Journal of Inequalities in Pure and Applied Mathematics ON BEST EXTENSIONS OF HARDY-HILBERT’S INEQUALITY WITH TWO PARAMETERS volume 6, issue 3, article 81, 2005. BICHENG YANG Department of Mathematics Guangdong Institute of Education Guangzhou, Guangdong 510303 People’s Republic of China Received 23 February, 2005; accepted 17 June, 2005. Communicated by: W.S. Cheung EMail: bcyang@pub.guangzhou.gd.cn Abstract Contents JJ J II I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 055-05 Quit Abstract This paper deals with some extensions of Hardy-Hilbert’s inequality with the best constant factors by introducing two parameters λ and α and using the Beta function. The equivalent form and some reversions are considered. 2000 Mathematics Subject Classification: 26D15. Key words: Hardy-Hilbert’s inequality; Beta function; Hölder’s inequality. Contents 1 Introduction . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3 2 Some Lemmas . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 3 Main Results . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 12 4 Some Best Extensions of (1.3) . . . . . . . . . . . . . . . . . . . . . . . . . . 26 References On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 2 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au 1. Introduction If an, bn ≥ 0 satisfy 0< ∞ X a2n < ∞ and 0< n=1 ∞ X b2n < ∞, n=1 then one has two equivalent inequalities as: (∞ ) 12 ∞ ∞ ∞ X X X X am b n (1.1) <π a2n b2n m + n n=1 m=1 n=1 n=1 and ∞ X (1.2) n=1 ∞ X am m+n m=1 !2 < π2 ∞ X Bicheng Yang a2n , n=1 2 where the constant factors π and π are the best possible. Inequality (1.1) is well known as Hilbert’s inequality (cf. Hardy et al. [1]). In 1925, Hardy [2] gave some extensions of (1.1) and (1.2) by introducing the (p, q)−parameter as: If p > 1, p1 + 1q = 1, an, bn ≥ 0 satisfy 0< ∞ X n=1 apn < ∞ and 0< ∞ X On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters bqn < ∞, n=1 then one has the following two equivalent inequalities: (∞ ) p1 ( ∞ ) 1q ∞ X ∞ X X X π am b n < (1.3) apn bqn π m + n sin p n=1 n=1 n=1 m=1 Title Page Contents JJ J II I Go Back Close Quit Page 3 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and ∞ X (1.4) n=1 ∞ X am m+n m=1 p !p < sin ∞ π X p an , π p n=1 h ip π π where the constant factors sin(π/p) and sin(π/p) are the best possible. Inequality (1.3) is called Hardy-Hilbert’s inequality, and is important in analysis and its applications (cf. Mitrinović et al. [3]). In 1997-1998, by estimating the weight coefficient and introducing the Euler constant γ, Yang and Gao [4, 5] gave a strengthened version of (1.3) as: ∞ X ∞ X am bn (1.5) m+n n=1 m=1 p1 1q ∞ ∞ X X π − 1 −1 γ apn π − 1 −1 γ bqn < , π π np nq n=1 sin p n=1 sin p where 1 − γ = 0.42278433+ is the best value. In 1998, Yang [6] first introduced an independent parameter λ and the Beta function to build an extension of Hilbert’s integral inequality. Recently, by introducing a parameter λ, Yang [7] and Yang et al. [8] gave some extensions of (1.3) and (1.4) as: If 2 − min{p, q} < λ ≤ 2, an, bn ≥ 0 satisfy 0< ∞ X n=1 n1−λ apn < ∞ and 0< ∞ X n=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 4 of 35 n1−λ bqn < ∞, J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au then one has the following two equivalent inequalities: (∞ ) p1 ( ∞ ) 1q ∞ X ∞ X X X am b n < kλ (p) (1.6) n1−λ apn n1−λ bqn λ (m + n) n=1 