Journal of Inequalities in Pure and Applied Mathematics HARDY’S INTEGRAL INEQUALITY FOR COMMUTATORS OF HARDY OPERATORS volume 7, issue 5, article 183, 2006. QING-YU ZHENG AND ZUN-WEI FU Department of Mathematics Linyi Normal University Linyi Shandong, 276005 People’s Republic of China EMail: zqy7336@163.com EMail: lyfzw@tom.com Received 26 March, 2006; accepted 09 October, 2006. Communicated by: B. Yang Abstract Contents JJ J II I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 083-06 Quit Abstract The authors establish the Hardy integral inequality for commutators generated by Hardy operators and Lipschitz functions. 2000 Mathematics Subject Classification: 26D15, 42B25. Key words: Hardy’s integral inequality, Commutator, Hardy operator, Lipschitz function. Hardy’s Integral Inequality For Commutators Of Hardy Operators This paper was supported by the National Natural Science Foundation (No.10371080) of People’s Republic of China. Qing-Yu Zheng and Zun-Wei Fu Contents Title Page 1 Introduction and Main Results . . . . . . . . . . . . . . . . . . . . . . . . . . 2 Proof of Theorem 1.3 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . References 3 7 Contents JJ J II I Go Back Close Quit Page 2 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au 1. Introduction and Main Results Let f be a non-negative and integral function on R+ , Hardy operators are defined by Z 1 x (Hf )(x) = f (t) dt, x > 0, x 0 and Z ∞ (Vf )(x) = f (t) dt, x > 0. x The Hardy integral inequality results are well known [9, 10, 11]; in particular Z ∞ p p1 (Hf (x)) dx (1.1) 0 p Qing-Yu Zheng and Zun-Wei Fu p1 ∞ Z p ≤ p−1 (f (x)) dx Hardy’s Integral Inequality For Commutators Of Hardy Operators , 0 Title Page and Contents Z (1.2) 0 ∞ (Vf (x))p dx p1 Z ≤p ∞ (xf (x))p dx p1 . 0 p In (1.1), the constant p−1 is the best possible. In (1.2), the constant p is also the best possible. The inequality (1.1) was first proved by Hardy in an attempt to give a simple proof of Hilbert’s double series theorem [12]. Let f be a non-negative and integral function on R+ , and the fractional Hardy operator be defined by Z x 1 α (H f )(x) = 1−α f (t) dt, x > 0, x 0 JJ J II I Go Back Close Quit Page 3 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au for p1 − 1q = α, 0 < α < 1. There are fractional order Hardy integral inequalities which correspond to (1.1) and (1.2): Z ∞ q α (H f (x)) dx (1.3) 1q p1 ∞ Z p ≤C (f (x)) dx 0 , 0 and Z ∞ q (Vf (x)) dx (1.4) 1q Z ≤C 0 ∞ (x 1−α p f (x)) dx p1 . 