THE PLANAR CANTOR SETS OF ZERO ANALYTIC CAPACITY
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1 JOURNAL OF THE AERICAN ATHEATICAL SOCIETY Volume 6, Number, Pages 9 28 S (02) Article electronically published on July 0, 2002 THE PLANAR CANTOR SETS OF ZERO ANALYTIC CAPACITY AND THE LOCAL T (b)-theore JOAN ATEU, XAVIER TOLSA, AND JOAN VERDERA. Introduction In this paper we characterize the planar Cantor sets of zero analytic capacity. Our main result answers a question of P. attila [a] and completes the solution of a long-standing open problem with a curious history, which goes back to 972. We refer the reader to [I2, p. 53] and [a] for more details. oreover, we confirm a conjecture of Eiderman [E] concerning the analytic capacity of the N-th approximation of a Cantor set. Before formulating our main results, we recall the definition of the basic objects involved. The analytic capacity of a compact subset E of the complex plane C is () γ(e) =sup f ( ), where the supremum is taken over all analytic functions f on C\E such that f on C\E. Although there has recently been important progress on our understanding of analytic capacity (see the survey papers [D], [V3] and the references given there), many basic questions about γ remain unanswered. One of the oldest is the semiadditivity problem, that is, the problem of showing the existence of an absolute constant C such that (2) γ(e F ) C {γ(e)+γ(f )}, for all compact sets E and F. If (2) were true, then one would have powerful geometric criteria for rational approximation, which are otherwise missing (see [V2] and [Vi2]). On the other hand, it has recently been established that a close variant of γ, called positive analytic capacity, is indeed semi-additive. The positive analytic capacity of a compact set E is γ + (E) =supµ(e), Received by the editors August 7, athematics Subject Classification. Primary 30C85; Secondary 42B20, 30E20. Key words and phrases. Analytic capacity, Cauchy integral, Cantor sets, T (b)-theorem, positive analytic capacity. The authors were partially supported by the grants BF , HPRN and 200- SGR The second author was supported by a arie Curie Fellowship of the European Union under contract HPFCT c 2002 American athematical Society
2 20 JOAN ATEU, XAVIER TOLSA, AND JOAN VERDERA where the supremum is taken over the positive Borel measures µ supported on E such that the Cauchy potential f = z µ is a function in L (C) with f. Since ( z µ) ( ) =µ(e), we clearly have γ + (E) γ(e). Since γ + is semi-additive, as shown in [T], it is clear that (2) follows from the inequality (3) γ(e) Cγ + (E), E compact C, where the positive constant C does not depend on E. Wewillseebelowthatour main result provides a proof of (3) for a particular (but significant) class of sets E. To the best of our knowledge, the first mention of (3) that can be found in the literature is in [DO]. An equivalent form of (3), which involves enger curvature, has recently been conjectured by elnikov (see [D]). NowweturnourattentiontoCantorsets. Givenasequenceλ = (λ n ) n=, 0 λ n /3, we construct a Cantor set by the following algorithm. Consider the unit square Q 0 =[0, ] [0, ]. At the first step we take four closed squares inside Q 0, of side-length λ, with sides parallel to the coordinate axes, such that each square contains a vertex of Q 0. At step 2 we apply the preceding procedure to each of the four squares produced at step, but now using the proportion factor λ 2. Then we obtain 6 squares of side-length σ 2 = λ λ 2. Proceeding inductively, we have at the n-thstep4 n squares Q n j, j 4n, of side-length σ n = n j= λ j. Write E n = E(λ,...,λ n )= and define the Cantor set associated with the sequence λ =(λ n ) n= by the identity E = E(λ) = E n. Our main result reads as follows. Theorem. The Cantor set E(λ) has zero analytic capacity if and only if (4 n σ n ) 2 =. n= The assumption λ n /3 for the Cantor sets E(λ) is purely technical. Actually