n=1 n=1 m=1 and #p ∞ X a m p (1.7) n(p−1)(λ−1) dy < [k (p)] n1−λ apn , λ λ (m + n) n=1 m=1 n=1 where the constant factors kλ (p) = B p+λ−2 and [kλ (p)]p are the best , q+λ−2 p q possible (B(u, v) is the β function). For λ = 1, inequalities (1.6) and (1.7) reduce respectively to (1.3) and (1.4). By introducing a parameter α, Kuang [9] gave an extension of (1.3), and Yang [10] gave an improvement of [9] as: If 0 < α ≤ min{p, q}, an, bn ≥ 0 satisfy " ∞ X 0< ∞ X ∞ X n(p−1)(1−α) apn < ∞ and n=1 0< ∞ X n(q−1)(1−α) bqn < ∞, n=1 am b n mα + nα n=1 m=1 π α sin πp Title Page Contents II I Go Back ∞ X ∞ X < Bicheng Yang JJ J then one has two equivalent inequalities as: (1.8) On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Close Quit (∞ X n=1 n(p−1)(1−α) apn ) p1 ( ∞ X n=1 ) 1q n(q−1)(1−α) bqn Page 5 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and (1.9) ∞ X " nα−1 n=1 ∞ X am mα + nα m=1 #p p ∞ X π dy < n(p−1)(1−α) apn , π α sin p n=1 h ip π π where the constant factors α sin(π/p) and α sin(π/p) are the best possible. For α = 1, inequalities (1.8) and (1.9) reduce respectively to (1.3) and (1.4). Recently, Hong [11] gave an extension of (1.3) by introducing two parameters λ 1 and α as: If α ≥ 1, 1 − αr < λ ≤ 1 (r = p, q), then (1.10) Bicheng Yang ∞ X ∞ X am b n α (m + nα )λ n=1 m=1 < Hλ,α (p) On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters (∞ X n=1 nα(1−λ) apn ) p1 ( ∞ X Title Page ) 1q nα(1−λ) bpn , n=1 where Contents JJ J II I p1 1q 1 1 1 1 ,λ + −1 ,λ + −1 . Hλ,α (p) = B 1 − B 1− αq αq αp αp Go Back For λ = α = 1, (1.10) reduces to (1.3). However, it is obvious that (1.10) is not an extension of (1.6) or (1.8). In 2003, Yang et al. [12] provided an extensive account of the above results. More recently, Yang [13] gave some extensions of (1.1) and (1.2) as: If 0 < Quit Close Page 6 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au λ ≤ min{p, q}, satisfy 0< ∞ X np−1−λ apn < ∞ and 0< n=1 ∞ X nq−1−λ apn < ∞, n=1 then one has the following two equivalent inequalities: (1.11) (∞ ) p1 ( ∞ ) 1q X X am b n < Kλ (p) np−1−λ apn nq−1−λ bpn λ (m + n) n=1 n=1 n=1 m=1 ∞ X ∞ X and (1.12) ∞ X " n(p−1)λ−1 n=1 ∞ X am (m + n)λ m=1 #p dy < [Kλ (p)]p ∞ X Bicheng Yang np−1−λ apn , Title Page n=1 where the constants Kλ (p) = B λp , λq and [Kλ (p)]p are the best possible. For λ = 1, (1.11) and (1.12) reduce to the following two equivalent inequalities: (1.13) ∞ X ∞ X am b n π < π m + n sin n=1 m=1 p (∞ X np−2 apn ) p1 ( ∞ X n=1 ) 1q nq−2 bqn n=1 and (1.14) On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Contents JJ J II I Go Back Close Quit ∞ X n=1 np−2 ∞ X am m+n m=1 !p p < sin ∞ π X p−2 p n an . Page 7 of 35 n=1 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 π p http://jipam.vu.edu.au For p = q = 2, inequalities (1.13) and (1.14) reduce respectively to (1.1) and (1.2). We find that inequalities (1.3) and (1.13) are different, although both of them are the best extensions of (1.1) with the (p, q)−parameter. The main objective of this paper is to obtain some extensions of (1.3) with the best constant factors, by introducing two parameters using the P∞λ and aαm band P n Beta function, related to the double series as ∞ n=1 m=1 (mα +nα )λ (λ, α > 0), so that inequality (1.10) can be improved. The equivalent form and some reversions are considered. On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 