rm2 - 82)/(1 - rm?) (m it 0) where c = C(8, r1). §4 Reoreeentetion of A125 Fonotione The duality result (Theorem 2.2.1) and the equivalence of norms result (Theorem 2.3.1) can be used to obtain a representation of Ag? functions as sums of kernel functions. This generalizes Luecking's Corollary 4.4 in [11]. If p is a weight function on {0, 1, 2, . . .}, we write c = {ka}m,k e Ill;q if 0° K“ / 1/ (mgo (Kzfl 'ka'p)q pum) q = ”C” 9.0.1) < 0°" Jheorem 2.4.] : Suppose that 1 < p < 00,1 < q < 00, and -1 < a. Let rm =1 - 2m and cm = (1 - rm)1 + Nq'lp't 01(1‘11'lrmZN'1 for m = 0, 1,2, . . . , and suppose {amk} is an 2-8 lattice for 8 = 8(p, q, to) sufficiently small. Then every f 6 A? is of the form 23 K 0° '“ N 1 “2) = mgo k2“ ka‘UmU-(Z, amk»- - for some C e tiff, and any f of this form is in Nix”. Note that no claim of uniqueness of c e If? is being made. Proof : AS in the proof of Theorem 2.3.1, IIgIIp',q',a(1-q°)" (m( Z(§ |g(a mk)Ip) )Q/P (1 - rm)1+NqH/p +oI(1-'mq)r 2N- -'1)1/q i.e., IIgII p',q',oi(1-q') N IIg( amk) II p',q',t)' Thus the map R. A111 -> 119:" defined by (R9)...k = g(amk) is a linear 0([1- J isomorphism. Hence :1 is one-to-one with closed range, and R‘: 113:1 —-> All? is onto. (Since max{1, a(1 - q') + 1} < q' < 00, we have(AEq‘I :1?”qu by Theorem 2.2.1, where the duality pairing does not involve a weight, and we have (tips) ~ 111:? by Theorem 3.1 of [2], where the duality pairing does involve the weight 1).) To identify R*, take g 6 A5“? q )and c e ll‘fj, supposing first that C has only finitely many nonzero terms. Then I B IR‘cig dm = IR‘c. g) = Ic. Rg) = g (; c..,..dIa1.,.l)1>m = g go...» ml}. gIz )(1 -Ia.....z>l-N-1 dm(Z) =IBm( (Z i: cmkomfi - (z, amk))'N’1)g z) dm(z), so R C(Z =2 g cmkom( (-z, amk))‘N'1. To get the result for general c e 113:1, use finite approximations to c (for which the result was just verified), the continuity 24 of R*, and the fact that convergence in AZ? implies pointwise convergence. 0 CHAPTER 3 This chapter is concerned with "Carleson measure theorems". Some of the classical results are described in the first section, some estimates (mostly geometric) are derived in the second section, and the third section is devoted to the statement and proof of the main theorem. Corollaries and related methods and results are given in sections four and five. §1 §Qme History In the course of proving the corona theorem in [3], Carleson characterized those finite positive measures u on B1 such that (J31 If]p du)”p .<. C||f|| Hp for every fe Hp (O < p < 00). He showed that this holds if and only if [IS 5 C(1 - p) for every set S of the form 8 = Sp60 = {rei9 | p .<. r<1 and 90 - 1t(1- p) 59 < 00 + 1t(1- p)}; such a measure It is now often called a Carleson measure, and such sets 8 are called Carleson sets. The necessity of this geometric condition is easily shown by the proper choice of a function f e Hp which is suitably large on 8; this procedure will be demonstrated in the proof of our Theorem 3.3.1. Carleson‘s proof of the sufficiency of the geometric condition used a complicated covering argument. Hormander ([9]) derived a version for more general regions in it“ using a maximal function, Marcinkiewicz interpolation, and a simpler covering argument. Using some of Hormander’s ideas, Duren ([5]) generalized the theorem to the following: 25 26 (L3 Iflp2 du)1’92 .