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A NOTE ON BOUNDEDNESS OF THE HARDY-LITTLEWOOD MAXIMAL OPERATOR ON MORREY SPACES 1 2 A. GOGATISHVILI AND R.CH. MUSTAFAYEV 5 Abstract. In this paper we prove that the Hardy-Littlewood maximal oper- 1 ator is bounded on Morrey spaces M1,λ(Rn), 0≤λ<n for radial, decreasing 0 functions on Rn. 2 n a J 1. Introduction 9 Morrey spaces M ≡ M (Rn), were introduced by C. Morrey in [8] in order ] p,λ p,λ A to study regularity questions which appear in the Calculus of Variations, and C defined as follows: for 0 ≤ λ ≤ n and 1 ≤ p < ∞, . math Mp,λ := (cid:26)f ∈ Llpoc(Rn) : kfkMp,λ := x∈Rsnu,pr>0rλ−pnkfkLp(B(x,r)) < ∞(cid:27), where B(x,r) is the open ball centered at x of radius r. [ Note that M (Rn) = L (Rn) and M (Rn) = L (Rn), when 1 ≤ p < ∞. 1 p,0 ∞ p,n p v These spaces describe local regularity more precisely than Lebesgue spaces 4 and appeared to be quite useful in the study of the local behavior of solutions to 8 partial differential equations, a priori estimates and other topics in PDE (cf. [4]). 4 6 Given a locally integrable function f on Rn and 0 ≤ α < n, the fractional 0 maximal function M f of f is defined by . α 2 50 Mαf(x) := sup|Q|α−nn |f(y)|dy, (x ∈ Rn), 1 Q∋x ZQ : where the supremum is taken over all cubes Q containing x. The operator M : v α Xi f → Mαf is called the fractional maximal operator. M := M0 is the classical Hardy-Littlewood maximal operator. r a The study of maximal operators is one of the most important topics in har- monic analysis. These significant non-linear operators, whose behavior are very informativeinparticularindifferentiationtheory, providedtheunderstandingand the inspiration for the development of the general class of singular and potential operators (see, for instance, [9], [7], [3], [10], [5], [6]). 2010 Mathematics Subject Classification. Primary 42B25; Secondary 42B35. Key words and phrases. Morrey spaces, maximal operator. The research of A. Gogatishvili was partly supported by the grants P201-13-14743Sof the GrantAgency ofthe CzechRepublic andRVO:67985840,by Shota RustaveliNationalScience Foundation grants no. 31/48 (Operators in some function spaces and their applications in Fourier Analysis) and no. DI/9/5-100/13 (Function spaces, weighted inequalities for integral operators and problems of summability of Fourier series). The research of both authors was partlysupportedby the jointprojectbetweenAcademy ofSciences ofCzechRepublic andThe Scientific and Technological Research Council of Turkey. 