8 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au 2. Some Lemmas First, we need the form of the Beta function as (cf. Wang et al. [14]): Z ∞ 1 (2.1) B(u, v) := tu−1 dt = B(v, u) (u, v > 0). u+v (1 + t) 0 Lemma 2.1. If p > 0 (p 6= 1), p1 + 1q = 1, λ, α > 0, φr = φr (λ, α) > 0 (r = p, q), satisfy φp + φq = λα, define the weight function ωr (x) as ∞ Z (2.2) ωr (x) := 0 1−φr 1 x dy (xα + y α )λ y λα−φr (x > 0; r = p, q). Bicheng Yang Then for x > 0, each ωr (x) is constant, that is φp φq 1 (2.3) ωr (x) = B , (x > 0; r = p, q). α α α y α x Proof. Setting u = ωr (x) = x λα−φr 1 = α Z 0 ∞ Title Page Contents 1 in the integral (2.2), one has dy = αx u α −1 du and Z ∞ 1 α (x + xα u)λ 0 φr 1 u α −1 du λ (1 + u) 1 xu1/α On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters 1−φr x 1 −1 u α du α (r = p, q). JJ J II I Go Back Close Quit Page 9 of 35 By (2.1), since φp + φq = λα, one has (2.3). The lemma is proved. J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au Lemma 2.2. If p > 1, p1 + 1q = 1, λ, α > 0, φr > 0 (r = p, q), satisfy φp + φq = λα, and 0 < ε < qφp , then one has (2.4) ε x−1+φq − p −1+φp − qε I1 := y dxdy (xα + y α )λ 1 1 1 φp ε φq ε > B − , + − O(1). εα α qα α qα Z ∞ Z ∞ If 0 < p < 1 and 0 < ε < −qφq , with the above assumption, then one has ∞ Z X (2.5) ε m−1+φq − p −1+φp − qε I2 := y dy (mα + y α )λ m=1 0 ∞ 1 φp ε φq ε X 1 = B − , + . α α qα α qα m=1 m1+ε Proof. Setting u = y α x ∞ in the integral I1 , one has Z ∞ Z ∞ 1 −1+φq − pε −1+φp − qε y I1 = x dy dx (xα + y α )λ 1 1 Z Z φp ε 1 ∞ −1−ε ∞ 1 − qα −1 α = x u dudx λ 1 α 1 (1 + u) xα Z ∞ φαp − qαε −1 Z Z 1 φp ε u 1 ∞ −1−ε xα u α − qα −1 1 dudx du − x = (1 + u)λ εα 0 (1 + u)λ α 1 0 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 10 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au (2.6) 1 > εα Z 1 = εα Z ∞ 0 0 ∞ φp ε Z Z 1 u α − qα −1 1 ∞ −1 xα φαp − qαε −1 du − u dudx x (1 + u)λ α 1 0 φp ε −2 u α − qα −1 ε du − φp − . (1 + u)λ q y α ) in the By (2.1), it follows that (2.4) is valid. For 0 < p < 1, setting u = ( m integral of I2 , in the same manner, one has (2.5). The lemma is thus proved. On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 11 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au 3. Main Results Theorem 3.1. If p > 1, p1 + 1q = 1, λ, α > 0, 0 < φr ≤ 1 (r = p, q), φp + φq = λα and an , bn ≥ 0 satisfy 0< ∞ X np(1−φq )−1 apn < ∞ and n=1 0< ∞ X nq(1−φp )−1 bqn < ∞, n=1 then one has (3.1) ∞ X ∞ X n=1 m=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters am b n + nα )λ (mα Bicheng Yang ) p1 ( ∞ ) 1q (X ∞ X φp φq 1 , < B , np(1−φq )−1 apn nq(1−φp )−1 bqn α α α n=1 n=1 where the constant factor α1 B φp φq , α α is the best possible. Proof. By Hölder’s inequality with weight (see [15]), one has ∞ X ∞ X am b n H(am , bn ) := α (m + nα )λ n=1 m=1 ∞ X ∞ X (1−φq )/q (1−φp )/p 1 m n = am bn α α λ (1−φ )/p p (m + n ) n m(1−φq )/q n=1 m=1 Title Page Contents JJ J II I Go Back Close Quit Page 12 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au ( ≤ ) p1 # mλα−φp 1 mp(1−φq )−1 apm · α + nα )λ n1−φp (m n=1 (∞ " ∞ # ) 1q X X nλα−φq 1 × · 1−φq nq(1−φp )−1 bqn . α α λ (m + n ) m n=1 m=1 "∞ ∞ X X m=1 (3.2) Since λ, α > 0, and 1 − φr ≥ 0 (r = p, q), in view of (2.2), we rewrite (3.2) as ( H(am , bn ) < ∞ X ωp (m)mp(1−φq )−1 apm m=1 ) p1 ( ∞ X ωq (n)nq(1−φp )−1 bqn (3.3) , n=1 Bicheng Yang and then by (2.3), one has (3.1). For 0 < ε < qφp , setting ε ε n−1+φq − p , b0n = n−1+φp − q , n ∈ N, then we find (∞ X On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters ) 1q np(1−φq )−1 a0p n ) p1 ( ∞ X n=1 n=1 ) 1q nq(1−φp )−1 b0q n a0n and b0n as: a0n = ∞ X 1 =1+ n1+ε n=2 Z ∞ 1 <1+ dt t1+ε 1 1 = (1 + ε). ε Title Page Contents JJ J II I Go Back Close Quit If the constant factor 1 B α φp φq , α α in (3.1) is not the best possible, then there exists a positive constant k (with k < α1 B φαp , φαq ), such that (3.1) is still valid Page 13 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au if one replaces α1 B 1 B α φp φq , α α by k. In particular, by (2.4) and (3.3), φp ε φq ε − , + − εO(1) α qα α qα < εI1 < εH(a0m , b0n ) (∞ ) 1q ) p1 ( ∞ X X < εk nq(1−φp )−1 b0q np(1−φq )−1 a0p n n n=1 n=1 = k(1 + ε), φp φq 1 and then α B α , α ≤ k (ε → 0+ ). This contradicts the fact that k < φp φq φp φq 1 1 B , . Hence the constant factor B , in (3.1) is the best possiα α α α α α ble. The theorem is proved. Theorem 3.2. If p > 1, p1 + 1q = 1, λ, α > 0, 0 < φr ≤ 1 (r = p, q), φp + φq = λα and an ≥ 0 satisfy 0< ∞ X np(1−φq )−1 apn < ∞, n=1 (3.4) n=1 Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit then one has ∞ X On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters " n pφp −1 ∞ X am α (m + nα )λ m=1 #p Page 14 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au 1 < B α where the constant factor is equivalent to (3.1). h 1 B α φp φq , α α ip φp φq , α α p X ∞ np(1−φq )−1 apn , n=1 is the best possible. Inequality (3.4) Proof. Set " ∞ X bn := npφp −1 m=1 (mα am + nα )λ #p−1 , On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters and use (3.1) to obtain (3.5) 0< = = ∞ X n=1 ∞ X nq(1−φp )−1 bqn " n pφp −1 n=1 ∞ X ∞ X n=1 m=1 ≤ 1 B α Bicheng Yang Title Page ∞ X am α (m + nα )λ m=1 am b n + nα )λ (X ∞ φq #p Contents JJ J (mα φp , α α n=1 II I Go Back np(1−φq )−1 apn ) p1 ( ∞ X n=1 ) 1q nq(1−φp )−1 bqn Close Quit Page 15 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and 0< (∞ X ) p1 nq(1−φp )−1 bqn n=1 # ) p1 a m p = npφp −1 α + nα )λ (m n=1 m=1 ) p1 (X ∞ φp φq 1 < ∞. ≤ B , np(1−φq )−1 apn α α α n=1 (∞ X (3.6) " ∞ X It follows that (3.5) takes the form of strict inequality by using (3.1); so does (3.6). Hence, one has (3.4). On the other hand, if (3.4) is valid, by Hölder’s inequality, one has (3.7) ∞ X ∞ X am b n + nα )λ n=1 m=1 " # 1 ∞ ∞ −1+φp X X q n am h 1−φp − 1q i bn = n (mα + nα )λ n=1 m=1 (∞ " ∞ #p ) p1 ( ∞ ) 1q X X X am ≤ npφp −1 nq(1−φp )−1 bqn . α α λ (m + n ) n=1 m=1 n=1 (mα By (3.4), one has (3.1). It follows that inequalities (3.4) and (3.1) are equivalent. If the constant factor in (3.4) is not the best possible, one can obtain a contradiction that the constant factor in (3.1) is not the best possible by using (3.7). On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 16 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au Hence the constant factor in (3.4) is still the best possible. Thus the theorem is proved. 