Theorem (as well as Theorem 2 below) holds for any sequence (λ n ) n with 0 < λ n < /2. See Remark 2 at the end of the paper for more details. attila showed in [a] that the above condition is necessary and our contribution in this paper is to prove the sufficiency. The special case λ n =/4, n, was obtained independently by Garnett [G] and Ivanov [I] in the 970 s and, since then, the corner quarters Cantor set has become the favorite example of a set of zero analytic capacity and positive length. P. Jones gave in [J] an alternative proof of Garnett s result, based on harmonic measure. Recently Jones approach has been used to establish the vanishing of the analytic capacity of E(λ) forsome special classes of sequences λ =(λ n ) n= with 4n σ n tending to infinity [GY]. Theorem follows from a more precise result on the analytic capacity of the set E N = E(λ,...,λ N ). The asymptotic behaviour of γ + (E N ) is completely n= 4 n j= Q n j,
3 ANALYTIC CAPACITY OF CANTOR SETS 2 understood: for some constant C>andallN =, 2,... one has N C ( ) /2 ( N γ + ) /2 (4) (4 n σ n= n ) 2 (E N ) C. (4 n σ n= n ) 2 The upper estimate is due to Eiderman [E] and a different proof has been given in [T2]. The lower estimate was proved by attila in [a]. However, the result was not explicitly stated in [a], presumably because at that time the main object of interest was γ rather than γ +. An indication of how one proves the lower estimate in (4) will be provided at the end of Section 2. See also [E, p. 82]. Theorem follows from the upper estimate in (4) and the next result. Theorem 2. There exists a positive constant C 0 such that (5) γ(e N ) C 0 γ + (E N ),N=, 2,... If λ n =/4, n, then combining Theorem 2 with (4), we get γ(e N ) C N,N=, 2,..., which improves considerably urai s inequality [u] γ(e N ) C,N=2, 3,..., log N the best estimate known up to now. The main tool used in our proof of Theorem 2 is the local T (b)-theorem of. Christ [CH2], a particular version of which will be discussed and stated in Section 2. Section 2 also contains some basic facts on the Cauchy transform and the Plemelj formulae. The proof of Theorem 2 is presented in Section 3. Our notation and terminology are standard. For example D(z,r) istheopen disk centered at z and of radius r, ds is the arclength measure on a rectifiable arc and P Q means that C Q P CQ for some absolute constant C>. The symbols C, C,C,C 0,C,... stand for absolute constants with a definite value. We will also use the symbol A to denote an absolute constant that may vary at different occurrences. Remark. The second author [T3] has recently proved that Theorem 2 also holds for a general compact set. In particular, this implies the semi-additivity of analytic capacity. The proof in [T3] also involves an induction argument and an appropriate T (b)-theorem as in the present paper. 2. Background results 2.. Cauchy integrals. Fix an integer >0andletE = E(λ,...,λ )be the -th approximation of the Cantor set associated with the sequence (λ n ) n=. Then E is the union of 4 closed squares Q j, j 4,and E is the union of the 4 closed piecewise linear curves Q j. For a Borel measure µ supported on E set dµ(ζ) C(µ)(z) = ζ z, z / E, and dµ(ζ) C(µ)(z) = lim ε 0 ζ z >ε ζ z, z E,
4 22 JOAN ATEU, XAVIER TOLSA, AND JOAN VERDERA whenever the principal value integral exists. Let C + (µ)(z) (respectively, C (µ)(z)) stand for the non-tangential limit of C(µ)(w) asw tends to z from the interior of E (respectively, from the complement of E ). It follows from standard classical results that Cµ(z), C + µ(z) andc µ(z) exist for almost all z with respect to arclength measure ds on E. oreover one has the Plemelj formulae (see [V3]) { C + µ(z) =Cµ(z)+πif(z), (6) C µ(z) =Cµ(z) πif(z), where the identities hold for ds-almost all z E and µ = f(z)dz + µ s, f being integrable and µ s being singular with respect to ds. Assume that one has µ s =0and f(z) A, for ds-almost all