1 2 A. GOGATISHVILIAND R.CH.MUSTAFAYEV The boundedness of the Hardy-Littlewood maximal operator M in Morrey spaces M was proved by F. Chiarenza and M. Frasca in [2]: It was shown that p,λ Mf is a.e. finite if f ∈ M and an estimate p,λ kMfk ≤ ckfk (1.1) Mp,λ Mp,λ holds if 1 < p < ∞ and 0 < λ < n, and a weak type estimate (1.1) replaces for p = 1, that is, the inequality t|{Mf > t}∩B(x,r)| ≤ crn−λkfk (1.2) M1,λ holds with constant c independent of x, r, t and f. Inthispaperweshowthat(1.1)isnottrueforp = 1. According toourexample the right result is (1.2). If restricted to the cone of radial, decreasing functions on Rn, inequality (1.1) holds true for p = 1. The paper is organized as follows. We start with notation and preliminary results in Section 2. In Section 3, we prove that the Hardy-Littlewood maximal operator M is bounded on M , 0 < λ < n, for radial, decreasing functions, and 1,λ we give an example which shows that M is not bounded on M , 0 < λ < n. 1,λ 2. Notations and Preliminaries Now we make some conventions. Throughout the paper, we always denote by c a positive constant, which is independent of main parameters, but it may vary from line to line. By a . b we mean that a ≤ cb with some positive constant c independent of appropriate quantities. If a . b and b . a, we write a ≈ b and say that a and b are equivalent. For a measurable set E, χ denotes the E characteristic function of E. Let Ω be any measurable subset of Rn, n ≥ 1. Let M(Ω) denote the set of all measurable functions on Ω and M (Ω) the class of functions in M(Ω) 0 that are finite a.e., while M↓(0,∞) (M+,↓(0,∞)) is used to denote the subset of those functions which are non-increasing (non-increasing and non-negative) on (0,∞). Denote by Mrad,↓ = Mrad,↓(Rn) the set of all measurable, radial, decreasing functions on Rn, that is, Mrad,↓ := {f ∈ M(Rn) : f(x) = ϕ(|x|), x ∈ Rnwithϕ ∈ M↓(0,∞)}. Recall that Mf ≈ Hf, f ∈ Mrad,↓, where 1 Hf(x) := |f(y)|dy |B(0,|x|) ZB(0,|x|) is n-dimensional Hardy operator. Obviously, Hf ∈ Mrad,↓, when f ∈ Mrad,↓. For p ∈ (0,∞], we define the functional k·k on M(Ω) by p,Ω ( |f(x)|pdx)1/p if p < ∞, kfk := Ω p,Ω esssup |f(x)| if p = ∞. ( R Ω The Lebesgue space L (Ω) is given by p L (Ω) := {f ∈ M(Ω) : kfk < ∞} p p,Ω A NOTE ON BOUNDEDNESS OF THE MAXIMAL FUNCTION ON MORREY SPACES 3 and it is equipped with the quasi-norm k·k . p,Ω The decreasing rearrangement (see, e.g., [1, p. 39]) of a function f ∈ M (Rn) 0 is defined by f∗(t) := inf{λ > 0 : |{x ∈ Rn : |f(x)| > λ}| ≤ t} (0 < t < ∞). 3. Boundedness of M on M for radial, decreasing functions 1,λ Reacall that α−n Mαf(x) ≈ sup|B| n |f(y)|dy B∋x ZB ≈ sup|B(x,r)|α−nn |f(y)|dy, (x ∈ Rn), r>0 ZB(x,r) where the supremum is taken over all balls B containing x. In order to prove our main result we need the following auxiliary lemmas. Lemma 3.1. Assume that 0 < λ < n. Let f ∈ Mrad,↓(Rn) with f(x) = ϕ(|x|). The equivalency x kfk ≈ supxλ−n |ϕ(ρ)|ρn−1dρ M1,λ x>0 Z0 holds with positive constants independent of f. Proof. Recall that kfkM1,λ ≈ sup|B|λ−nn f = kMλfk∞, f ∈ M(Rn). B ZB Switching to polar coordinates, we have that λ−n Mλ(f)(y) & |B(0,|y|)| n |f(z)|dz ZB(0,|y|) |y| ≈ |y|λ−n |ϕ(ρ)|ρn−1dρ. Z0 Consequently, |y| kfk & esssup|y|λ−n |ϕ(ρ)|ρn−1dρ M1,λ y∈Rn Z0 x = supxλ−n |ϕ(ρ)|ρn−1dρ, x>0 Z0 where f(·) = ϕ(|·|). 