Volume 9 (2008), Issue 2, Article 49, 9 pp. A REVERSE HARDY-HILBERT-TYPE INTEGRAL INEQUALITY GAOWEN XI D EPARTMENT OF M ATHEMATICS L UOYANG T EACHERS ’ C OLLEGE L UOYANG 471022, P. R. C HINA xigaowen@163.com Received 07 December, 2007; accepted 25 May, 2008 Communicated by B. Opić A BSTRACT. By estimating a weight function, a reverse Hardy-Hilbert-type integral inequality with a best constant factor is obtained. As an application, some equivalent forms and some particular results have been established. Key words and phrases: Hardy-Hilbert-type integral inequality; weight function; β function; Hölder’s inequality. 2000 Mathematics Subject Classification. 26D15. 1. I NTRODUCTION R∞ R∞ Let p > 1, p1 + 1q = 1, f (x) ≥ 0, g(x) ≥ 0, and 0 < 0 f p (x)dx < ∞, 0 < 0 g q (x)dx < ∞. Then the Hardy-Hilbert’s integral inequality is as follows: Z ∞ p1 Z ∞ 1q Z ∞Z ∞ π f (x)g(y) p q (1.1) dxdy < g (x)dx , f (x)dx x+y sin( πp ) 0 0 0 0 where the constant factor sin(π π ) is the best possible (see [1]). For (1.1), Yang et al. [2], [3], [4], p [8] and [9] gave some strengthened versions and extensions. In particular, in [7], Yang obtained Z ∞Z ∞ f (x)g(y) p+λ−2 q+λ−2 (1.2) dxdy < B , (x + y − 2α)λ p q α α Z ∞ p1 Z ∞ 1q 1−λ p 1−λ q (x − α) g (x)dx , × (x − α) f (x)dx α α where α ∈ R, λ > 2 − min{p, q}, The author wishes to thank the referee for several helpful comments. This research is supported by the Natural Science Foundation of Henan Province (Grant No. 2008B110011). 360-07 2 G AOWEN X I Recently, in [5], Xi gave a reverse Hardy-Hilbert-type inequality (1.3) ∞ X ∞ X am b n (m + n + 1)λ n=0 m=0 ) 1q (∞ ) p1 (X ∞ 2−λ X (n + 1)2−λ (λ − 1)2 (n + 1) 2 , bqn > 1− apn 2 2n + 3 − λ λ − 1 n=0 2n + 3 − λ 4(n + 1) n=0 P (n+1)2−λ apn where 0 < p < 1, p1 + 1q = 1, 1.5 ≤ λ < 3 and an ≥ 0, bn > 0, such that 0 < ∞ n=0 2n+3−λ < P (n+1)2−λ bqn ∞, 0 < ∞ n=0 2n+3−λ < ∞. In this paper, by estimating the weight function, a reverse Hardy-Hilbert-type integral inequality with a best constant factor is obtained. As an application, some equivalent forms and some particular results have been established. 2. S OME L EMMAS Lemma 2.1. Z ∞ B(p, q) = B(q, p) = (2.1) 0 1 up−1 du (1 + u)p+q (p, q > 0), where B(p, q) is the β function . Proof. See [6]. Lemma 2.2. Let p < 0 or 0 < p < 1, and p1 + 1q = 1, f (x), g(x) ≥ 0, f ∈ Lp (E), g ∈ Lq (E), x ∈ Rk and the set E is Borel measurable in Rk , where k is a positive integer. Then Z Z f (x)g(x)dx ≥ (2.2) p1 Z p f (x)dx E E 1q q g (x)dx , E where the equality holds if and only if there exist non-negative real numbers a and b, such that they are not all zero and af p (x) = bg q (x), a. e. in E. Proof. See [1, Section 6.9, Theorem 189]. Lemma 2.3. Let p < 0 or 0 < p < 1, and p1 + 1q = 1, 2 − max{p, q} < λ < 2 − min{p, q}, y > α, The weight function ωλ (y, p) is defined by Z (2.3) ∞ ωλ (y, p) = α Then we have (2.4) p+λ−2 p > 0, 1 (x + y − 2α)λ q+λ−2 q y−α x−α 2−λ p dx, y ∈ (0, ∞). > 0, and 1−λ ωλ (y, p) = (y − α) B p+λ−2 q+λ−2 , p q Proof. If p < 0, then 0 < q < 1. Since 1 < λ < 2 − p, p+λ−2 > 0 and p q+λ−2 p+λ−2 we have q < 0, 1 < λ < 2 − q, p > 0, q > 0. J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. . q+λ−2 q > 0. If 0 < p < 1, http://jipam.vu.edu.au/ R EVERSE H ARDY-H ILBERT-T YPE I NTEGRAL I NEQUALITY Setting t = Z ∞ α x−α , y−α by p+λ−2 p 1 (x + y − 2α)λ + q+λ−2 q y−α x−α 3 = λ, we have 2−λ p Z ∞ 2−λ 1 t− p dt λ (1 + t) Z0 ∞ p+λ−2 1 = (y − α)1−λ t p −1 dt λ (1 + t) 0 p+λ−2 q+λ−2 1−λ = (y − α) B , . p q 1−λ dx = (y − α) The lemma is thus proved. Lemma 2.4. Let p < 0, Z (2.5) 1 p ∞ + 1 q Z ∞ = 1, 2 − q < λ < 2 − p, 0 < ε < q+λ−2 , 2 then we have λ−2−ε λ−2−ε 1 (x − α) p (y − α) q dxdy λ α+1 α+1 (x + y − 2α) 1 q+λ−2 ε p+λ−2 ε = B − , + − Oε (1). ε q q p q I= Proof. Setting x − α = s, y − α = t, then Z ∞ Z ∞ λ−2−ε λ−2−ε 1 p q (x − α) (y − α) dxdy λ α+1 α+1 (x + y − 2α) Z ∞Z ∞ λ−2−ε λ−2−ε 1 = s p t q dsdt λ (s + t) Z ∞ Z1 ∞ 1 λ−2−ε λ−2−ε 1 p q = s t dt ds. (s + t)λ 1 1 I= Let u = st , we have # q+λ−2−ε 1 I= s−1−ε u q −1 du ds λ 1 (1 + u) 1 s Z ∞ Z ∞ q+λ−2−ε 1 −1 −1−ε du ds = s u q (1 + u)λ 1 0 # "Z 1 Z ∞ s q+λ−2−ε 1 u q −1 du ds − s−1−ε λ 0 (1 + u) 1 1 q+λ−2 ε p+λ−2 ε = B − , + ε q q p q # "Z 1 Z ∞ s q+λ−2−ε 1 u q −1 du ds. − s−1−ε λ (1 + u) 0 1 Z ∞ "Z ∞ J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/ 4 G AOWEN X I By 1 < 2 − q < λ, 0 < ε < q+λ−2 . Hence 2 "Z 1 Z ∞ s 0< s−1−ε 1 0 ∞ Z < s −1−ε "Z ∞ < s −1 u "Z = q+λ−2−ε −1 q du ds # du ds 1 s u q+λ−2 −1 q # du ds 0 1 1 s # 0 1 Z 1 u (1 + u)λ q+λ−2−ε −1 q q q+λ−2 2 . The lemma is proved. 3. M AIN R ESULTS Let p < 0 or 0 < p < 1, p1 + 1q = 1, 2 − max{p, q} < λ < 2 − min{p, q}, R∞ R∞ f (x), g(x) ≥ 0, and 0 < α (x − α)1−λ f p (x)dx < ∞, 0 < α (x − α)1−λ g q (x)dx < ∞, α ∈ R. Then Z ∞Z ∞ f (x)g(y) p+λ−2 q+λ−2 (3.1) dxdy > B , (x + y − 2α)λ p q α α 1q Z ∞ p1 Z ∞ 1−λ p 1−λ q × (x − α) f (x)dx (x − α) g (x)dx , Theorem 3.1. α where the constant factor B p+λ−2 q+λ−2 , q p α is the best possible. Proof. By (2.2), we have 2−λ # Z ∞Z ∞ Z ∞Z ∞" f (x)g(y) f (x) x − α pq (3.2) dxdy = λ (x + y − 2α)λ α α α α (x + y − 2α) p y − α " 2−λ # x − α pq g(y) dxdy × λ (x + y − 2α) q y − α 2−λ # p1 Z ∞Z ∞" f p (x) x−α q ≥ dx (x + y − 2α)λ y − α α α # 1q 2−λ Z ∞Z ∞" q p g (y) y−α × dy . λ (x + y − 2α) x−α α α If (3.2) takes the form of equality, then by (2.2), there exist non-negative numbers a and b such that they are not all zero and 2−λ 2−λ f p (x) x−α q g q (y) y−α p =b , a.e. in (α, ∞) × (α, ∞). a (x + y − 2α)λ y − α (x + y − 2α)λ x − α