Research article

Some new Chebyshev type inequalities utilizing generalized fractional integral operators

  • Received: 03 October 2019 Accepted: 28 November 2019 Published: 14 January 2020
  • MSC : 26D15, 26A33, 26D10

  • Chebyshev type inequalities for the generalized fractional integral operators are studied based on two synchronous functions in a rather general form. The main results of this paper generalize some previous results obtained by the authors. We also present the special cases of related inequalities for this type of fractional integral is obtained.

    Citation: Fuat Usta, Hüseyin Budak, Mehmet Zeki Sarıkaya. Some new Chebyshev type inequalities utilizing generalized fractional integral operators[J]. AIMS Mathematics, 2020, 5(2): 1147-1161. doi: 10.3934/math.2020079

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  • Chebyshev type inequalities for the generalized fractional integral operators are studied based on two synchronous functions in a rather general form. The main results of this paper generalize some previous results obtained by the authors. We also present the special cases of related inequalities for this type of fractional integral is obtained.


    In recent years, there has been an increasing interest in the fractional calculus. One of the significant motivations for such deep interest in the subject is its capability to model a number of natural phenomena, see, for example, the papers [9,12]. On the other hand Chebyshev inequality has broad practicability in statistical problems, numerical quadrature, probability and transform theory, and the bounding of special functions. Its basic appeal develops out of a desire to approximate, for instance, information in the form of a particular measure of the product of functions in terms of the products of the individual function measures. It is, also, of great interest in differential and difference equations [7,13].

    The essential destination of the present study is to prove a Chebyshev type inequality for the generalized fractional integral operators. After some preliminaries and summarization of some previous known results in Section 2, Section 3 deals with general Chebyshev type inequalities for generalized fractional integral operators. Finally, some concluding remarks are given in Section 4.

    In this section we recall some basic definitions and previous results which will be used in what follows.

    In 1882, Chebyshev [3] proved the following inequality:

    Theorem 2.1. Let f and g be two integrable functions in [0,1]. If both functions are simultaneously increasing or decreasing for the same values of x in [0,1], then

    10f(x)g(x)dx10f(x)dx10g(x)dx. (2.1)

    If one function is increasing and the other is decreasing for the same values of x in [0,1], then (2.1) reverses. In the last years, many papers were devoted to the generalization of the inequalities (2.1), we can mention the works [1,2,4,5,6,8,11,15,16,17,18,19].

    In [14], Raina defined the following results connected with the general class of fractional integral operators.

    Fσρ,λ(x)=Fσ(0),σ(1),...ρ,λ(x)=k=0σ(k)Γ(ρk+λ)xk (ρ,λ>0;|x|<R), (2.2)

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers and R is the set of real numbers. With the help of (2.2), in [14], Raina defined the following fractional integral operators, as follows:

    Jσρ,λ,a+;ωf(x)=xa(xt)λ1Fσρ,λ[ω(xt)ρ]f(t)dt,  x>a, (2.3)

    The importance of these operators stems indeed from their generality. Many useful fractional integral operators can be obtained by specializing the coefficient σ(k). Here, we just point out that the classical Riemann-Liouville fractional integrals Iαa+ of order α defined by (see, [10])

    (Iαa+f)(x):=1Γ(α)xa(xt)α1f(t)dt  (x>a;α>0), (2.4)

    follow easily by setting

    λ=ασ(0)=1, w=0, (2.5)

    in (2.3).

    In [19], Usta et. al gave the following Chebychev type inequalities for the generalized fractional integral operators:

    Theorem 2.2. Let f and g be two synchronous functions on [0,), that is they are having the same sense of variation on [0,). Then for all t,ρ,λ>0 and wR, we have

    Jσρ,λ,0+;ω(1)(t)Jσρ,λ,0+;ω(fg)(t)Jσρ,λ,0+;ωf(t)Jσρ,λ,0+;ωg(t), (2.6)

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Theorem 2.3. Let f and g be two synchronous functions on [0,), that is they are having the same sense of variation on [0,). Then for all t>0 and ρ1,ρ2,λ1,λ2>0 and w1,w2R, we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fg)(t)Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)+Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(f)(t) (2.7)

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    For more details, one may consult [19].