<. Cllflal1 for every f e H91 (0 < p1 s p2 < 00) if and only if us 3 C(1 - p)|°2’PI for every Carleson set S = Spoo- The results mentioned so far have concerned the Hardy spaces; i.e., measures on B are compared to ”measures on 8". Other results have been gotten concerning the (weighted) Bergman spaces; i.e., measures on B are compared to measures on B. For example, there is a theorem due to Hastings ([8]) for the polydisc lDN (the product of N copies of [D = 8,): (IBM [flpz dp)1/pz _<_ C(Jmulflpt dm)"PI for every analytic function f on [DN (0 < 91 -<- 92 < GO) if and only if us 3 C'[(1 - p1) - .(1 - pN)]292’PI for every set S ofthe form 8 = Splemx- - «8390". The result of Luecking in [11], already discussed at the end of Section 3 of Chapter 2, can be viewed as a Carleson measure theorem for the measures demainduced by "large enough" sets G in B1. Cima and Wogen proved a Carleson measure theorem for weighted Bergman spaces in BN ([4]); the Cima-Wogen theorem is a consequence of Luecking's general technique in [12], and also of the proof of the main result here (see Theorem 3.4.3). The main 27 result here, Theorem 3.3.1, is for weighted mixed norm generaliZations of Bergman spaces in I”, and is thus of the second type mentioned. §2 ngg Estimates Recall from section 3 of Chapter 1 that for p e- (0, 1), n 6 SN, and 8> 0 we defined B( (apt), )-.-{t e le |(d(1:, 11))2 < 5(1 - p)}, where d is the nonisotropic metric on sN given by d(1?, n) = H - (1:,11)|1/2;We also defined Rm, 6) = 3N. Also recall that oB(pr), 8) ~ (1 - p)”. (Now the constants of comparability involve 8.) Our first lemma is the construction of a "nice" covering of S by sets B. Lemma 3.2.1 : Suppose p e (O, 1) and 8 > 0 are fixed. Then é(pn1, 5), . . . , §(pnkp, 8) can be chosen inductively so that (1) S C 91911108). (2) B(pm, 8/2), . . . , B(pnkp, 8/2) are pain/vise disjoint, and (3) no point of S is in more than L of the sets B(pnk, 8), where L = L(N, 8) < 00 isindependentofp. M : In the induction scheme, if there exists some n e S \ LkJB(pnk, 8), then add B(pn, 8) to the collection; condition (2) will continue to hold because d is a metric. The scheme will terminate in finitely many steps because oB(pnk, 8/2) >c(1 - p.)N oS =1, and (2) holds. To demonstrate condition (3), take any point I] e S; then B(pr), 28) contains all of the sets B(pnk, 8) which contain n because d is a metric; but (2) holds, oB(pnk, 8/2) 2 c(1 - p)N , and C(1 - p)N 2 cam 25). El 28 The geometric facts above do not depend strongly on the particular metric being used. However, the nonisotropic metric is being used here because of its close connection with (the denominator of) the invariant Poisson kernel P(z, c) = ((1 - Iziz)/|1 - (2, QB)". in particular, it allows the following argument. Fix f e H(BN) and r0 6 (O, 