Volume 10 (2009), Issue 3, Article 86, 5 pp. ON SOME NEW FRACTIONAL INTEGRAL INEQUALITIES SOUMIA BELARBI AND ZOUBIR DAHMANI D EPARTMENT OF M ATHEMATICS , U NIVERSITY OF M OSTAGANEM soumia-math@hotmail.fr zzdahmani@yahoo.fr Received 23 May, 2009; accepted 24 June, 2009 Communicated by G. Anastassiou A BSTRACT. In this paper, using the Riemann-Liouville fractional integral, we establish some new integral inequalities for the Chebyshev functional in the case of two synchronous functions. Key words and phrases: Fractional integral inequalities, Riemann-Liouville fractional integral. 2000 Mathematics Subject Classification. 26D10, 26A33. 1. I NTRODUCTION Let us consider the functional [1]: Z b Z b Z b 1 1 1 (1.1) T (f, g) := f (x) g (x) dx − f (x) dx g (x) dx , b−a a b−a b−a a a where f and g are two integrable functions which are synchronous on [a, b] i.e. (f (x) − f (y))(g(x) − g(y)) ≥ 0, for any x, y ∈ [a, b] . Many researchers have given considerable attention to (1.1) and a number of inequalities have appeared in the literature, see [3, 4, 5]. The main purpose of this paper is to establish some inequalities for the functional (1.1) using fractional integrals. 2. D ESCRIPTION OF F RACTIONAL C ALCULUS We will give the necessary notation and basic definitions below. For more details, one can consult [2, 6]. Definition 2.1. A real valued function f (t), t ≥ 0 is said to be in the space Cµ , µ ∈ R if there exists a real number p > µ such that f (t) = tp f1 (t), where f1 (t) ∈ C([0, ∞[). Definition 2.2. A function f (t), t ≥ 0 is said to be in the space Cµn , n ∈ R, if f (n) ∈ Cµ . The authors would like to thank professor A. El Farissi for his helpful. 139-09 2 S OUMIA B ELARBI AND Z OUBIR DAHMANI Definition 2.3. The Riemann-Liouville fractional integral operator of order α ≥ 0, for a function f ∈ Cµ , (µ ≥ −1) is defined as Z t 1 α (2.1) J f (t) = (t − τ )α−1 f (τ )dτ ; α > 0, t > 0, Γ(α) 0 J 0 f (t) = f (t), R∞ where Γ(α) := 0 e−u uα−1 du. For the convenience of establishing the results, we give the semigroup property: (2.2) J α J β f (t) = J α+β f (t), α ≥ 0, β ≥ 0, which implies the commutative property: (2.3) J α J β f (t) = J β J α f (t). From (2.1), when f (t) = tµ we get another expression that will be used later: Γ(µ + 1) α+µ (2.4) J α tµ = t , α > 0; µ > −1, t > 0. Γ(α + µ + 1) 3. M AIN R ESULTS Theorem 3.1. Let f and g be two synchronous functions on [0, ∞[. Then for all t > 0, α > 0, we have: Γ(α + 1) α (3.1) J α (f g)(t) ≥ J f (t)J α g(t). tα Proof. Since the functions f and g are synchronous on [0, ∞[, then for all τ ≥ 0, ρ ≥ 0, we have (3.2) f (τ ) − f (ρ) g(τ ) − g(ρ) ≥ 0. Therefore (3.3) f (τ )g(τ ) + f (ρ)g(ρ) ≥ f (τ )g(ρ) + f (ρ)g(τ ). Now, multiplying both sides of (3.3) by (t−τ )α−1 , Γ(α) τ ∈ (0, t), we