1 p Theorem 3.3. If 0 < p < 1, + 1 q = 1, A = {(λ, α); λ, α > 0, 0 < φr ≤ 1 (r = p, q), φp + φq = λα} = 6 Φ, and an , bn ≥ 0 satisfy 0< ∞ X np(1−φq )−1 apn < ∞ and 0< n=1 ∞ X nq(1−φp )−1 bqn < ∞, On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters n=1 then for (λ, α) ∈ A, one has Bicheng Yang ∞ X ∞ X am b n + nα )λ n=1 m=1 ) p1 ( ∞ ) 1q (X ∞ X φp φq 1 , nq(1−φp )−1 bqn , > B [1 − θp (n)]np(1−φq )−1 apn α α α n=1 n=1 (3.8) Title Page (mα where 0 < θp (n) = O 1 nφp < 1; the constant α1 B φp φq , α α Contents JJ J is the best possible. Proof. By the reverse of Hölder’s inequality (see [15]), following the method of proof in Theorem 3.1, since 0 < p < 1 and q < 0, one has (3.9) H(am , bn ) > (∞ X n=1 $p (n)np(1−φq )−1 apn ) p1 ( ∞ X n=1 Go Back Close Quit Page 17 of 35 ) 1q ωq (n)nq(1−φp )−1 bqn II I , J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au where ωq (n) is defined as in (2.2) and (3.10) $p (n) := ∞ X k=1 nλα−φp (nα + k α )λ 1−φp 1 k (n ∈ N). Define θp (n) as (3.11) nλα−φp θp (n) := ωp (n) 1 Z 0 Since Z ωp (n) > 0 1 1 α (n + y α )λ 1−φp 1 dy y (n ∈ N). 1−φp nλα−φp 1 dy, α α λ (n + y ) y then we find 0 < θp (n) < 1, and 1−φp Z ∞ nλα−φp 1 dy = ωp (n) [1 − θp (n)] . (3.12) $p (n) > (nα + y α )λ y 1 By (3.12), (2.3) and (3.9), one has (3.8). Since 1−φp Z nλα−φp 1 1 1 1 1 (3.13) 0 < θp (n) < dy = · φp , λα ωp (n) 0 n y ωp (n)φp n and ωp (n) is a constant, we have θp (n) = O n1φp (n → ∞). ε For 0 < ε < min{q(φp − 1), −qφq }, setting a0n and b0n as: a0n = n−1+φq − p , ε b0n = n−1+φp − q , n ∈ N, since φp > 0, then ∞ X 1 O = O(1) (ε → 0+ ), φ p+1+ε n n=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 18 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and (3.14) (∞ X [1 − θp (n)]np(1−φq )−1 a0p n ) p1 ( ∞ X n=1 ) 1q nq(1−φp )−1 b0q n n=1 p1 P∞ 1 ∞ O X n=1 1 nφp+1+ε P = 1 − ∞ 1 n1+ε n=1 n1+ε n=1 ∞ X 1 1 = (1 − o(1)) p . 1+ε n n=1 φp φq 1 If the constant α B α , α in (3.8) is not the best possible, then there exists a positive number K (with K > α1 B φαp , φαq ), such that (3.8) is still valid if one φp φq 1 replaces α B α , α by K. In particular, by (3.14) and (2.5), one has ∞ X 1 1 {1 − o(1)} p K 1+ε n n=1 (∞ ) 1q ) p1 ( ∞ X X =K [1 − θp (n)]np(1−φq )−1 a0p nq(1−φp )−1 b0q n n < n=1 H(a0m , b0n ) 1 < I2 = B α n=1 φp ε φq ε − , + α qα α qα X ∞ n=1 1 n On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 19 of 35 , 1+ε J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and then K ≤ α1 B φp φq , α α (ε → 0+ ). By this contradiction we can conclude that the constant α1 B φαp , φαq in (3.8) is the best possible. Thus the theorem is proved. Theorem 3.4. If 0 < p < 1, 1 p + 1 q = 1, A = {(λ, α); λ, α > 0, 0 < φr ≤ 1 (r = p, q), φp + φq = λα} = 6 Φ, and an , bn ≥ 0 satisfy 0< ∞ X On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters np(1−φq )−1 apn < ∞, n=1 Bicheng Yang for (λ, α) ∈ A, one has " ∞ ∞ X X pφp −1 (3.15) n #p am (mα + nα )λ n=1 m=1 p X ∞ 1 φp φq > B , [1 − θp (n)]np(1−φq )−1 apn , α α α n=1 h ip φp φq 1 1 where 0 < θp (n) = O nφp < 1, and the constant factor α B α , α is the best possible. Inequality (3.15) is equivalent to (3.8). Title Page Contents JJ J II I Go Back Close Quit Proof. Still setting " bn := n pφp −1 ∞ X am α (m + nα )λ m=1 Page 20 of 35 #p−1 , J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au by (3.8), one has (3.16) 0< ∞ X nq(1−φp )−1 bqn n=1 #p ∞ X ∞ X a am bn m pφp −1 = = n α α λ α (m + n ) (m + nα )λ n=1 m=1 n=1 m=1 ) p1 (X ∞ φp φq 1 ≥ B , [1 − θp (n)]np(1−φq )−1 apn α α α n=1 (∞ ) 1q X × nq(1−φp )−1 bqn " ∞ X ∞ X On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang n=1 and 0< (∞ X Title Page ) p1 Contents nq(1−φp )−1 bqn JJ J n=1 = (∞ X " npφp −1 n=1 (3.17) P∞ ≥ 1 B α ∞ X m=1 φp φq , α α (mα (X ∞ am + nα )λ #p ) p1 Go Back ) p1 [1 − θp (n)]np(1−φq )−1 apn II I . n=1 If n=1 nq(1−φp )−1 bqn < ∞, by (3.8), (3.16) takes the form of strict inP∞usingq(1−φ p )−1 q equality; so does (3.17). If n=1 n bn = ∞, (3.17) takes naturally strict inequality. Hence we have (3.15). Close Quit Page 21 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au On the other hand, if (3.15) is valid, by the reverse of Hölder’s inequality, (3.18) ∞ X ∞ X am b n + nα )λ n=1 m=1 " ∞ # ∞ X X n 1q −1+φp am 1 = [n1−φp − q bn ] α α λ (m + n ) n=1 m=1 ) 1q (∞ " ∞ #p ) p1 ( ∞ X X X a m . ≥ nq(1−φp )−1 bqn npφp −1 α + nα )λ (m n=1 n=1 m=1 (mα Hence by (3.15), one has (3.8). If the constant factor in (3.15) is not the best possible, we can conclude that the constant factor in (3.8) is not the best possible by using (3.18). The theorem is proved. Note: In view of (3.1), if φr = φr (λ, α) (r = p, q) satisfy B(φp (1, 1), φq (1, 1)) = sin π , π p and rφr (1, 1) = 1 (r = p, q), one can get a best extension of (1.3); if π B(φp (1, 1), φq (1, 1)) = sin(π/p) (or π2 ), and rφr (1, 1) 6= 1 (r = p, q), one can get a best extension of (1.1) but not a best extension of (1.3). For example, setting 1 φr = r (α − 2) + 1 λ (r = p, q), then rφr (1, 1) = r − 1 6= 1, by Theorems 3.1 – 3.4, one can get a best extension of (1.13) and (1.1) as follows: On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 22 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au Corollary 3.5. If p > 1, p1 + 1q = 1, λ > 0, α > 2−min{p, q}, 1 (r = p, q), an, bn ≥ 0, satisfy 0< ∞ X 1 r (α − 2) + 1 λ ≤ np[1−λ(α−1)]+(α−2)λ−1 apn < ∞ n=1 and 0< ∞ X nq[1−λ(α−1)]+(α−2)λ−1 bqn < ∞, n=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters one has equivalent inequalities as: (3.19) ∞ ∞ X X n=1 m=1 am b n < Kλ,α (p) + nα )λ (∞ ) p1 X × np[1−λ(α−1)]+(α−2)λ−1 apn Bicheng Yang (mα Title Page Contents n=1 × (∞ X ) 1q nq[1−λ(α−1)]+(α−2)λ−1 bqn n=1 II I Go Back and (3.20) JJ J ∞ X n=1 " n (p+α−2)λ−1 ∞ X am α (m + nα )λ m=1 Close #p < [Kλ,α (p)]p Quit ∞ X n=1 Page 23 of 35 np[1−λ(α−1)]+(α−2)λ−1 apn , J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au where 1 p+α−2 q+α−2 Kλ,α (p) = B λ ,λ α αp αq and [Kλ,α (p)]p are the best possible. In particular, (i) for α = 1, one has 0 < λ ≤ min{p, q} and (1.11); (ii) for λ = 1, one has 2 − min{p, q} < α ≤ 2 and (3.21) ∞ X ∞ X am b n mα + nα n=1 m=1 (∞ ) p1 ( ∞ ) 1q X X < K1,α (p) n(p−1)(2−α)−1 apn n(q−1)(2−α)−1 bqn n=1 Contents ∞ X n=1 " n p+α−3 ∞ X am α m + nα m=1 #p p < [K1,α (p)] ∞ X n(p−1)(2−α)−1 apn . n=1 If 0 < p < 1, for (λ, α) = (1, 2) ∈ A(6= Φ), by (3.8), (3.15) and (3.13), one can obtain two equivalent reversions as (3.23) Bicheng Yang Title Page n=1 and (3.22) On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters ∞ X ∞ X am b n π > 2 2 m +n 2 n=1 m=1 (∞ X n=1 1− 2 πn apn n ) p1 ( ∞ )1 X bq q n n=1 JJ J II I Go Back Close Quit Page 24 of 35 n J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and (3.24) ∞ X n=1 " n p−1 ∞ X am 2 m + n2 m=1 #p > ∞ π p X 2 n=1 2 1− πn apn , n where the constant factors in the above inequalities are the best possible. On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 25 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au 4. Some Best Extensions of (1.3) Setting φr = λα r (r = p, q), by Theorems 3.1 – 3.4, one has Corollary 4.1. If p > 1, satisfy 0< ∞ X 1 p + n(p−1)(1−λα) apn 1 q = 