0 The Hardy inequality (1.3) can be found in [2], (1.4) in [13]. The Hardy integral inequalities have received considerable attention and a large number of papers have appeared which deal with its alternative proofs, various generalizations, numerous variants and applications. For earlier developments of this kind of inequality and many important applications in analysis, see [11]. Among numerous papers dealing with such inequalities, we choose to refer to the papers [3], [5], [9], [10], [16] – [21] and some of the references cited therein. Definition 1.1. Let 0 ≤ α < 1 and b(x) be a measurable, locally integrable function. Then the commutator of the Hardy operator Ubα is defined by Z x 1 α Hb f (x) = 1−α f (t)(b(x) − b(t))dt, x > 0. x 0 Fu [7] obtained the following results. Hardy’s Integral Inequality For Commutators Of Hardy Operators Qing-Yu Zheng and Zun-Wei Fu Title Page Contents JJ J II I Go Back Close Quit Page 4 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au Theorem 1.1. For b ∈ ∧˙ β (R+ ), 0 < β < 1, Hbα is a bounded operator from Lp (R+ ) to Lq (R+ ), 1 < p < q < ∞, 0 ≤ α < 1, 0 < α+β < 1, p1 − 1q = α+β. Remark 1. In Theorem 1.1, If we let α = 0, Then the result corresponds to Hardy inequality (1.3). Definition 1.2. Let b(x) be a measurable, locally integrable function. Then the commutator of the Hardy operator Vb is defined by Z ∞ Vb f (x) = f (t)(b(x) − b(t))dt, x > 0. x In Definition 1.1, if we let α = 0, then we denote Hbα by Hb . It can be seen that if b ∈ ∧˙ β (Rn ), 0 < β < 1, then Hb has a similar boundedness property to Hβ . A natural question regarding the boundedness property of Vb , can be answered in the affirmative by the following inequality (1.5). Theorem 1.2. If b ∈ ∧˙ β (R+ ), (1.5) 1 p − 1 q = β, 0 < β < 1, p > 1. Then kVb f kq ≤ Ckbk∧˙ β (R+ ) k(·)f (·)kp . Theorem 1.3. If b ∈ ∧˙ β (R+ ), 0 < β < 1, 0 ≤ α < 1, p > 1. Then 1 p − 1 q = α + β, 0 < α + β < 1, Hardy’s Integral Inequality For Commutators Of Hardy Operators Qing-Yu Zheng and Zun-Wei Fu Title Page Contents JJ J II I Go Back Close (1.6) kVb f kq ≤ Ckbk∧˙ β (R+ ) k(·)1−α f (·)kp . If we let α = 0 in Theorem 1.3, then Theorem 1.2 can be obtained without difficulty. Thus we just need to prove Theorem 1.3. Before we prove the main theorem, let us state some lemmas and notations. Quit Page 5 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au The Besov-Lipschitz space ∧˙ β (R+ ) is the space of functions f satisfying kf k∧˙ β (R+ ) = |f (x + h) − f (x)| < ∞. |h|β x,h∈R+ ,h6=0 sup Lemma 1.4 ([8, 15]). For any x, y ∈ R+ , if f ∈ ∧˙ β (R+ ), 0 < β < 1, then |f (x) − f (y)| ≤ |x − y|β kf k∧˙ β (R+ ) , (1.7) Hardy’s Integral Inequality For Commutators Of Hardy Operators and given any interval I in R+ sup |f (x) − fI | ≤ C|I|β kf k∧˙ β (R+ ) , x∈I where 1 fI = |I| Z Qing-Yu Zheng and Zun-Wei Fu Title Page f. Contents I Lemma 1.5 ([7, 14]). Let s > 0, q ≥ p > 1 , then ! p1 q pq Z ∞ Z 2k+1 ∞ X X ∞ (i−k)/s 2 |f (t)|p dt ≤ C |f (t)|p dt , k 2 0 i=−∞ k=i JJ J II I Go Back Close where C= 2p/2s 2p/2s − 1 0 2q /2s 2q0 /2s − 1 qq0 , 1 1 + = 1. q0 q There are two different methods to prove Theorem 1.3. Quit Page 6 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au 2. Proof of Theorem 1.3 First Proof. Z ∞ |Vb f (x)|q dx 0 ∞ Z 2i+1 Z X = ≤ i i=−∞ 2 ∞ Z 2i+1 X ∞ Z X ≤2 Hardy’s Integral Inequality For Commutators Of Hardy Operators