4 A. GOGATISHVILIAND R.CH.MUSTAFAYEV On the other hand, |B| kfkM1,λ . sup|B|λ−nn f∗(t)dt B Z0 |B| λ−n 1 = sup|B| n |ϕ(tn)|dt B Z0 1 |B|n ≈ sup|B|λ−nn |ϕ(ρ)|ρn−1dρ B Z0 x = supxλ−n |ϕ(ρ)|ρn−1dρ, x>0 Z0 where f(·) = ϕ(|·|). (cid:3) Corollary 3.2. Assume that 0 < λ < n. Let f ∈ Mrad,↓(Rn) with f(x) = ϕ(|x|). The equivalency x x kMfk ≈ supxλ−n ϕ(ρ)ρn−1ln dρ M1,λ ρ x>0 Z0 (cid:18) (cid:19) holds with positive constants independent of f. Proof. Let f ∈ Mrad,↓ with f(x) = ϕ(|x|). Since Mf ≈ Hf and Hf ∈ Mrad,↓, by Lemma 3.1, switching to polar coordinates, using Fubini’s Theorem, we have that x 1 kMfk ≈ supxλ−n |f(y)|dy tn−1dt M1,λ |B(0,t| x>0 Z0 (cid:18) ZB(0,t) (cid:19) x 1 t ≈ supxλ−n ϕ(ρ)ρn−1dρdt t x>0 Z0 Z0 x x = supxλ−n ϕ(ρ)ρn−1ln dρ. ρ x>0 Z0 (cid:18) (cid:19) (cid:3) Lemma 3.3. Assume that 0 < λ < n. Let f ∈ Mrad,↓ with f(x) = ϕ(|x|). The inequality kMfk . kfk , f ∈ Mrad,↓ M1,λ M1,λ holds if and only if the inequality x x x supxλ−n ϕ(ρ)ρn−1ln dρ . supxλ−n ϕ(ρ)ρn−1dρ, ϕ ∈ M+,↓(0,∞) ρ x>0 Z0 (cid:18) (cid:19) x>0 Z0 holds. Proof. Thestatement immediatelyfollowsfromLemma3.1andCorollary3.2. (cid:3) Lemma 3.4. Let 0 < λ < n. Then inequality x x x supxλ−n ϕ(ρ)ρn−1ln dρ . supxλ−n ϕ(ρ)ρn−1dρ (3.1) ρ x>0 Z0 (cid:18) (cid:19) x>0 Z0 holds for all ϕ ∈ M+,↓(0,∞). A NOTE ON BOUNDEDNESS OF THE MAXIMAL FUNCTION ON MORREY SPACES 5 Proof. Indeed: x x supxλ−n ϕ(ρ)ρn−1ln dρ ρ x>0 Z0 (cid:18) (cid:19) x 1 t = supxλ−n ϕ(ρ)ρn−1dρdt t x>0 Z0 Z0 x t = supxλ−n tn−λ−1tλ−n ϕ(ρ)ρn−1dρdt x>0 Z0 Z0 t x ≤ suptλ−n ϕ(ρ)ρn−1dρ· supxλ−n tn−λ−1dt t>0 Z0 (cid:18)x>0 Z0 (cid:19) t ≈ suptλ−n ϕ(ρ)ρn−1dρ. t>0 Z0 (cid:3) Now we are in position to prove our main result. Theorem 3.5. Assume that 0 < λ < n. The inequality kMfk . kfk (3.2) M1,λ M1,λ holds for all f ∈ Mrad,↓ with constant independent of f. Proof. The statement follows by Lemmas 3.3 and 3.4. (cid:3) Remark 3.6. Note that inequality (3.2) holds true when λ = 0, for M (Rn) = 1,0 L (Rn) and M is bounded on L (Rn). ∞ ∞ Remark 3.7. It is obvious that the statement of Theorem 3.5 does not hold when λ = n, for in this case M (Rn) = L (Rn) and the inequality 1,n 1 kMfk . kfk L1(Rn) L1(Rn) is true only for f = 0 a.e., which follows from the fact that Mf(x) ≈ |x|−n for |x| large when f ∈ Lloc(Rn). 