z E, and that one wants to show (7) C(µ)(z) A, for ds-almost all z E. Then one only has to check that C(µ)(z) A, for z/ E, because then C (µ)(z) A, for ds-almost all z E, and thus the second identity in (6) gives (7) The local T (b)-theorem. The local T (b)-theorem is a criterion for the L 2 boundedness of a singular integral that was proved originally by. Christ in the setting of homogeneous spaces [CH2]. We state below a very particular version of Christ s result, which is adapted to the principal value Cauchy integral and to ameasureµ supported on E. The reader may think that µ is of the form µ = cds E for some (small) positive constant c. However, one should keep in mind that, for 4 n σ n, ds E does not satisfy condition (i) in the statement below with a constant independent of. As will become clear later, an appropriate choice of c is required to get (i) and (iii) with absolute constants. Theorem (Christ). Let µ be a positive Borel measure supported on E satisfying, for some absolute constant C, the following conditions: (i) µ(d(z,r)) Cr, z E, r>0. (ii) µ(d(z,2r)) Cµ(D(z,r)), z E, r>0. (iii) For each disc D centered at a point in E there exists a function b D in L (µ), b D supported on D, satisfying b D and C(b D µ) µ-almost everywhere on E,andµ(D) C b D dµ. Then (8) C(fµ) 2 dµ C f 2 dµ, f L 2 (µ), for some absolute constant C (depending only on C). The relevance of inequality (8) for our problem lies in the fact that it implies (9) µ(k) C γ + (K), K compact E, for some absolute constant C (depending only on C ).
5 ANALYTIC CAPACITY OF CANTOR SETS 23 The derivation of (9) from (8) goes through a well-known path: first, by classical Calderón-Zygmund theory one gets a weak (, ) inequality from (8); then, a surprisingly simple method to dualize a weak (, ) inequality leads immediately to (9). The original argument is in [DO]. Some years before [DO] Uy found a slightly different way of dualizing a weak (, ) inequality, which, however, does not yield (9) (see [Uy]). The interested reader will find additional information in [CH], [T] and [V]. Inequality (9) also explains why the lower estimate in (4) follows from attila s arguments in [a]; see Theorem 3.7 on p. 202 and the first paragraph after it. 3. Proof of Theorem 2 We first give a sketch of the argument. Assume that one can find a positive Borel measure µ supported on E N, E N = E(λ,...,λ N ), which satisfies (i) and (ii) with replaced by N, such that µ = γ(e N ) and the Cauchy integral is bounded on L 2 (µ). Then we get (9) with replaced by N, as we explained in Section 2. For K = E N (9) yields γ(e N )= µ Aγ + (E N ), as desired. In the actual argument we do not construct µ on E N. For reasons that will become clear later, we are forced to work in E with smaller than N. On the other hand, cannot be much smaller than N, because in the course of the subsequent reasoning one needs to have γ + (E ) Aγ + (E N ). Hence has to be chosen carefully, in such a way that the local T (b)-theorem can be applied to get the boundedness of the Cauchy integral on L 2 (µ), with an absolute constant. Now we start the proof of Theorem 2. Set a n =4 n σ n and S n = a 2 + a a 2. n We can assume, without loss of generality, that for each N>, there exists, <N, such that S S N (0) 2 <S +. Otherwise S N 2 <S and thus, by (4), γ + (E N ) A λ. On the other hand, taking into account the obvious estimate of analytic capacity by length, we clearly have γ(e N ) γ(e ) 2π length( E )= 8 π λ. Therefore (5) is trivial in the present case, provided C 0 is chosen to satisfy C 0 8 π A. Assume, then, that (0) holds and let us proceed to prove (5) by induction on N. ThecaseN = is obviously true. The induction hypothesis is γ(e n ) C 0 γ + (E n ), 0 <n<n, where the precise value of the absolute constant C 0 will be determined later. We distinguish two cases. Case : For some absolute constant C, to be determined later, () a γ(e(λ +,...,λ N )) C γ(e N ).