q |(b(x) − b(t))f (t)| dt dx 2i+1 i=−∞ |(b(x) − b(t))f (t)| dt ∞ Z X 2i ∞ X k=i Z 2i+1 2i !q 2k+1 Qing-Yu Zheng and Zun-Wei Fu dx 2k k=i i=−∞ 0 ∞ ∞ Z X 2i+1 ∞ Z X + 2q/q q (b(x) − b(t))f (t)dt dx 2i 2i i=−∞ q/q 0 x Z 2i i=−∞ = ∞ 2k+1 !q (b(x) − b(2i ,2i+1 ] )f (t) dt dx 2k ∞ Z X k=i 2k+1 !q (b(t) − b(2i ,2i+1 ] )f (t) dt dx Title Page Contents JJ J II I 2k Go Back := I + J. Close By Lemma 1.4 and the Hölder inequality, q/q 0 I=2 ∞ Z X i=−∞ 2i+1 2i Quit ∞ Z X b(x) − b(2i ,2i+1 ] q dx k=i 2k+1 2k !q Page 7 of 16 |f (t)| dt J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au ∞ X q/q 0 ≤2 !q 2i sup x∈(2i ,2i+1 ] i=−∞ × Z ∞ X q/q 0 ≤ C2 ∞ X b(x) − b(2i ,2i+1 ] ! p1 2k+1 |f (t)|p dt 2k k=i 2i(qβ+1) kbk∧˙ β (R+ ) Z 2k+1 2k ! p1 0 q dt q i=−∞ × Z ∞ X q/q 0 ≤ C2 ∞ X ! p1 2k+1 |f (t)|p dt 2i(qβ+1) kbk∧˙ β (R+ ) 2k+1 2k 2k k=i Z Hardy’s Integral Inequality For Commutators Of Hardy Operators ! 10 q p dt Qing-Yu Zheng and Zun-Wei Fu q Title Page i=−∞ × ∞ X Z k/p0 2 2k k=i Notice that q/q 0 I ≤ C2 1 p − 1 q 2k+1 ! p1 q 2−k(1−α)p |t1−α f (t)|p dt . = α + β, kbk∧˙ β (R+ ) ∞ q X i=−∞ Contents JJ J II I Go Back ∞ X k=i (i−k)( 1q +β) Z 2k+1 2 2k ! p1 q |t1−α f (t)|p dt . Close Quit Page 8 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au By Lemma 1.5 s = q 1+qβ , I ≤ C kbk∧˙ β (R+ ) (2.1) q ∞ Z 1−α |t pq f (t)| dt . p 0 Now estimate J, ∞ Z X q/q 0 J =2 2i i=−∞ 2q/q 0 ≤2 ∞ Z X 2i+1 ∞ Z X 2q/q 0 +2 ∞ Z X 2i+1 k=i ∞ Z X i=−∞ !q (b(t) − b(2i ,2i+1 ] )f (t) dt dx Hardy’s Integral Inequality For Commutators Of Hardy Operators 2k k=i 2i i=−∞ 2k+1 2i+1 2i 2k+1 !q (b(t) − b(2k ,2k+1 ] )f (t) dt dx Qing-Yu Zheng and Zun-Wei Fu 2k ∞ Z X 2k+1 !q (b(2k ,2k+1 ] − b(2i ,2i+1 ] )f (t) dt dx Title Page 2k k=i Contents := J1 + J2 . Notice that 2q/q 0 J1 ≤ 2 1 p − 1 q ∞ Z X i=−∞ 2q/q 0 ≤ C2 = α + β, 2i+1 2i kbk∧˙ β (R+ ) 1 p + 1 p0 ∞ X k=i = 1, by Lemma 1.4, it can be inferred that sup b(t) − b(2k ,2k+1 ] t∈(2k ,2k+1 ] ∞ Z q X i=−∞ JJ J 2i+1 2i !Z |f (t)|dt 2k ∞ X k=i kβ Z 2k+1 dx Close Quit !q |f (t)|dt 2 Go Back !q 2k+1 II I dx Page 9 of 16 2k J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au 0 ≤ C22q/q kbk∧˙ β (R+ ) ∞ q X 2i ∞ X i=−∞ i=−∞ = C2 2k k=i kbk∧˙ β (R+ ) ∞ ∞ X X k(β+ p10 ) i × 2 2 2q/q 0 |f (t)|p dt 2 q 2q/q 0 ≤ C2 k(β+ p10 ) ! p1 q 2k+1 Z kbk∧˙ β (R+ ) ∞ X i=−∞ 2−k(1−α)p |t1−α f (t)|p dt 2k k=i ∞ q X ! p1 q 2k+1 Z Z (i−k)/q ! p1 q 2k+1 1−α |t 2 p f (t)| dt 2k k=i . Hardy’s Integral Inequality For Commutators Of Hardy Operators Qing-Yu Zheng and Zun-Wei Fu In the third inequality, the Hölder inequality is applied. By Lemma 1.5 (s = q), (2.2) J1 ≤ C kbk∧˙ β (R+ ) q Title Page pq ∞ 1−α p |t f (t)| dt . Z 0 To estimate J2 , for i > k, by Lemma 1.4, the following result is obtained. b(2k ,2k+1 ] − b(2i ,2i+1 ] ≤ 1 2i ≤ Z b(y) − b(2k ,2k+1 ] dy 2i 1 1 2i 2k JJ J II I Go Back 2i+1 Z Contents 2k+1 Z 2i+1 |b(y) − b(z)| dydz 2k ≤ kbk∧˙ β (R+ ) Quit Page 10 of 16 2i 1 1 2i 2k Close Z 2k+1 2k Z 2i+1 2i |y − z|β dydz J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au 1 2i ≤ kbk∧˙ β (R+ ) Z 2i+1 1 y β dy + k 2 2i Z ! 