1). Choose a positive integer M so large that 8 <1 - 2"M and then let R = 1 - (1 - ro)2'M. Note that O < r0 < R < 1, so there is no problem with the existence of fR on S. Define u on RB = {R2 | z e B} by Ulr’r) =13 lfn(C)Ip((R2 - rzi/IR - l"2+l1-|"2+l1-l"2 +l1-l“2 S (1 - ro-)1l2 + 51/2“ - ro)1/2 + (1 , rov)1/2 +11 _ (ro'Tl. 011/2 5 (1 - To')“2 + (1 - 2"“)1’20 - r0)”2 + (1 ~ [dim + I1 -I2 = (1 - ro'll - Rea. Z2)) S((2M - 1)/(2M'1 - 1))2(1 - r'll - Rah. Q) S C|1 - (r'T, QIZ. So u(z‘) ~ u(z) follows as before by integrating. The claims made above also hold if r0 = 0; some of the estimates become simpler. D We will also need the following. 30 Lemma 3.2.3: Fix a, b, c e lR satisfying 0 > -1, b < -1 - c, and a < -1 - b - c. Then for 0 s p s 1,I1°°((1-p)x + p)a xb (x - 1)° dx is finite and bounded above by a constant C = C(a, b, c) independent of p. Prgof : Use the fact that 1 s (1-p)x + p s x, consider the cases a < O and a 2 O separately, and write I 1°° =11? + .12”. D §3 A Qarlesgn Measgre Thegrem With the preliminaries disposed of, we proceed to the statement and the proof of a Carleson measure theorem for mixed norm generalizations of Bergman spaces in the unit ball of it”. Thegrem 3.1: Suppose O)l’qz s cllillpn... for every t 6 Ali“. (3.2) (p(é‘xpn, 5)))1/p(v([p, 1)))1/Q2 3 C(1 - p)N/p + (wt/qt for every n e s and every p e [0, 1). Proof :To showthat (3.1) implies (3.2), fix r) e S and p 6 [1/2, 1). (For p near 0, (3.2) is true with large enough constant 0' since It and v are finite measures.) Let w = pr) and define f(2) = (1 - (z, M)5 where s > N/p + (a+1)/q1. Take 2 = r1 where 31 p < r <1 and ‘t e B(w, 5) and let 2' = p‘t. Then |1 - (z, w)|“2 .<. H -(z, z')|1’2 + |1 - (2', MI"2 s I1 -<2, 2W2 + (l1 -l + Kn. t) - (ml. pt>l)"2 s <1 - rpl12 + (5(1 -pl + <1 432))“2 s C(1 -p)"2. i.e., |f(z)| > C(1 - p)'5 for such 2. So the left-hand side of (3.1) is greater than (I91 (Iéipn. 5) C(1 ' Pi's" dm(w))‘h’p dv(r))1/qz = C“ ' Pi's(u(B(pn. 8)))"P(v([p, 1 )))1/,-1 O, p e (O, 1), and n 6 SN, define B(pn, 8) = {’C 6 SN) I‘C - n| < 8(1- p)}. Note that o(B(pn, 8)) ~ 82N"(1 - p)2N". Considerthe two conditions (5.1) (I. (is If,(r)lp du(‘t))q2/p dv(r))1/Q2 s Clllllp,q,,a for every t e Aliflt, (5.2) (u(étpn. 8)))""(V(lp. t)))“qz s C'(1 - p)‘2”'1”°*(“*”’qi for every n e s and every p e [0, 1). Asusual,wesuppose0 1/(2 - y). For m = 0, 1, 2, . . . let rrn =1 - yr" and Rm =1 - W1“, and let um be the least harmonic majorant of |f|p on RmB. Fix zm = rmn and z = r1 with rm .<. r < rm+1 and t e g(zm, 8). Note that [z - zml .<. [1'12 - l’m‘tl + lrmn - rm'rl s (1 + 8hrm - Ym‘1 - 872'“. Let am = y’" - yr” and bm = am - |z - zml. Recall that B(z, r) is an isotropic ball; i.e., B(z, r) = {w 6 [EN | (z - wl < r}. Then, since we may assume 8 < (y- 1)/y2, we have 1> bm/am 2(7-1- 572 + (”ZN/(72 - 1) > (7-1 - 8y2)/(‘y2 - 1) > 0, so m(B(z, bm)) ~ m(B(zm, am)), independently of m, and um(z) = 08(2. bm) um dm)/m(B(z, bm)) (m(B(zm, am))/m(B(z, bm)))()B(zm, am) urn dm )/m(B(zm, am)) 3 Cum(zm) IA by the ordinary mean value property (which is not true for M-harmonic