6 24 JOAN ATEU, XAVIER TOLSA, AND JOAN VERDERA Case 2: () does not hold. We deal first with Case 2. By the induction hypothesis applied to the sequence λ +,...,λ N and by (4) we have γ(e N ) C a γ(e(λ +,...,λ N )) C C 0a γ + (E(λ +,...,λ N )) C C a 0A ( N (4λ + 4λ n ) 2 Clearly, the inequality S S N 2 ( N and so, again by (4), n=+ = C C 0A( N ). /2 a 2 n=+ n a 2 n=+ n is equivalent to 2 ) /2 ( N ), /2 a 2 n= n ) /2 γ(e N ) C C 0Aγ + (E N ). If C = A, wherea is the constant in the preceding inequality, we get (5), as desired. Now let us now consider Case. Set γ(e N ) µ = length( E ) ds E, so that µ = γ(e N ). To check condition (i) in the local T (b)-theorem of Section 2, we consider two cases. If r σ,then γ(e N ) µ(d) 2r Cr, length( E ) because γ(e N ) γ(e ) length( E ). For r>σ we can replace arbitrary discs centered at points in E by the squares Q n j,0 n, 0 j 4n. In other words, it suffices to prove (2) µ(q n j ) Cl(Qn j ), 0 n, j 4n. To show this, given a disc D of radius r centered at z E, one considers a square Q n j D, wheren is chosen so that l(qn j ) is comparable to r. Then, µ(q n j )=γ(e N ) 4 n = 4γ(E N) length( E n ) l(qn j ) 4γ(E n) length( E n ) l(qn j ) 2 π l(qn j ), and so (2) is proved. It is also a simple matter to ascertain that (ii) holds.
7 ANALYTIC CAPACITY OF CANTOR SETS 25 Now our goal is to prove that hypothesis (iii) of the local T (b)-theorem is satisfied. Once this has been verified, (9) applied to K = E yields (3) γ(e N )= µ Aγ + (E ) A S /2 Assuming that (3) holds, to complete the proof we again distinguish two cases, according to whether /a 2 + is greater than S or not. If /a 2 + >S,then and so Hence γ + (E + ) S + = S + a 2 + S /2 + a 2, + a + = 4 length( E +). γ(e N ) γ(e + ) 2π length( E +) γ + (E + ) γ + (E N ), and thus (5) holds for a sufficiently big constant C 0. If /a 2 + S,thenS + S and so γ + (E N ) S /2 N S /2 which gives (5), with a big enough C 0,by(3). Summing up, we have reduced the proof of Theorem 2 to checking that hypothesis (iii) of the local T (b)-theorem is satisfied. As we already remarked when dealing with hypothesis (i), in proving (iii) we can replace discs centered at points in E by squares Q n j, j 4n,0 n. In other words, it is enough to show that, given a square Q n j,0 n, j 4n, there exists a function b n j in L (µ), supported on Q n j, satisfying bn j and C(bn j µ) dµ-almost everywhere on E and such that µ(q n j ) C b n j dµ. Let f be the Ahlfors function of E N. Then f is analytic on C\E N, f(z), z / E N, f( ) =0andf ( ) =γ(e N ). The non-tangential boundary value of f at ζ E N,whichexistsfords-almost all ζ E N, is denoted by f(ζ). Set ν = 2πi f(ζ)dζ E N,sothat f(z) = z ζ dν(ζ), z / E N. Fix a generation n, 0 n. Then, for some index k, k 4 n, γ(e N )= 4 n j= ν(q n j ) 4 n ν(q n k), or, equivalently, µ(q n k ) ν(qn k ). To define the function b n k associated with Qn k, we need to describe a simple preliminary construction.,.