2k+1 z β dz 2k ≤ C2iβ+1 kbk∧˙ β (R+ ) . Notice that p1 − 1q = α + β, p1 + p10 = 1; by Lemma 1.4 and the Hölder inequality, we have !q ∞ Z 2i+1 ∞ Z 2k+1 X X 0 q J2 ≤ C22q/q +q kbk∧˙ β (R+ ) 2iβ |f (t)|dt dx 2i i=−∞ 2q/q 0 +q ≤ C2 kbk∧˙ β (R+ ) ∞ q X k=i i(β+ 1q ) 2 ∞ X i=−∞ 2q/q 0 +q = C2 kbk∧˙ β (R+ ) Z ∞ X i=−∞ ! 1 q 2k+1 2 p |f (t)|p dt ! p1 q 2k+1 2−k(1−α)p |t1−α f (t)|p dt (i−k)(β+ 1q ) Z ! 1 q 2k+1 p 1−α |t 2 2k In the second inequality, the Hölder inequality is applied. q By Lemma 1.5 s = qβ+1 , (2.3) J2 ≤ C kbk∧˙ β (R+ ) Z 0 ∞ Contents 2k k=i q Qing-Yu Zheng and Zun-Wei Fu 2k Hardy’s Integral Inequality For Commutators Of Hardy Operators Title Page Z k=i ∞ q X k/p0 k=i q 0 ≤ C22q/q +q kbk∧˙ β (R+ ) ∞ ∞ X 1 X 0 ) i(β+ 2 q 2k/p × i=−∞ 2k pq 1−α p |t f (t)| dt . p f (t)| dt . JJ J II I Go Back Close Quit Page 11 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au Combining (2.1), (2.2) and (2.3), we complete the proof of Theorem 1.3. Second Proof. By inequality (1.7) and comparing the size of x and t, we have ∞ Z |Vb f (x)|q dx = 0 ∞ Z X 2i i=−∞ ≤ 2i+1 ∞ Z X x q f (t)|b(x) − b(x)|dt dx ∞ Z X 2i+1 2i i=−∞ ∞ Z k=i ≤ C kbk∧˙ β (R+ ) |t − x|β kbk∧˙ β (R+ ) |f (t)| dt 2k ∞ Z q X q ∞ X Z = C kbk∧˙ β (R+ ) i=−∞ By the Hölder inequality, Z 2k+1 2k t1−α |f (t)| dt ≤ t1−α−β 1 p 1 p0 + Z 2 tβ |f (t)| dt dx 2k 2k k=i k=i !q 2k+1 2k+1 2k Hardy’s Integral Inequality For Commutators Of Hardy Operators Qing-Yu Zheng and Zun-Wei Fu ∞ Z 2k+1 X ∞ Z X dx 1−α t |f (t)| t1−α−β !q dt dx !q t1−α |f (t)| dt t1−α−β Title Page Contents . JJ J = 1, the following estimate is obtained. 2k+1 2k i ∞ Z X k=i 2i+1 2i i=−∞ ∞ q X 2i+1 2i i=−∞ = C kbk∧˙ β (R+ ) !q 2k+1 II I Go Back ! p1 |t1−α f (t)|p dt Z 2k+1 2k ! 10 p 0 t(α+β−1)p dt Close . Quit Page 12 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au Notice that Z 1 p − 1 q = α + β, ∞ |Vb f (x)|q dx 0 ≤ C kbk∧˙ β (R+ ) q ∞ X i=−∞ ∞ X 2(i−k)/q k=i By Lemma 1.5, the desired result is obtained. Z 2k+1 2k ! p1 q 1−α p |t f (t)| dt . Hardy’s Integral Inequality For Commutators Of Hardy Operators Qing-Yu Zheng and Zun-Wei Fu Title Page Contents JJ J II I Go Back Close Quit Page 13 of 16 J. Ineq. Pure and Appl. Math. 7(5) Art. 183, 2006 http://jipam.vu.edu.au References [1] C. BENNET, R.A. DEVORE AND R. SHARPLEY, Weak L∞ and BMO, Ann. of Math., 113 (1981), 601–611. [2] G.A. BLISS, An integral inequality, J. London Math. Soc., 5(1930), 4046. [3] T.A.A. BROADBENT, A proof of Hardy’s convergence theorem, J. London Math. Soc., 3 (1928), 242–243 1 [4] A.P. CALDERÓN, Space between L and L cikiewiez, Studia Math., 26 (1966), 273–299. ∞ and the theorem of Mar- [5] E. COPSON, Some integral inequality, Proc. Roy. Soc. Edinburgh Sect. A. 75 (1975-76), 157–164. [6] R.A. DEVORE AND R.C. 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