Research article

Ostrowski type inequalities via the Katugampola fractional integrals

  • Received: 15 July 2019 Accepted: 26 September 2019 Published: 17 October 2019
  • MSC : 26A33, 26D10, 26D15

  • The main aim of this study is to reveal new generalized-Ostrowski-type inequalities using Katugampola fractional integral operator which generalizes Riemann-Liouville and Hadamard fractional integral operators into a single form. For this purpose, at first, a new fractional integral identity is generated by the researchers. Then, by using this identity, some inequalities for the class of functions whose certain powers of absolute values of derivatives are pconvex are derived. Some applications to special means for positive real numbers are also given. It is observed that the obtained inequalities are generalizations of some well known results.

    Citation: Mustafa Gürbüz, Yakup Taşdan, Erhan Set. Ostrowski type inequalities via the Katugampola fractional integrals[J]. AIMS Mathematics, 2020, 5(1): 42-53. doi: 10.3934/math.2020004

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  • The main aim of this study is to reveal new generalized-Ostrowski-type inequalities using Katugampola fractional integral operator which generalizes Riemann-Liouville and Hadamard fractional integral operators into a single form. For this purpose, at first, a new fractional integral identity is generated by the researchers. Then, by using this identity, some inequalities for the class of functions whose certain powers of absolute values of derivatives are pconvex are derived. Some applications to special means for positive real numbers are also given. It is observed that the obtained inequalities are generalizations of some well known results.


    Fractional calculus was first suggested for consideration by Leibnitz in his letter to L'Hospital which dealt with derivatives of order α=12 (see [10]). Hereupon, this theory has been used in many fields of science such as economics, biology, engineering, physics and mathematics for sure. Many types of fractional derivatives and integrals were studied by Hadamard, Caputo, Riemann-Liouville, Grünwald-Letnikov, etc. Various properties of these operators have been summarized in [9]. For the last decades, this theory has been used in inequality theory frequently because it enables scientists to obtain integral inequalities for also non-integer orders. One of the most famous inequality is Ostrowski's which has lead to gain many practical inequalities with fractional calculus as well.

    Ostrowski proved an important integral inequality in 1938 which gives an upper bound for difference between the value f(x) and mean value of  f for functions whose derivatives' absolute values are bounded, which can be seen in [11] as the following.

    Theorem 1. Let f:IRR be a differentiable mapping on I and a,bI with a<b. If |f(x)|M then,

    |f(x)1babaf(t)dt|M(ba)[14+(xa+b2)2(ba)2]

    holds for all x[a,b]. Here 14 is the best possible constant.

    Zhang and Wan introduced pconvex functions in [14], and İşcan gave a different version of this definition in [5] as follows.

    Definition 1. Let I(0,) be a real interval and pR{0}. A function f:IR is said to be a pconvex function, if

    f([txp+(1t)yp]1p)tf(x)+(1t)f(y) (1.1)

    for all x,y I and t[0,1].

    It is easy to see that pconvexity reduces to ordinary convexity for p=1 and harmonically convexity for p=1.

    pconvex functions are frequently considered in the inequalities especially when using fractional integral calculations. Some fractional integral operators are used to do these calculations. Therefore, some new definitions about fractional calculus are given. First of them is Riemann-Liouville fractional integration operator (see [9]) which ables to integrate functions on fractional orders.

    Definition 2. Let fL1[a,b]. The Riemann-Liouville integrals Jαa+f and Jαbf of order α>0 with a0 are defined by

    Jαa+f=1Γ(α)xa(xt)α1f(t)dt,   x>a

    and

    Jαbf=1Γ(α)bx(tx)α1f(t)dt,   x<b

    respectively where Γ(α)=0etuα1du. Here J0a+f(x)=J0bf(x)=f(x).

    Definition 3. [9] The left and right-side Hadamard fractional integrals of order αR+ are defined as

    αa+φ=1Γ(α)xaφ(t)(lnxt)1αdtt,   x>a>0αbφ=1Γ(α)bxφ(t)(lntx)1αdtt,   0<x<b.

    where Γ is the gamma function.

    Definition 4. [8] Let the space Xpc(a,b) (cR, 1p) of those complex-valued Lebesque measurable functions f on [a,b] for which fxpc<, where the norm is defined by

    fxpc=(ba|tcf(t)|pdtt)1p< (1.2)

    for 1p, cR and for the case p=,

    fxpc=esssupatb[tc|f(t)|]        (cR). (1.3)

    Katugampola revealed a new fractional integration operator which generalizes both Riemann-Liouville and Hadamard fractional integration operators. This integration operator also holds semigroup property (see [6,7]) and is defined as the following statement.

    Definition 5. Let [a,b]R be a finite interval. Then, the left and right-side Katugampola fractional integrals of order (α>0) of fXpc(a,b) are defined by

    ρIαa+f(x)=ρ1αΓ(α)xatρ1(xρtρ)1αf(t)dt

    and

    ρIαbf(x)=ρ1αΓ(α)bxtρ1(tρxρ)1αf(t)dt

    with a<x<b and ρ>0 if the integral exists.