8 26 JOAN ATEU, XAVIER TOLSA, AND JOAN VERDERA Take a compactly supported C function ϕ on C, 0 ϕ, ϕds, Q 0 such that ϕ vanishes on 4 j= D(z j, /4), where the z j are the vertices of Q 0.Then C(ϕds Q0 ) A, as one checks easily. Set ( z v ) ϕ j (z) =ϕ j χ σ Q j, where vj is the left lower vertex of Q j. Hence C(ϕ j dµ) A and ϕ j dµ = length( Q j ) ϕ j ds, µ(q j ) 4 µ(q j ). Define b = b n k = ν(q j ) ϕ j ϕ j dµ. Q j Qn k For j k we construct b n j by simply translating bn k. We have Qn j = wn j + Qn k,for some complex number wj n.set b n j (z) =bn k (z wn j ), z C. Now we will prove that b n k satisfies condition (iii). Clearly, bdµ = ν(qn k ) µ(q n k). To show that b is bounded, it suffices to prove (4) ν(q j ) Aµ(Q j ), j 4, and for this we first remark that C(χ Q j ν)(z) A, z/ E N.Thisisprovedin[G2, Lemma 2.3 (a), p. 90]. Since C(χ Q j ν) is analytic outside Q j E N, we conclude that ν(q j ) Aγ(Q j E N ). Now notice that the set Q j E N can be obtained from E(λ +,...,λ N )bya dilation of factor σ and a translation. Hence, recalling (), γ(q j E N )=σ γ(e(λ +,...,λ N )) C 4 γ(e N )=C µ(q j ), which gives (4). It is worth noting at this point that the above inequality explains why cannot be taken to be N. Thanks to the discussion in Section 2 on Cauchy integrals and the Plemelj formulae, it becomes clear that we are only left with the task of proving C(bdµ)(z) A, z / E Q n k. Since C(χ Q n k ν)(z) A, z/ E N Q n k, we only need to estimate, for z/ E Q n k, the difference (5) C(bdµ)(z) C(χ Q n k ν)(z) = C(α j )(z), where Q j Qn k α j = ν(q j ) ϕ j dµ ϕ j dµ χ Q j ν.
9 ANALYTIC CAPACITY OF CANTOR SETS 27 We have dα j =0and C(α j )(z) A, z/ Q j, j 4, again using [G2, Lemma 2.3 (a), p. 90]. Thus, if z j is the center of Q j, (6) C(α j σ 2 )(z) A dist(z,q, z z j )2 j >σ. By the maximum principle, in estimating (5), we can assume that z zj for some j with Q j Q n k. Hence (5) is not greater than σ (7) A + A l j σ 2 dist(z,q l ) 2. For 0 n let Q n be the square in the n-th generation that contains Q j can estimate (7) by.we A + A n=0 Q l Q n \Q σ2 n+ dist(z,q l ) 2 A + A σ n n=0 σ 2 σn 2 4 n A + A ( 4 ) n A, 9 because σ = σ n λ n+ λ,0 n. 3 n This completes the construction of the function b n k associated with the square Q n k as required by hypothesis (iii) in the local T (b)-theorem. Now, by translation invariance it is clear that b n j for j k also satisfies (iii). This shows that the local T (b)-theorem can be applied to µ and thus completes the proof of Theorem 2. n=0 Remark 2. For simplicity, we assumed above that λ n /3 for all n. However, both Theorem and Theorem 2 hold for 0 <λ n < /2. Let us sketch the changes needed in the proof. First it should be noticed that the estimate (4) for γ + (E N )holdsfor0<λ n < /2. Indeed, the arguments for the left inequality in (4) in [a] are valid in this case. On the other hand, the right inequality in (4) is also true for 0 <λ n < /2. For example, arguing as in [T2], one can easily check that ( γ + (E N ) A + n N, λ n /3 (4 n σ n ) 2 ) /2 ( n N ) /2 (4 n σ n ) 2. The other places where the assumption λ n /3 has been used are (4) and (5). The inequality (4) also holds for 0 <λ n < /2. It follows from Vitushkin s estimates for the integral f(z) dz for piecewise Lyapunov curves Γ [Vi] (in our Γ case Γ = Q j ). To prove (5), one can use the sharper estimate C(α j )(z) Aσ γ(q j E N ) σ µ(q j dist(z,q AC ) j )2 dist(z,q, z z j )2 j >σ, instead of (6) (see [G2, pp. 2 3], for example). We leave the details for the reader.