get (t − τ )α−1 (t − τ )α−1 f (τ )g(τ ) + f (ρ)g(ρ) Γ(α) Γ(α) (t − τ )α−1 (t − τ )α−1 ≥ f (τ )g(ρ) + f (ρ)g(τ ). Γ(α) Γ(α) Then integrating (3.4) over (0, t), we obtain: Z t Z t 1 1 α−1 (3.5) (t − τ ) f (τ )g(τ )dτ + (t − τ )α−1 f (ρ)g(ρ)dτ Γ(α) 0 Γ(α) 0 Z t Z t 1 1 α−1 ≥ (t − τ ) f (τ )g(ρ)dτ + (t − τ )α−1 f (ρ)g(τ )dτ. Γ(α) 0 Γ(α) 0 Consequently, Z t 1 α (3.6) J (f g)(t) + f (ρ) g (ρ) (t − τ )α−1 dτ Γ (α) 0 Z Z g (ρ) t f (ρ) t α−1 ≥ (t − τ ) f (τ ) dτ + (t − τ )α−1 g (τ ) dτ. Γ (α) 0 Γ (α) 0 (3.4) J. Inequal. Pure and Appl. Math., 10(3) (2009), Art. 86, 5 pp. http://jipam.vu.edu.au/ F RACTIONAL I NTEGRAL I NEQUALITIES 3 So we have (3.7) J α (f g)(t) + f (ρ) g (ρ) J α (1) ≥ g (ρ) J α (f )(t) + f (ρ) J α (g)(t). Multiplying both sides of (3.7) by (3.8) (t−ρ)α−1 , Γ(α) ρ ∈ (0, t), we obtain: (t − ρ)α−1 α (t − ρ)α−1 J (f g)(t) + f (ρ) g (ρ) J α (1) Γ (α) Γ (α) (t − ρ)α−1 (t − ρ)α−1 α ≥ g (ρ) J f (t) + f (ρ) J α g(t). Γ (α) Γ (α) Now integrating (3.8) over (0, t), we get: Z Z t (t − ρ)α−1 J α (1) t α (3.9) J (f g)(t) dρ + f (ρ)g(ρ)(t − ρ)α−1 dρ Γ(α) Γ(α) 0 0 Z Z J α f (t) t J α g(t) t α−1 ≥ (t − ρ) g(ρ)dρ + (t − ρ)α−1 f (ρ)dρ. Γ(α) 0 Γ(α) 0 Hence J α (f g)(t) ≥ (3.10) 1 J α (1) J α f (t)J α g(t), and this ends the proof. The second result is: Theorem 3.2. Let f and g be two synchronous functions on [0, ∞[. Then for all t > 0, α > 0, β > 0, we have: (3.11) tα tβ J β (f g)(t) + J α (f g)(t) ≥ J α f (t)J β g(t) + J β f (t)J α g(t). Γ (α + 1) Γ (β + 1) Proof. Using similar arguments as in the proof of Theorem 3.1, we can write (3.12) (t − ρ)β−1 α (t − ρ)β−1 J (f g) (t) + J α (1) f (ρ) g (ρ) Γ (β) Γ (β) ≥ (t − ρ)β−1 (t − ρ)β−1 g (ρ) J α f (t) + f (ρ) J α g (t) . Γ (β) Γ (β) By integrating (3.12) over (0, t) , we obtain Z t Z (t − ρ)β−1 J α (1) t α (3.13) J (f g)(t) dρ + f (ρ) g (ρ) (t − ρ)β−1 dρ Γ (β) Γ (β) 0 0 Z t Z α J f (t) J α g (t) t β−1 ≥ (t − ρ) g (ρ) dρ + (t − ρ)β−1 f (ρ) dρ, Γ (β) 0 Γ (β) 0 and this ends the proof. Remark 1. The inequalities (3.1) and (3.11) are reversed if the functions are asynchronous on [0, ∞[ (i.e. (f (x) − f (y))(g(x) − g(y)) ≤ 0, for any x, y ∈ [0, ∞[). Remark 2. Applying Theorem 3.2 for α = β, we obtain Theorem 3.1. The third result is: J. Inequal. Pure and Appl. Math., 10(3) (2009), Art. 86, 5 pp. http://jipam.vu.edu.au/ 4 S OUMIA B ELARBI AND Z OUBIR DAHMANI Theorem 3.3. Let (fi )i=1,...,n be n positive increasing functions on [0, ∞[. Then for any t > 0, α > 0, we have ! n n Y Y 1−n α α (3.14) J fi (t) ≥ (J (1)) J α fi (t) . i=1 i=1 Proof. We prove this theorem by induction. Clearly, for n = 1, we have J α (f1 ) (t) ≥ J α (f1 ) (t) , for all t > 0, α > 0. For n = 2, applying (3.1), we obtain: J α (f1 f2 ) (t) ≥ (J α (1))−1 J α (f1 ) (t) J α (f2 ) (t) , for all t > 0, α > 0. Now, suppose that (induction hypothesis) ! n−1 n−1 Y Y 2−n α α fi (t) ≥ (J (1)) J α fi (t) , (3.15) J i=1 t > 0, α > 0. i=1 Qn−1 Since (fi )i=1,...,n are positive increasing functions, then fi (t) is an increasing function. Qn−1 i=1 Hence we can apply Theorem 3.1 to the functions i=1 fi = g, fn = f. We obtain: ! ! n n−1 Y Y (3.16) Jα fi (t) = J α (f g) (t) ≥ (J α (1))−1 J α fi (t) J α (fn ) (t) . i=1 i=1 Taking into account the hypothesis (3.15), we obtain: ! n Y (3.17) Jα fi (t) ≥ (J α (1))−1 ((J α (1))2−n i=1 n−1 Y ! J α fi (t))J α (fn ) (t) , i=1 and this ends the proof. We further have: Theorem 3.4. Let f and g be two functions defined on [0, +∞[ , such that f is increasing, g is differentiable and there exists a real number m := inf t≥0 g 0 (t) . Then the inequality mt α J f (t) + mJ α (tf (t)) (3.18) J α (f g)(t) ≥ (J α (1))−1 J α f (t)J α g(t) − α+1 is valid for all t > 0, α > 0. Proof. We consider the function h (t) := g (t) − mt. It is clear that h is differentiable and it is increasing on [0, +∞[. Then using Theorem 3.1, we can write: (3.19) J α (g − mt) f (t) ≥ (J α (1))−1 J α f (t) J α g(t) − mJ α (t) m (J α (1))−1 tα+1 α ≥ (J (1)) J f (t)J g(t) − J f (t) Γ (α + 2) mΓ (α + 1) t α ≥ (J α (1))−1 J α f (t)J α g(t) − J f (t) Γ (α + 2) mt α ≥ (J α (1))−1 J α f (t)J α g(t) − J f (t). α+1 α −1 α α Hence (3.20) J α (f g)(t) ≥ (J α (1))−1 J α f (t)J α g(t) − Theorem 3.4 is thus proved. J. Inequal. Pure and Appl. Math., 10(3) (2009), Art. 86, 5 pp. mt α J f (t) + mJ α (tf (t)) , α+1 t > 0, α > 0. http://jipam.vu.edu.au/ F RACTIONAL I NTEGRAL I NEQUALITIES 5 Corollary 3.5. Let f and g be two functions defined on [0, +∞[. (A) Suppose that f is decreasing, g is differentiable and there exists a real number M := supt≥0 g 0 (t). Then for all t > 0, α > 0, we have: Mt α J f (t) + M J α (tf (t)) . α+1 (B) Suppose that f and g are differentiable and there exist m1 := inf t≥0 f 0 (x) , m2 := inf t≥0 g 0 (t). Then we have (3.21) J α (f g)(t) ≥ (J α (1))−1 J α f (t)J α g(t) − (3.22) J α (f g)(t) − m1 J α tg(t) − m2 J α tf (t) + m1 m2 J α t2 ≥ (J α (1))−1 J α f (t)J α g(t) − m1 J α tJ α g(t) − m2 J α tJ α f (t) + m1 m2 (J α t)2 . (C) Suppose that f and g are differentiable and there exist M1 := supt≥0 f 0 (t) , M2 := supt≥0 g 0 (t) . Then the inequality (3.23) J α (f g)(t) − M1 J α tg(t) − M2 J α tf (t) + M1 M2 J α t2 ≥ (J α (1))−1 J α f (t)J α g(t) − M1 J α tJ α g(t) − M2 J α tJ α f (t) + M1 M2 (J α t)2 . is valid. Proof. (A): Apply Theorem 3.1 to the functions f and G(t) := g(t) − m2 t. (B): Apply Theorem 3.1 to the functions F and G, where: F (t) := f (t) − m1 t, G(t) := g(t) − m2 t. To prove (C), we apply Theorem 3.1 to the functions F (t) := f (t) − M1 t, G(t) := g(t) − M2 t. R EFERENCES [1] P.L. 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