functions, e.g., those gotten by integrating with the invariant Poisson kernel as in the proof of 38 Theorem 3.3.1). To get the other direction, let cm = 7”” - WW and dm = 0m - |z - zml. Then, since )M" > 1/(2 - y) and since we may assume 8 < (W'1(2 - y) - 1)/yM, we have 1 > dm/cm 2 (2)NH - yM - 1 - 5W + 5y'l/l-rii)/(y~'-1 - 1) > (W"(2 -1()- 1 - 51M)/(1(M" - 1) > 0. so m(B(zm, dm)) ~ m(B(z, cm)) and um(zm) s Cum(z) as above. We remark that if 1 s p < 00 and 1 s q1 .<. q2 < 00, "f e A?” could be replaced by "f positive subharmonic in BN" in the argument above. This method doesn't seem to work with nonisotropic balls B because the nonisotropic metric fails to give adequate control in all directions. This manifests itself in the argument above in ”radii" bm and dm that may fail to be positive. We close with a generalization of Hastings‘ result in [8] for the polydisc. Thegrem 3.3.1 : Suppose O < p < 00, 0 < q1s q2 < 00, and -1 < a1, . . . , aN, suppose 111, . . . , W are finite positive measures on ii = S1, and suppose v1, . . . ,vN are finite positive measures on [0, 1). Then the following two conditions are equivalent: (5.3) (Jr "J1 Utr- - in |f(r1e‘91. . . . . rNeieimp du1(61)~-de(eN))Qz/p dv1(r1)- . .va(rN))1/q2 S C((]: - 'L (In - a)“ |f( r1ei91, . . . , rNeieN)|Pde1- - ~deN)qr/p (1 ' r1)<11 r1dr1n-(1 - rN)°lN rN drN)1/qt for every function f analytic on ll)”, 39 (5.4) (111([901 - 1:51, 901 + 1:81)))“P x- - -x (ttho0N - 1:5,], SON + tr5N)))l/P x (v1([1 - 81,1)))1’q2 x. - ex (vN([1 - 8N,1)))1/q2 g (:5 1(1/p + (a1+1)/qr) x. . .x 5N(1/p + (aN+1)/q1) for every 901, . . . , 90M 6 Ti and every 81, . . . , 8N e (O,1]. grog: First fix 901,. . . ,OON a ii and 51,. . . ,5N e (0.1]. Let wj = (1 - 8j)ei90j for j=1, . . .,Nanddefine t(z,, . . . , 2N) = (1 - z,W,')~S. - -(1 - szfiys where s > 1/p + (ctJ-+1)/q1 for each j. Then |f(z1, . . . , 2N)| > 081'5- - -8N's if zj = rjeiei satisfies 6j e [901-- 1181-, 901+ “51) and rj e [1 - 8]., 1) for each j. (See [6], p. 157.) So (5.3) implies (5.4) as before. Forthe proof that (5.4) implies (5.3), fix ye (1, 2), choose M so large that W" >1/(2 - 7), write rmi =1 - yr") and Rmj =1 - yM'mj forj = 1, . . . , N, and write in = (m, . . . , mN) e {0, 1, 2, . . . }N. For each N-tuple m, let uan be the least n-harmonic (i.e., harmonic in each variable separately) majorant of |f|p on Rm1lD x- - -x RleD (see [14], p. 52). If ej e [90j - u(1 - rmj), 90]. + n(1 - rmj)) and rj e [rmr 'mj +1) for each j, then um(r1ei91, . . . , rNeieN) ~ um(rm1ei901, . . . , rmNeieou) by applying the geometric argument with isotropic balls given at the beginning of this section. (The argument is applied N times, one time on each "slice”.) One other needed observation (see [14], p. 52) is that 4O um(0) = )n- - J11 |f(Rm1el91, . . . , RmNeieNMp d631- - -d9N. Then the proof is completed in the manner of the proof of Theorem 3.3.1. [J When 1 s p < 00 and 1 s q1 s q2 < 00 the theorem is also true with "f analytic on 0”" replaced by "f positive N-subharmonic in [[DN". 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