    In this section, we will present some fractional integral inequalities for functions defined on the positive real line with the help of fractional integral operators given above. The inequalities to be given in this section are a generalization of the former inequalities.

    Theorem 3.1. Let f and g be two synchronous functions on [0,), that is they are having the same sense of variation on [0,) and h0. Then for all t>0 and ρ1,ρ2,λ1,λ2>0 and w1,w2R, we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fgh)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fgh)(t)Jσ1ρ1,λ1,0+;ω1(hf)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)+Jσ1ρ1,λ1,0+;ω1(hg)(t)Jσ2ρ2,λ2,0+;ω2(f)(t)+Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(hg)(t)+Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(hf)(t)Jσ1ρ1,λ1,0+;ω1(fg)(t)Jσ2ρ2,λ2,0+;ω2(h)(t)Jσ1ρ1,λ1,0+;ω1(h)(t)Jσ2ρ2,λ2,0+;ω2(fg)(t)

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. Let f, g and h be three functions satisfying the conditions of Theorem 3.1. Then, we have

    (f(η)f(ξ))(g(η)g(ξ))(h(η)+h(ξ))0.

    Therefore

    f(η)g(η)h(η)+f(ξ)g(ξ)h(ξ)h(η)f(η)g(ξ)+h(η)f(ξ)g(η)+h(ξ)f(η)g(ξ)+h(ξ)f(ξ)g(η)f(η)g(η)h(ξ)f(ξ)g(ξ)h(η). (3.1)

    Now, by multiplying both sides of (3.1) by (tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2], we obtain:

    (tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]f(η)g(η)h(η)+(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]f(ξ)g(ξ)h(ξ)(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]h(η)f(η)g(ξ)+(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]h(η)f(ξ)g(η)+(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]h(ξ)f(η)g(ξ)+(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]h(ξ)f(ξ)g(η)(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]f(η)g(η)h(ξ)(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]f(ξ)g(ξ)h(η). (3.2)

    Finally, if we double integrate (3.2) with respect to η and ξ over (0,t)×(0,t), we get the desired result.

    Corollary 3.2. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.1, we obtain the following inequality

    tλFσρ,λ+1[ωtρ]Jσρ,λ,0+;ω(fgh)(t)+Jσρ,λ,0+;ω(h)(t)Jσρ,λ,0+;ω(fg)(t)Jσρ,λ,0+;ω(hf)(t)Jσρ,λ,0+;ω(g)(t)+Jσρ,λ,0+;ω(hg)(t)Jσρ,λ,0+;ω(f)(t)

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Remark 3.3. If we choose h=1 in Theorem 3.1, Theorem 3.1 reduce to Theorem 2.3 which was proved by Usta et al. in [19].

    Theorem 3.4. Let f, g and h be three monotonic functions defined on [0,), satisfying the following

    (f(η)f(ξ))(g(η)g(ξ))(h(η)h(ξ))0

    for all η,ξ[0,t], then for all t>0 and ρ1,ρ2,λ1,λ2>0 and w1,w2R, we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fgh)(t)tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fgh)(t)Jσ1ρ1,λ1,0+;ω1(hf)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)+Jσ1ρ1,λ1,0+;ω1(hg)(t)Jσ2ρ2,λ2,0+;ω2(f)(t)Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(hg)(t)Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(hf)(t)+Jσ1ρ1,λ1,0+;ω1(fg)(t)Jσ2ρ2,λ2,0+;ω2(h)(t)Jσ1ρ1,λ1,0+;ω1(h)(t)Jσ2ρ2,λ2,0+;ω2(fg)(t)

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. The proof is similar to previous theorem.