1 Example 3.8. We show that M is not bounded on M (Rn), 0 < λ < n. For 1,λ simplicity let n = 1 and λ = 1/2. Consider the function ∞ f(x) = χ[k2,k2+1](x). k=0 X Then kfkM1,1/2(R) = sup|I|−1/2 f ≤ sup |I|−1/2 f + sup |I|−1/2 f, I ZI I:|I|≤1 ZI I:|I|>1 ZI where the supremum is taken over all open intervals I ⊂ R. It is easy to see that sup |I|−1/2 f ≤ sup |I|1/2 ≤ 1. I:|I|≤1 ZI I:|I|≤1 6 A. GOGATISHVILIAND R.CH. MUSTAFAYEV Note that sup |I|−1/2 f = sup sup |I|−1/2 f I:|I|>1 ZI m∈NI:m<|I|≤m+1 ZI ∞ = sup sup |I|−1/2 χ[k2,k2+1](x) dx m∈NI:m<|I|≤m+1 ZI k=0 ! X ∞ = sup sup |I|−1/2 I ∩ [k2,k2 +1] . m∈NI:m<|I|≤m+1 (cid:12) (cid:12) (cid:12) k[=0 (cid:12) (cid:12) (cid:12) Since (cid:12) (cid:12) ∞ (cid:12) ∞ (cid:12) I ∩ [k2,k2 +1] ≤ [0,m+1]∩ [k2,k2 +1] (cid:12) (cid:12) (cid:12) (cid:12) (cid:12) k[=0 (cid:12) (cid:12) k[=0 (cid:12) for any interval(cid:12)I such that m < |(cid:12)I| ≤(cid:12)m+1, we obtain that (cid:12) (cid:12) (cid:12) (cid:12) (cid:12) (cid:12) (cid:12) (cid:12) (cid:12) ∞ sup |I|−1/2 f . supm−1/2 [0,m+1]∩ [k2,k2 +1] I:|I|>1 ZI m∈N (cid:12)(cid:12) k[=0 (cid:12)(cid:12) . supm−1/2m(cid:12)(cid:12) 1/2 = 1. (cid:12)(cid:12) m∈N (cid:12) (cid:12) Consequently, we arrive at kfk . 2. M1,1/2(R) On the other hand, since ∞ 1 1 Mf ≥ χ[k2,k2+1] + x−k2χ[k2+1,k2+k+1] + (k +1)2 +1−xχ[k2+k+1,(k+1)2] , k=0(cid:18) (cid:19) X we have that k2 k−1 (i+1)2 kMfk ≥ supk−1 Mf ≥ supk−1 Mf M1,1/2(R) k∈N Z0 k∈N i=1 Zi2 X k−1 ≥ supk−1 lnj & suplnk = ∞. k∈N k∈N j=1 X References [1] C. Bennett and R. 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MR2463316(2011d:42001) A NOTE ON BOUNDEDNESS OF THE MAXIMAL FUNCTION ON MORREY SPACES 7 [7] M. de Guzma´n, Differentiation of integrals in Rn, Lecture Notes in Mathematics, Vol. 481, Springer-Verlag, Berlin-New York, 1975. With appendices by Antonio C´ordoba, and Robert Fefferman, and two by Roberto Moriy´on. MR0457661(56 #15866) [8] C.B. Morrey,On the solutions of quasi-linear elliptic partial differential equations, Trans. Amer. Math. Soc. 43 (1938), no. 1, 126–166,DOI 10.2307/1989904. MR1501936 [9] E.M.Stein,Singular integrals anddifferentiability properties offunctions,PrincetonMath- ematicalSeries,No.30,PrincetonUniversityPress,Princeton,N.J.,1970. MR0290095(44 #7280) [10] , Harmonic analysis: real-variable methods, orthogonality, and oscillatory inte- grals, Princeton Mathematical Series, vol. 43, Princeton University Press, Princeton, NJ, 1993.With the assistance of Timothy S. Murphy; Monographs in Harmonic Analysis, III. MR1232192(95c:42002) [11] A. Torchinsky, Real-variable methods in harmonic analysis, Pure and Applied Mathemat- ics, vol. 123, Academic Press, Inc., Orlando, FL, 1986. MR869816 (88e:42001) 1 InstituteofMathematics oftheAcademyofSciences oftheCzechRepublic, Z´itna 25, 115 67 Prague 1, Czech Republic. E-mail address: [email protected] 2 Department of Mathematics, Faculty of Science and Arts, Kirikkale Uni- versity, 71450 Yahsihan, Kirikkale, Turkey. E-mail address: [email protected]

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