1, λ, α > 0, λα ≤ min{p, q}, an , bn ≥ 0, <∞ and 0 < n=1 ∞ X n(q−1)(1−λα) bqn < ∞, n=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters then one has the following equivalent inequalities: (4.1) ∞ X ∞ X Bicheng Yang am b n (mα + nα )λ n=1 m=1 Kλ (p) < α (∞ X n(p−1)(1−λα) apn ) p1 ( ∞ X n=1 ) 1q n(q−1)(1−λα) bqn n=1 (4.2) " n λα−1 n=1 where Kλ (p) = B ∞ X am α (m + nα )λ m=1 λ λ , p q #p Kλ (p) < α p X ∞ Contents JJ J and ∞ X Title Page n(p−1)(1−λα) apn , n=1 II I Go Back Close Quit . In particular, Page 26 of 35 (i) for α = 1, one has 0 < λ ≤ min{p, q} and the following two equivalent J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au inequalities: (4.3) ∞ X ∞ X am b n (m + n)λ n=1 m=1 < Kλ (p) (∞ X n(p−1)(1−λ) apn n=1 ) p1 ( ∞ X ) 1q n(q−1)(1−λ) bqn n=1 and (4.4) ∞ X " nλ−1 n=1 ∞ X am (m + n)λ m=1 #p On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters ∞ X p < [Kλ (p)] n(p−1)(1−λ) apn ; n=1 Bicheng Yang (ii) for λ = 1, 0 < α ≤ min{p, q} one has two equivalent inequalities as: (4.5) Title Page ∞ X ∞ X am b n mα + nα n=1 m=1 < π α sin πp Contents (∞ X n(p−1)(1−α) apn ) p1 ( ∞ X ) 1q n(q−1)(1−α) bqn n=1 n=1 and (4.6) JJ J II I Go Back Close ∞ X n=1 " n α−1 ∞ X am α m + nα m=1 #p < p ∞ X π n(p−1)(1−α) apn , π α sin p n=1 where the constant factors in the above inequalities are the best possible. Quit Page 27 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au Note: Since for 0 < p < 1, φq = λα < 0, then A = Φ. It follows that both q + 1r (r = p, q), by (4.1) and (4.2) do not possess reversions. Setting φr = λα−1 2 Theorems 3.1 – 3.4, one has n o Corollary 4.2. If p > 1, p1 + 1q = 1, λ, α > 0, 1 − 2 min p1 , 1q < λα ≤ n o 1 + 2 min p1 , 1q , an , bn ≥ 0, satisfy 0< ∞ X n p (1−λα) 2 apn <∞ and n=1 0< ∞ X q n 2 (1−λα) bqn < ∞, n=1 then one has the following equivalent inequalities: (4.7) ∞ ∞ X X am b n α (m + nα )λ n=1 m=1 pλα − p + 2 qλα − q + 2 1 < B , α 2pα 2qα (∞ ) p1 ( ∞ ) 1q X p X q × n 2 (1−λα) apn n 2 (1−λα) bqn n=1 Bicheng Yang Title Page Contents JJ J II I n=1 Go Back and (4.8) On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters ∞ X n=1 #p am dy (mα + nα )λ m=1 p X ∞ p 1 pλα − p + 2 qλα − q + 2 < B , n 2 (1−λα) apn . α 2pα 2qα n=1 " n p (λα−1) 2 ∞ X Close Quit Page 28 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au In particular, n o n o (i) for α = 1, one has 1 − 2 min p1 , 1q < λ ≤ 1 + 2 min p1 , 1q , and the following two equivalent inequalities: ∞ X ∞ X pλ − p + 2 qλ − q + 2 am b n (4.9) <B , λ (m + n) 2p 2q n=1 m=1 ) 1q ) p1 ( ∞ (∞ X q X p n 2 (1−λ) bqn × n 2 (1−λ) apn n=1 n=1 and ∞ X " ∞ X Bicheng Yang #p am dy (m + n)λ m=1 n=1 p X ∞ p pλ − p + 2 qλ − q + 2 < B , n 2 (1−λα) apn ; 2p 2q n=1 n o n o (ii) for λ = 1, one has 1 − 2 min p1 , 1q < α ≤ 1 + 2 min p1 , 1q and two equivalent inequalities as: ∞ X ∞ X 1 pα − p + 2 qα − q + 2 am b n (4.11) < B , α + nα m α 2pα 2qα n=1 m=1 (∞ ) p1 ( ∞ ) 1q X p X q × n 2 (1−α) apn n 2 (1−α) bqn (4.10) p n 2 (λ−1) n=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters n=1 Title Page Contents JJ J II I Go Back Close Quit Page 29 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and (4.12) ∞ X #p am dy mα + nα m=1 p X ∞ p 1 pα − p + 2 qα − q + 2 < B , n 2 (1−α) apn , α 2pα 2qα n=1 " n p (α−1) 2 n=1 ∞ X where the constant factors in the above inequalities are the best possible. Note: Since for 0 < p < 1, we find λα − 1 1 