    Theorem 3.5. Let f, g be two functions on [0,). Then for all t>0 and ρ1,ρ2,λ1,λ2>0 and w1,w2R, we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(f2)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(g2)(t)2Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(g)(t),

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. As

    ((f(η)g(ξ))20

    we have

    f2(η)+g2(ξ)2f(η)g(ξ). (3.3)

    Now, by multiplying both sides of (3.3) by (tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2], we get

    (tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]f2(η)+(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]g2(ξ)2(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]f(η)g(ξ). (3.4)

    Finally by double integration (3.4) over (0,t)×(0,t), we get the desired result.

    Corollary 3.6. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.5, we obtain the following inequality

    tλFσρ,λ+1[ωtρ]Jσρ,λ,0+;ω(f2)(t)+tλFσρ,λ+1[ωtρ]Jσρ,λ,0+;ω(g2)(t)2Jσρ,λ,0+;ω(f)(t)Jσρ,λ,0+;ω(g)(t).

    In particular

    tλFσρ,λ+1[ωtρ]Jσρ,λ,0+;ω(f2)(t)[Jσρ,λ,0+;ω(f)(t)]2

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Theorem 3.7. Let f, g be two functions on [0,). Then for all t>0 and ρ1,ρ2,λ1,λ2>0 and w1,w2R, we have

    Jσ1ρ1,λ1,0+;ω1(f2)(t)Jσ2ρ2,λ2,0+;ω2(g2)(t)+Jσ2ρ2,λ2,0+;ω2(f2)(t)Jσ1ρ1,λ1,0+;ω1(g2)(t)2Jσ1ρ1,λ1,0+;ω1(fg)(t)Jσ2ρ2,λ2,0+;ω2(fg)(t).

    where the coefficents σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. As

    ((f(η)g(ξ)f(ξ)g(η))20

    we have

    f2(η)g2(ξ)+f2(ξ)g2(η)2f(η)g(η)g(ξ)f(ξ). (3.5)

    Then by multiplying both sides of (3.5) by (tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2] and following the similar steps in Theorem 3.5, we get the desired result.

    Corollary 3.8. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.7, we obtain the following inequality

    Jσρ,λ,0+;ω(f2)(t)Jσρ,λ,0+;ω(g2)(t)[Jσρ,λ,0+;ω(fg)(t)]2

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Lemma 3.9. Let f:RR, and define

    ¯f(x)=x0f(t)dt,

    then for all t,ρ>0, λ>1 and wR, we have

    Jσρ,λ1,0+;ω(¯f)(t)=Jσρ,λ,0+;ω(f)(t)

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Proof.

    Jσρ,λ,0+;ω(¯f)(t)=t0(tτ)λ1Fσρ,λ[ω(xτ)ρ](τ0f(u)du)dτ=t0f(u)tu(tu)λ1Fσρ,λ[ω(tu)ρ]dτdu=t0(tτ)λFσρ,λ+1[ω(xt)ρ]f(u)du=Jσρ,λ+1,0+;ω(f)(t).

    Theorem 3.10. Let f and g be two functions on [0,), Then for all t,ρ>0, λ1,λ2>1 and w1,w2R, we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ11,0+;ω1(¯fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ21,0+;ω2(¯fg)(t)Jσ1ρ1,λ11,0+;ω1(¯f)(t)Jσ2ρ2,λ21,0+;ω2(¯g)(t)+Jσ1ρ1,λ11,0+;ω1(¯g)(t)Jσ2ρ2,λ21,0+;ω2(¯f)(t),

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. From Lemma 3.9 and inequality (2.7), we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ11,0+;ω1(¯fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ21,0+;ω2(¯fg)(t)=tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fg)(t)Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)+Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(f)(t)=Jσ1ρ1,λ11,0+;ω1(¯f)(t)Jσ2ρ2,λ21,0+;ω2(¯g)(t)+Jσ1ρ1,λ11,0+;ω1(¯g)(t)Jσ2ρ2,λ21,0+;ω2(¯f)(t)

    which completes the proof.