It follows that a(x − α)2−λ f p (x) = b(y − α)2−λ g q (y) = c, J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/ R EVERSE H ARDY-H ILBERT-T YPE I NTEGRAL I NEQUALITY 5 a. e. in (0, ∞) × (0, ∞). Without loss of generality, suppose a 6= 0. One has c (x − α)1−λ f p (x) = (x − α)−1 , a R∞ a. e. in (0, ∞) × (0, ∞), which contradicts 0 < α (x − α)1−λ f P (x)dx < ∞. Therefore, by (2.3), we have Z ∞ Z α ∞ α f (x)g(y) dxdy > (x + y − 2α)λ Z ∞ 1−λ p ωλ (x, q)(x − α) p1 f (x)dx α Z ∞ 1−λ q × ωλ (y, p)(y − α) g (y)dy 1q . α By (2.4), we obtain (3.1). Without loss of generality, suppose p < 0, which implies that 0 < q < 1. For 0 < ε < set λ−2−ε fε (x) = 0, x ∈ (α, α + 1); fε (x) = (x − α) p , x ∈ [α + 1, ∞), q+λ−2 2 λ−2−ε gε (x) = 0, x ∈ (α, α + 1); gε (x) = (x − α) q , x ∈ [α + 1, ∞). If the constant factor B p+λ−2 , q+λ−2 in (3.1) is not the best possible, then, there exists a q p q+λ−2 p+λ−2 q+λ−2 positive constant K > B p+λ−2 , , such that (3.1) is still valid if B , is p q p q replaced by K. By (2.5), we have q+λ−2 ε p+λ−2 ε B − , + − εOε (1) q q p q Z ∞Z ∞ fε (x)gε (y) =ε dxdy (x + y − 2α)λ α α 1q Z ∞ p1 Z ∞ 1−λ q 1−λ p > εK (x − α) fε (x)dx (y − α) gε (y)dy = K. α+1 α+1 Letting ε −→ 0+ , we obtain B p+λ−2 , q+λ−2 ≥ K. Hence the constant factor p q B p+λ−2 , q+λ−2 in (3.1) is the best possible when 2 − q < λ < 2 − p, 0 < ε < q+λ−2 . p q 2 The theorem is proved. In (3.1), when α = − 12 , we have: Corollary 3.2. Let p < 0, or 0 < p < 1, p1 + 1q = 1, 2 − max{p, q} < λ < 2 − min{p, q}, 1−λ p 1−λ q R∞ R∞ f (x), g(x) ≥ 0, 0 < − 1 x + 12 f (x)dx < ∞, 0 < − 1 x + 12 g (x)dx < ∞. Then 2 ∞Z ∞ 2 p+λ−2 q+λ−2 (3.3) , p q − 12 − 12 # p1 "Z # 1q 1−λ 1−λ ∞ ∞ 1 1 × x+ f p (x)dx x+ g q (x)dx , 1 1 2 2 −2 −2 where the constant factor B p+λ−2 , q+λ−2 is the best possible. p q Z f (x)g(y) dxdy > B (x + y + 1)λ "Z In (3.1), when λ = 2, we have: J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/ 6 G AOWEN X I R∞ Corollary 3.3. Let p < 0, or 0 < p < 1, p1 + 1q = 1, f (x), g(x) ≥ 0, 0 < α (x − α)−1 f p (x)dx R∞ < ∞, 0 < α (x − α)−1 g q (x)dx < ∞, α ∈ R. Then Z ∞ p p1 Z ∞ q 1q Z ∞Z ∞ f (x) f (x)g(y) g (x) dx . (3.4) dxdy > dx (x + y − 2α)2 x−α x−α α α α α In (3.1), when α = − 12 , λ = 2, we have: R∞ Corollary 3.4. Let p < 0, or 0 < p < 1, p1 + 1q = 1, f (x), g(x) ≥ 0, 0 < − 1 (x + 12 )−1 f p (x)dx 2 −1 q R∞ < ∞, 0 < − 1 x + 12 g (x)dx < ∞. Then 2 "Z # p1 "Z # 1q Z ∞Z ∞ ∞ q ∞ p f (x)g(y) f (x) g (x) . (3.5) dxdy > 1 dx 1 dx 2 − 12 − 12 (x + y + 1) − 12 x + 2 − 21 x + 2 4. A N E QUIVALENT F ORM R∞ Theorem 4.1. Let p < 0, p1 + 1q = 1, 2−q < λ < 2−p, f (x) ≥ 0, and 0 < α (x − α)1−λ f p (x)dx < ∞, α ∈ R. Then Z ∞ p Z ∞ f (x) (p−1)(λ−1) dx dy (4.1) (y − α) (x + y − 2α)λ α α p Z ∞ p+λ−2 q+λ−2 < B , (x − α)1−λ f p (x)dx. p