A = (λ, α); λ, α > 0, 0 < + ≤ 1 (r = p, q) = Φ, 2 r it follows that both (4.7) and (4.8) do not possess reversions. Setting φr = 1 1 − r (λα − 2) + 1 (r = p, q), by Theorems 3.1 – 3.4, one has Corollary 4.3. If p > 1, p1 + 1q = 1, λ, α > 0, 2 − min{p, q} < λα ≤ 2, an , bn ≥ 0, satisfy ∞ ∞ X X 0< n1−λα apn < ∞ and 0 < n1−λα bqn < ∞, n=1 n=1 then one has the following equivalent inequalities: ∞ X ∞ X 1 p + λα − 2 q + λα − 2 am bn (4.13) < B , α + nα )λ (m α pα qα n=1 m=1 (∞ ) p1 ( ∞ ) 1q X X × n1−λα apn n1−λα bqn n=1 n=1 On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 30 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au and (4.14) #p a m n(p−1)(λα−1) α + nα )λ (m n=1 m=1 p X ∞ 1 p + λα − 2 q + λα − 2 < B , n1−λα apn , α pα qα n=1 ∞ X " ∞ X where the constant factors in the above inequalities are the best possible. If 0 < p < 1, one has (α/2, α) ∈ A and two equivalent reversions as: ) 1q (∞ ) p1 ( ∞ ∞ X ∞ X1 X X am b n 1 1 p bqn (4.15) > kα 1− an α + nα )2/α n (m k n n α n=1 m=1 n=1 n=1 and Bicheng Yang Title Page ∞ X " ∞ X #p ∞ X am 1 1 p p > k 1 − an , α α + nα )2/α (m k n n α n=1 m=1 n=1 where kα = α1 B α1 , α1 , and the constant factors are the best possible. (4.16) On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters np−1 Proof. For 0 < p < 1, 1 (λα − 2) + 1 ≤ 1 φr = 1 − r JJ J II I Go Back (r = p, q), we obtain λα = 2 and φr = 1. By (3.13), we find 0 < θp (n) < Contents 1 1 1 · φp = . ωp (n)φp n kα n Close Quit Page 31 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au Hence by (3.8) and (3.15), one has (4.15) and (4.16). The corollary is proved. On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang Title Page Contents JJ J II I Go Back Close Quit Page 32 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au Remark 1. (i) For α = 1, by (4.13) and (4.14), one has (1.6) and (1.7); for λ = 1, by (4.13) and (4.14), one has (1.8) and (1.9). It follows that (4.13) is an extension of (1.6) and (1.8), which is an improvement of (1.10), and (4.14) is an extension of (1.7) and (1.9). (4.11) and (4.12) are extensions of (3.23) and (3.24). (ii) Inequalities (1.6), (4.3) and (4.9) are different extensions of (1.3) with a parameter λ; inequalities (1.8), (4.5) and (4.11) are different extensions of (1.3) with a parameter α and inequalities (4.1), (4.7) and (4.13) are different extensions of (1.3) with two parameters λ and α. On Best Extensions of Hardy-Hilbert’s Inequality with Two Parameters Bicheng Yang (iii) Inequalities (1.7), (4.4) and (4.10) are different extensions of (1.4) with a parameter λ; inequalities (1.9), (4.6) and (4.12) are different extensions of (1.4) with a parameter α and inequalities (4.2), (4.8) and (4.14) are different extensions of (1.4) with two parameters λ and α. Since the above inequalities and some reversions are all with the best constant factors, one gives some new results. Title Page Contents JJ J II I Go Back Close Quit Page 33 of 35 J. Ineq. Pure and Appl. Math. 6(3) Art. 81, 2005 http://jipam.vu.edu.au References [1] G.H. HARDY, J.E. LITTLEWOOD AND G. POLYA, Inequalities, Cambridge University Press, Cambridge, 1952. [2] G.H. HARDY, Note on a theorem of Hilbert concerning series of positive terms, Proc. Math. Soc., 23(2) (1925), Records of Proc. XLV-XLVI. [3] D.S. MINTRINOVIĆ, J.E. PEČARIĆ AND A.M. 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