    Corollary 3.11. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.10, we obtain the following inequality

    tλFσρ,λ+1[ωtρ]Jσρ,λ1,0+;ω(¯fg)(t)Jσρ,λ1,0+;ω(¯f)(t)Jσρ,λ1,0+;ω(¯g)(t)

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Theorem 3.12. Let f and g be two differentiable function on [0,). Then for all t,ρ>0, λ1,λ2>0 and w1,w2R, we have

    |tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fg)(t)Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(f)(t)|fgtλ1+λ2+2Fσ1ρ1,λ1+1[ω1tρ1]Fσ2ρ2,λ2+1[ω2tρ2],

    where

    f=supx[0,)|f(x)|<,

    and the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. With basic calculation, we have

    tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fg)(t)Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(f)(t)=t0t0(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2](f(η)f(ξ))(g(η)g(ξ))dηdξ.

    Then taking modulus of the above equality, we find that

    |tλ2Fσ2ρ2,λ2+1[ω2tρ2]Jσ1ρ1,λ1,0+;ω1(fg)(t)+tλ1Fσ1ρ1,λ1+1[ω2tρ1]Jσ2ρ2,λ2,0+;ω2(fg)(t)Jσ1ρ1,λ1,0+;ω1(f)(t)Jσ2ρ2,λ2,0+;ω2(g)(t)Jσ1ρ1,λ1,0+;ω1(g)(t)Jσ2ρ2,λ2,0+;ω2(f)(t)|=|t0t0(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2](f(η)f(ξ))(g(η)g(ξ))dηdξ|=|t0t0(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2](ηξf(u)du)(ηξg(v)dv)dηdξ|fg|t0t0(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2](ηξ)2dηdξ|fgt2Fσ1ρ1,λ1+1[ω1tρ1]Fσ2ρ2,λ2+1[ω2tρ2]

    which completes the proof.

    Corollary 3.13. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.12, we obtain the following inequality

    |tλFσρ,λ+1[ωtρ]Jσρ,λ,0+;ω(fg)(t)Jσρ,λ,0+;ω(f)(t)Jσρ,λ,0+;ω(g)(t)|12fgt2λ+2[Fσρ,λ+1[ωtρ]]2

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Remark 3.14. If we choose λ1=α, λ2=β, σ1(0)=σ2(0)=1, and w1=w2=0, in Theorem 3.1, Theorem 3.4, Theorem 3.5, Theorem 3.7, Theorem 3.10 and Theorem 3.12, then the inequalities reduces to Theorem 2.1, Theorem 2.2, Theorem 2.3, Theorem 2.4, Theorem 2.6 and Theorem 2.7 proved by Sulaiman in [18], respectively.

    Theorem 3.15. Let f and g be two synchronous functions on [0,), that is they are having the same sense of variation on [0,), and let v1, v2:[0,)[0,). Then for all t,ρ>0, λ1,λ2>0 and w1,w2R, we have

    Jσ2ρ2,λ2,0+;ω2(v2)(t)Jσ1ρ1,λ1,0+;ω1(v1fg)(t)+Jσ2ρ2,λ2,0+;ω2(v2fg)(t)Jσ1ρ1,λ1,0+;ω1(v1)(t)Jσ2ρ2,λ2,0+;ω2(v2g)(t)Jσ1ρ1,λ1,0+;ω1(v1f)(t)+Jσ2ρ2,λ2,0+;ω2(v2f)(t)Jσ1ρ1,λ1,0+;ω1(v1g)(t), (3.6)

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. As f and g be two synchronous functions on [0,), then for all η,ξ0 we have

    (f(η)f(ξ))(g(η)g(ξ))0.