10 28 JOAN ATEU, XAVIER TOLSA, AND JOAN VERDERA References [CH]. Christ, Lectures on singular integral operators, CBS Regional Conference Series in athematics 77, American athematical Society, Providence, RI, 990. R 92f:4202 [CH2]. Christ, AT (b) theorem with remarks on analytic capacity and the Cauchy Integral, Colloq. ath. 60/6(2) (990), R 92k:42020 [D] G. David, Analytic capacity, Calderón-Zygmund operators, and rectifiability, Publ. at. 43() (999), R 2000e:30044 [DO] A.. Davie, B. Øksendal, Analytic capacity and differentiability properties of finely harmonic functions, Acta. ath. 49 (982), R 84h:300 [E] V. Y. Eiderman, Hausdorff measure and capacity associated with Cauchy potentials, ath. Notes 63 (998), R 99m:2805 [G] J. Garnett, Positive length but zero analytic capacity, Proc.Amer.ath.Soc.24 (970), R 43:2203 [G2] J. Garnett, Analytic capacity and measure, Lectures Notes in athematics 297, Springer-Verlag, Berlin-New York, 972. R 56:2257 [GY] J. Garnett, S. Yoshinobu, Large sets of zero analytic capacity, Proc. Amer. ath. Soc. 29 (200), [I] L. D. Ivanov, Variations of sets and functions, Nauka, oscow, 975 (Russian). R 57:6498 [I2] L. D. Ivanov, On sets of analytic capacity zero, in Linear and Complex Analysis Problem Book 3 (part II), Lectures Notes in athematics 574, Springer-Verlag, Berlin, 994, pp [J] P. Jones, Square functions, Cauchy integrals, analytic capacity, and harmonic measure, in: Harmonic Analysis and Partial Differential Equations, (El Escorial, 987), Lectures Notes in athematics 384, Springer, Berlin, 989, pp R 9b:42032 [a] P. attila, On the analytic capacity and curvature of some Cantor sets with non σ-finite length, Publ. at. 40 (996) R 97d:30052 [u] T. urai, ConstructionofH functions concerning the estimate of analytic capacity, Bull. London ath. Soc. 9 (987), R 88d:30034 [T] X. Tolsa, L 2 -boundedness of the Cauchy integral operator for continuous measures, Duke ath. J. 98(2) (999), R 2000d:300 [T2] X. Tolsa, On the analytic capacity γ +, Indiana Univ. ath. J. (5) (2) (2002), [T3] X. Tolsa, Painlevé s problem and the semiadditivity of analytic capacity, Acta ath. (to appear). [Uy] N. X. Uy, Removable sets of analytic functions satisfying a Lipschitz condition, Ark. at. 7 (979), [V] J. Verdera, A weak type inequality for Cauchy transforms of finite measures, Publ. at. 36 (992), R 94k:30099 [V2] J. Verdera, Removability, capacity and approximation, in: Complex Potential Theory, (ontreal,pq,993),natoadv.sci.int.ser.cath.phys.sci.439, KluwerAcademic Publ., Dordrecht, 994, pp R 96b:30086 [V3] J. Verdera, L 2 boundedness of the Cauchy integral and enger curvature, Contemporary ath. 277, American athematical Society, Providence, RI, 200, pp R 2002f:30052 [Vi] A. G. Vitushkin, Estimate of the Cauchy integral, at. Sb. 7(4) (966), [Vi2] A. G. Vitushkin, Analytic capacity of sets in problems of approximation theory, Russian ath. Surveys 22 (967), Departament de atemàtiques, Universitat Autònoma de Barcelona, 0893 Bellaterra,(Barcelona),Spain Département de athématiques, Université de Paris Sud 9405 Orsay, cedex, France Departament de atemàtiques, Universitat Autònoma de Barcelona, 0893 Bellaterra,(Barcelona),Spain
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