q α where the constant factor B p+λ−2 , q+λ−2 is the best possible. Inequalities (4.1) and (3.1) p q are equivalent as p < 0. Proof. Let (p−1)(λ−1) Z ∞ g(y) = (y − α) α f (x) dx (x + y − 2α)λ p−1 , y ∈ (α, ∞). Then by (3.1) and p < 0, we have Z ∞ (4.2) 0< (y − α)1−λ g q (y)dy Z ∞ p Zα∞ f (x) (p−1)(λ−1) = (y − α) dx dy (x + y − 2α)λ α α Z ∞Z ∞ f (x)g(y) dxdy = (x + y − 2α)λ α α Z ∞ p1 p+λ−2 q+λ−2 1−λ p ≥B , (x − α) f (x)dx p q α Z ∞ 1q 1−λ q × (y − α) g (y)dy . α Since p < 0, we obtain that Z ∞ (4.3) (y − α)1−λ g q (y)dy α p Z ∞ p+λ−2 q+λ−2 ≤ B , (x − α)1−λ f p (x)dx < ∞. p q α J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/ R EVERSE H ARDY-H ILBERT-T YPE I NTEGRAL I NEQUALITY 7 By (4.3) and (4.2), we obtain (4.1). Whereas, assume that (4.1) is true, by (2.2), we have Z ∞Z ∞ f (x)g(y) dxdy (x + y − 2α)λ α α h Z ∞ Z ∞ i 1−λ λ−1 f (x) q g(y) dy dx (y − α) = (y − α) q (x + y − 2α)λ α α 1q Z ∞ Z ∞ p p1 Z ∞ f (x) (p−1)(λ−1) 1−λ q (y − α) g (y)dy . ≥ (y − α) dx dy (x + y − 2α)λ α α α Since p < 0, by (4.1), then (3.1) is proved. Hence inequalities (4.1) and (3.1) are equivalent as p < 0. 1−λ p R∞ Corollary 4.2. Let p < 0, p1 + 1q = 1, 2−q < λ < 2−p, f (x) ≥ 0, 0 < − 1 x + 12 f (x)dx 2 < ∞. Then Z ∞ (4.4) − 12 1 y+ 2 #p f (x) dx dy λ − 12 (x + y + 1) 1−λ p Z ∞ p+λ−2 q+λ−2 1 x+ f p (x)dx, < B , 1 2 p q −2 (p−1)(λ−1) "Z where the constant factor B ∞ p+λ−2 q+λ−2 , q p is the best possible. R∞ Corollary 4.3. Let p < 0, p1 + 1q = 1, f (x) ≥ 0, 0 < α (x − α)−1 f p (x)dx < ∞, α ∈ R. Then Z ∞ p Z ∞ Z ∞ p f (x) f (x) (p−1) (4.5) (y − α) dx dy < dx. 2 (x + y − 2α) x−α α α α Corollary 4.4. Let p < 0, Z ∞ (4.6) − 21 1 p 1 y+ 2 + 1 q = 1, f (x) ≥ 0, 0 < (p−1) "Z ∞ − 12 R∞ − 12 f (x) dx (x + y + 1)2 x+ 1 −1 2 #p Z f p (x)dx < ∞. Then ∞ dy < − 12 f p (x) dx. x + 12 Theorem 4.5. Let 0 < p < 1, p1 + 1q = 1, 2 − p < λ < 2 − q, f (x) ≥ 0, and 0 < R∞ (x − α)1−λ f p (x)dx < ∞, α ∈ R. Then α p f (x) (4.7) (y − α) dx dy (x + y − 2α)λ α α p Z ∞ p+λ−2 q+λ−2 > B , (x − α)1−λ f p (x)dx, p q α q+λ−2 , is the best possible. Inequalities (4.7) and (3.1) where the constant factor B p+λ−2 p q are equivalent as 0 < p < 1. Z ∞ (p−1)(λ−1) Z ∞ J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/ 8 G AOWEN X I Proof. Since 0 < p < 1, by (2.2) and (2.4),we have 2−λ # p (Z ∞ " Z ∞ f (x) x − α pq f (x) (4.8) dx = λ (x + y − 2α)λ α α (x + y − 2α) p y − α " 2−λ # )p 1 y − α pq dx × λ (x + y − 2α) q x − α 2−λ Z ∞ f p (x) x−α q ≥ dx (x + y − 2α)λ y − α α "Z 2−λ #p−1 ∞ y−α p 1 dx × (x + y − 2α)λ x − α α p−1 p+λ−2 q+λ−2 , (y − α)(p−1)(1−λ) = B p q 2−λ Z ∞ f p (x) x−α q × dx. (x + y − 2α)λ y − α α If (4.8) takes the form of equality, then by (2.2), there exist non-negative numbers a and b, such that they are not all zero and f p (x) a (x + y − 2α)λ x−α y−α 2−λ q 1 =b λ (x + y − 2α) p y−α x−α 2−λ p , a.e. (α, ∞). It follows that a(x − α)2−λ f p (x) = b(y − α)2−λ , a.e. in (α, ∞). Obviously a 6= 0, (otherwise a = b = 0), one has b (x − α)1−λ f p (x) = (y − α)2−λ x−1 , a.e. (α, ∞) a R∞ which contradicts 0 < α (x − α)1−λ f P (x)dx < ∞. Hence Z ∞ p Z ∞ f (x) (p−1)(λ−1) (y − α) dx dy (x + y − 2α)λ α α p−1 Z ∞ "Z ∞ 2−λ # p+λ−2 q+λ−2 f p (x) x−α q , dx dy > B p q (x + y − 2α)λ y − α α α p−1 p+λ−2 q+λ−2 = B , p q 2−λ # Z ∞ "Z ∞ 1 x−α q × dy f p (x)dx. λ (x + y − 2α) y − α α α By (2.3) and (2.4), we obtain (4.7). Obviously, inequalities (4.7) and (3.1) are equivalent as 0 < p < 1 and the constant factor p+λ−2 q+λ−2 B , q is the best possible. p J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/ R EVERSE H ARDY-H ILBERT-T YPE I NTEGRAL I NEQUALITY 9 1−λ p R∞ Corollary 4.6. Let 0 < p < 1, p1 + 1q = 1, 2−p < λ < 2−q, 0 < − 1 x + 12 f (x)dx < ∞, 2 f (x) ≥ 0. Then #p (p−1)(λ−1) "Z ∞ Z ∞ f (x) 1 dx dy y+ λ 2 − 12 (x + y + 1) − 12 1−λ p Z ∞ p+λ−2 q+λ−2 1 f p (x)dx, > B , x+ 1 2 p q −2 where the constant factor B p+λ−2 , q+λ−2 is the best possible. p q R∞ Corollary 4.7. Let 0 < p < 1, p1 + 1q = 1, f (x) ≥ 0, 0 < α (x − α)−1 f p (x)dx < ∞, α ∈ R. Then Z ∞ p Z ∞ p Z ∞ f (x) f (x) (p−1) dx dy > dx. (4.9) (y − α) 2 (x + y − 2α) x−α α α α −1 p R∞ Corollary 4.8. Let 0 < p < 1, p1 + 1q = 1, f (x) ≥ 0, 0 < − 1 x + 12 f (x)dx < ∞. Then 2 " # p (p−1) Z ∞ Z ∞ Z ∞ p f (x) f (x) 1 dx dy > (4.10) y+ 1 dx. 2 2 − 12 − 12 x + 2 − 12 (x + y + 1) R EFERENCES [1] G.H. HARDY, J.E. LITTLEWOOD Cambridge, 1952. AND G. POLYA, Inequalities, Cambridge University Press, [2] M. KRNIĆ AND J. PEČARIĆ, General Hilbert’s and Hardy’s inequalities, Math. Inequal. Appl., 8(1) (2005), 29-51. [3] A. SHAMANDY, On new extensions of integral inequalities similar to Hilbert’s inequality(I), Proc. Pakistan Acad. Sci., 42(2) (2005), 89–98. [4] A. SHAMANDY, On new extensions of integral inequalities similar to Hilbert’s inequality(II), Proc. Pakistan Acad. Sci., 42(2) (2005), 99–109. [5] G. XI, A reverse Hardy-Hilbert-type inequality, J. Inequal. Appl., 2007 (2007), Art. 79758. [6] B. YANG AND L. DEBNATH, On a new generalization of Hardy-Hilbert’s inequality and its applications, J. Math. Anal. Appl., 233 (1999), 484–497. [7] B. Yang, On Hardy-Hilbert’s integral inequality, J. Math. Anal. Appl., 261 (2001), 295–306. [8] B. YANG, On best extensions of Hardy-Hilbert’s inequality with two parameters, J. Inequal. Pure Appl. Math., 6(3) (2005), Art. 81. [ONLINE: http://jipam.vu.edu.au/article.php? sid=554]. [9] B. YANG, A new Hilbert-type inequality, Bull. Belg. Math. Soc., 13 (2006), 479–487. J. Inequal. Pure and Appl. Math., 9(2) (2008), Art. 49, 9 pp. http://jipam.vu.edu.au/