    Therefore

    f(η)g(η)+f(ξ)g(ξ)f(η)g(ξ)+f(ξ)g(η). (3.7)

    Mutlipying both sides of (3.7) by (tη)λ11Fσ1ρ1,λ1[ω1(tη)ρ1]v1(η), η(0,t), we find that

    (tη)λ11Fσ1ρ1,λ1[ω1(tη)ρ1]v1(η)f(η)g(η)+(tη)λ11Fσ1ρ1,λ1[ω1(tη)ρ1]v1(η)f(ξ)g(ξ)(tη)λ11Fσ1ρ1,λ1[ω1(tη)ρ1]v1(η)f(η)g(ξ)+(tη)λ11Fσ1ρ1,λ1[ω1(tη)ρ1]v1(η)f(ξ)g(η). (3.8)

    Integrating (3.7) with repect to η over (0,t), we get

    Jσ1ρ1,λ1,0+;ω1(v1fg)(t)+f(ξ)g(ξ)Jσ1ρ1,λ1,0+;ω1(v1)(t)g(ξ)Jσ1ρ1,λ1,0+;ω1(v1f)(t)+f(ξ)Jσ1ρ1,λ1,0+;ω1(v1g)(t). (3.9)

    Now, similarly, by multiplying both sides of (3.9) by (tξ)λ21Fσ2ρ2,λ2[ω2(tξ)ρ2]v2(ξ), ξ(0,t) and integrating with respect to ξ over (0,t), we get the desired result.

    Corollary 3.16. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.15, we obtain the following inequality

    Jσρ,λ,0+;ω(v2)(t)Jσρ,λ,0+;ω(v1fg)(t)+Jσρ,λ,0+;ω(v2fg)(t)Jσρ,λ,0+;ω(v1)(t)Jσρ,λ,0+;ω(v2g)(t)Jσρ,λ,0+;ω(v1f)(t)+Jσρ,λ,0+;ω(v2f)(t)Jσρ,λ,0+;ω(v1g)(t),

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Remark 3.17. If we choose v1=v2=1 in Theorem 3.15, the inequality (3.14) reduce to inequality (2.7).

    Theorem 3.18. Let f and g be two synchronous functions on [0,), that is they are having the same sense of variation on [0,), and let p,q,r:[0,)[0,). Then for all t,ρ>0, λ1,λ2>0 and w1,w2R, we have

    Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(q)(t)Jσ1ρ1,λ1,0+;ω1(pfg)(t)+2Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(qfg)(t)Jσ1ρ1,λ1,0+;ω1(p)(t)+Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(q)(t)Jσ1ρ1,λ1,0+;ω1(rfg)(t)+Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(r)(t)Jσ1ρ1,λ1,0+;ω1(pfg)(t)+Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(rfg)(t)Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(qg)(t)Jσ1ρ1,λ1,0+;ω1(pf)(t)+Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(qf)(t)Jσ1ρ1,λ1,0+;ω1(pg)(t)+Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(rg)(t)Jσ1ρ1,λ1,0+;ω1(pf)(t)+Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(rf)(t)Jσ1ρ1,λ1,0+;ω1(pg)(t)+Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(qg)(t)Jσ1ρ1,λ1,0+;ω1(rf)(t)+Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(qf)(t)Jσ1ρ1,λ1,0+;ω1(rg)(t),

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. If we choose v1=p and v2=q in Theorem 3.15, we can write:

    Jσ2ρ2,λ2,0+;ω2(q)(t)Jσ1ρ1,λ1,0+;ω1(pfg)(t)+Jσ2ρ2,λ2,0+;ω2(qfg)(t)Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(qg)(t)Jσ1ρ1,λ1,0+;ω1(pf)(t)+Jσ2ρ2,λ2,0+;ω2(qf)(t)Jσ1ρ1,λ1,0+;ω1(pg)(t). (3.10)

    Multiplying both sides of (3.10) by Jσ1ρ1,λ1,0+;ω1(r)(t), we get

    Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(q)(t)Jσ1ρ1,λ1,0+;ω1(pfg)(t)+Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(qfg)(t)Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(qg)(t)Jσ1ρ1,λ1,0+;ω1(pf)(t)+Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ2ρ2,λ2,0+;ω2(qf)(t)Jσ1ρ1,λ1,0+;ω1(pg)(t). (3.11)

    If we choose v1=r and v2=q in Theorem 3.15 and multiplying by Jσ1ρ1,λ1,0+;ω1(p)(t), then we find that

    Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(q)(t)Jσ1ρ1,λ1,0+;ω1(rfg)(t)+Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(qfg)(t)Jσ1ρ1,λ1,0+;ω1(r)(t)Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(qg)(t)Jσ1ρ1,λ1,0+;ω1(rf)(t)+Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ2ρ2,λ2,0+;ω2(qf)(t)Jσ1ρ1,λ1,0+;ω1(rg)(t). (3.12)

    Similarly, if we choose v1=p and v2=r in Theorem 3.15 and multiplying by Jσ1ρ1,λ1,0+;ω1(q)(t), then we find that

    Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(r)(t)Jσ1ρ1,λ1,0+;ω1(pfg)(t)+Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(rfg)(t)Jσ1ρ1,λ1,0+;ω1(p)(t)Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(rg)(t)Jσ1ρ1,λ1,0+;ω1(pf)(t)+Jσ1ρ1,λ1,0+;ω1(q)(t)Jσ2ρ2,λ2,0+;ω2(rf)(t)Jσ1ρ1,λ1,0+;ω1(pg)(t). (3.13)

    Then by adding the inequalities of (3.11)-(3.13), the desired inequality has been obtained.

    Corollary 3.19. Choosing λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ and w1=w2=w in Theorem 3.18, we obtain the following inequality

    2Jσρ,λ,0+;ω(r)(t)Jσρ,λ,0+;ω(q)(t)Jσρ,λ,0+;ω(pfg)(t)+2Jσρ,λ,0+;ω(r)(t)Jσρ,λ,0+;ω(p)(t)Jσρ,λ,0+;ω(qfg)(t)+2Jσρ,λ,0+;ω(p)(t)Jσρ,λ,0+;ω(q)(t)Jσρ,λ,0+;ω(rfg)(t)Jσρ,λ,0+;ω(r)(t)[Jσρ,λ,0+;ω(qg)(t)Jσρ,λ,0+;ω(pf)(t)+Jσρ,λ,0+;ω(qf)(t)Jσρ,λ,0+;ω(pg)(t)]+Jσρ,λ,0+;ω(q)(t)[Jσρ,λ,0+;ω(rg)(t)Jσρ,λ,0+;ω(pf)(t)+Jσρ,λ,0+;ω(rf)(t)Jσρ,λ,0+;ω(pg)(t)]+Jσρ,λ,0+;ω(p)(t)[Jσρ,λ,0+;ω(qg)(t)Jσρ,λ,0+;ω(rf)(t)+Jσρ,λ,0+;ω(qf)(t)Jσρ,λ,0+;ω(rg)(t)]

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Remark 3.20. If we choose λ1=α, λ2=β, σ1(0)=σ2(0)=1, and w1=w2=0, in Theorem 3.15 and Theorem 3.18 then the inequalities reduces to Lemma 3 and Theorem 4 proved by Dahmani in [5], respectively.

    Theorem 3.21. Let v1 and v2 be two positive functions on [0,) and let f and g be two differentiable functions on [0,).If fLp([0,)), gLq([0,)), p>1, 1p+1q=1, then for all t>0 and ρ1,ρ2,λ1,λ2>0 and w1,w2R, we have

    T(f,g;v1,v2)tfpgqJσ1ρ1,λ1,0+;ω1(v1)(t)Jσ2ρ2,λ2,0+;ω2(v2)(t),

    where

    T(f,g;v1,v2):=Jσ2ρ2,λ2,0+;ω2(v2)(t)Jσ1ρ1,λ1,0+;ω1(v1fg)(t)+Jσ2ρ2,λ2,0+;ω2(v2fg)(t)Jσ1ρ1,λ1,0+;ω1(v1)(t)Jσ2ρ2,λ2,0+;ω2(v2g)(t)Jσ1ρ1,λ1,0+;ω1(v1f)(t)Jσ2ρ2,λ2,0+;ω2(v2f)(t)Jσ1ρ1,λ1,0+;ω1(v1g)(t)

    and the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Proof. Following the similar steps of proof of Theorem 8, we can write

    T(f,g;v1,v2):=t0t0H(η,ξ)(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ)dηdξ (3.14)

    where

    H(η,ξ)=(f(η)f(ξ))(g(η)g(ξ))=ηξηξf(x)g(y)dxdy.

    Using the well-known Hölder inequality for double integral, we find that

    |H(η,ξ)||ηξηξ|f(x)|pdxdy|1p|ηξηξ|g(y)|qdxdy|1q=|ηξ||ηξ|f(x)|pdx|1p|ηξ|g(y)|qdy|1q. (3.15)

    Substituting (3.15) into (3.14), we have

    |T(f,g;v1,v2)|t0t0|ηξ|(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ)×|ηξ|f(x)|pdx|1p|ηξ|g(y)|qdy|1qdηdξ. (3.16)

    Appying again Hölder inequality to the right hand side of (3.16), we find that

    |T(f,g;v1,v2)|(t0t0|ηξ|(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ)|ηξ|f(x)|pdx|dηdξ)1p×(t0t0|ηξ|(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ)|ηξ|g(x)|qdx|dηdξ)1qfpgq×(t0t0|ηξ|(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ)dηdξ)1p×(t0t0|ηξ|(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ))1q.

    Now using the fact that |ηξ|t and 1p+1q=1, we have

    |T(f,g;v1,v2)|tfpgq(t0t0(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ)dηdξ)1p×(t0t0(tη)λ11(tξ)λ21Fσ1ρ1,λ1[ω1(tη)ρ1]Fσ2ρ2,λ2[ω2(tξ)ρ2]v1(η)v2(ξ))1q=tfpgq[Jσ1ρ1,λ1,0+;ω1(v1)(t)]1p[Jσ2ρ2,λ2,0+;ω2(v2)(t)]1p[Jσ1ρ1,λ1,0+;ω1(v1)(t)]1q[Jσ2ρ2,λ2,0+;ω2(v2)(t)]1q=tfpgqJσ1ρ1,λ1,0+;ω1(v1)(t)Jσ2ρ2,λ2,0+;ω2(v2)(t).

    Thus the proof is completed.

    Corollary 3.22. If we choose λ1=λ2=λ, σ1=σ2=σ, ρ1=ρ2=ρ, w1=w2=w and v1=v2=v in Theorem 3.21, we have the following inequality

    T(f,g;v,v)tfpgq[Jσρ,λ,0+;ω(v)(t)]2

    where the coefficients σ(k) (kN0=N{0}) is a bounded sequence of positive real numbers.

    Remark 3.23. In particular, putting λ1=λ2=α, σ1(0)=σ2(0)=1, and w1=w2=0, then Corollary 3.22 reduce to Theorem 3.1 proved by Dahmani et. al in [6].

    Corollary 3.24. If we choose v1=v2=v in Theorem 3.21, we have the following inequality

    T(f,g;v,v)tfpgqJσ1ρ1,λ1,0+;ω1(v)(t)Jσ2ρ2,λ2,0+;ω2(v)(t)

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Remark 3.25. In particular, putting λ1=α, λ2=β, σ1(0)=σ2(0)=1, and w1=w2=0, then Corollary 3.24 reduce to Theorem 3.2 proved by Dahmani et. al in [6].

    Corollary 3.26. If we choose v1=v2=1 in Theorem 3.21, we have the following inequality

    T(f,g)tλ1+λ2+1Fσ1ρ1,λ1+1[ω1tρ1]Fσ2ρ2,λ2+1[ω2tρ2]fpgq.

    where the coefficients σ1(k),σ2(k) (kN0=N{0}) are bounded sequences of positive real numbers.

    Remark 3.27. In particular, putting λ1=α, λ2=β, σ1(0)=σ2(0)=1, and w1=w2=0, then Corollary 3.26 reduce to Corollary 3.4 given by Dahmani et. al in [6].

    We have introduced a general version of Chebyshev type integral inequality for the generalised fractional integral operators based on two synchronous functions. The established results are generalization of some existing Chebychev type integral inequalities in the previous published studies. For further investigations we propose to consider the Chebyshev type inequalities for other fractional integral operators.

    All authors declare no conflicts of interest in this paper.



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