    Theorem 2. [7] Let α>0 and ρ>0. Then for x>a,

    1.limρ1ρIαa+f(x)=Jαa+f(x)2.limρ0+ρIαa+f(x)=αa+f(x).

    Similar results also hold for right-sided operators.

    Erdélyi et al. deeply involved in hypergeometric functions which Whittaker discovered in 1904 and gave the definition of it in [4] as:

    2F1(a,b;c;z)=1β(b,bc)10tb1(1t)cb1(1zt)adt, c>b>0, |z|<1 (1.4)

    Throughout the paper the notation Yf(α,ρ;a,x,b) will be used in the meaning of following statement.

    Yf(α,ρ;a,x,b)=ρf(x)ba[(xρaρ)α+(bρxρ)α]ρα+1Γ(α+1)ba[ ρIαxf(a)+ ρIαx+f(b)]. (1.5)

    where Γ is Euler Gamma function, i.e., Γ(α)=0etuα1du.

    Alomari et al. proved the following lemma in 2010 in [2] to obtain new Ostrowski-type results.

    Lemma 1. Let f:IRR be a differentiable mapping on I where a,bI with a<b. If fL[a,b], then the following equality holds

    f(x)1babaf(t)dt=(xa)2ba10tf(tx+(1t)a)dt(bx)2ba10tf(tx+(1t)b)dt (1.6)

    for each x[a,b].

    Set proved the next lemma in 2012 which helps to obtain Ostrowski-type inequalities for Riemann-Liouville fractional integrals in [13].

    Lemma 2. Let f:[a,b]R, be a differentiable mapping on (a,b) with a<b. If fL[a,b], then for all x[a,b] and α>0 the following identity holds

    f(x)ba[(xa)α+(bx)α]Γ(α+1)ba[Jαxf(a)+Jαx+f(b)]=(xa)α+1ba10tαf(tx+(1t)a)dt(bx)α+1ba10tαf(tx+(1t)b)dt (1.7)

    where Γ is Euler Gamma function.

    To see more studies involving Ostrowski-type inequalities, one can see references [1,3,12]. Also in [2] and [5], Ostrowski-type inequalities using integer order integrals and in [13], Ostrowski-type inequalities using Riemann-Liouville integral operator were obtained. On the other hand, the findings in this study were obtained using Katugampola fractional integration operator, which gives more general results than inequalities using integer order integral or Riemann-Liouville fractional integral operator.

    In this paper, a new lemma including Katugampola fractional integral has been proved inspired by Lemma 2. Then with the help of some properties and inequalities like Hölder and power mean, new Ostrowski-type inequalities are proved. It is seen that results are supported by the literature.

    Lemma 3. Let f:I(0,)R be a differentiable mapping on I where a,bI with a<b. If fL[a,b], then for all x[a,b] the following identity holds

    Yf(α,ρ;a,x,b)=(xρaρ)α+1ba10tαf([txρ+(1t)aρ]1ρ)(txρ+(1t)aρ)11ρdt(bρxρ)α+1ba10tαf([txρ+(1t)bρ]1ρ)(txρ+(1t)bρ)11ρdt (2.1)

    where α>0, ρ>0.

    Proof. By integrating by parts, the following statement is obtained

    I1=10tαf([txρ+(1t)aρ]1ρ)(txρ+(1t)aρ)11ρdt=ρf(x)xρaραρxρaρ10tα1f([txρ+(1t)aρ]1ρ)dt.

    With changing the variable u=[txρ+(1t)aρ]1ρ, it is easy to get

    I1=ρf(x)xρaραρxρaρxa(uρaρxρaρ)α1ρuρ1xρaρf(u)du=ρf(x)xρaραρ2(xρaρ)α+1xauρ1(uρaρ)1αf(u)du=ρf(x)xρaραρ2Γ(α)(xρaρ)α+1ρ1αρIαxf(a)=ρf(x)xρaρρα+1Γ(α+1)(xρaρ)α+1ρIαxf(a). (2.2)

    In the same way, integrating by parts I2 can be revealed as

    I2=10tαf([txρ+(1t)bρ]1ρ)(txρ+(1t)bρ)11ρdt=ρf(x)xρbραρxρbρ10tα1f([txρ+(1t)bρ]1ρ)dt.

    With same change of variable, it can be seen that

    I2=ρf(x)xρbραρxρbρxb(uρbρxρbρ)α1ρuρ1xρbρf(u)du=ρf(x)bρxρ+αρ2(bρxρ)α+1bxuρ1(bρuρ)1αf(u)du=ρf(x)bρxρ+αρ2Γ(α)(bρxρ)α+1ρ1αρIαx+f(b)=ρf(x)bρxρ+ρα+1Γ(α+1)(bρxρ)α+1ρIαx+f(b). (2.3)

    Multiplying (2.2) with (xρaρ)α+1ba and (2.3) with ((bρxρ)α+1ba) and summing them side by side, the following calculations can be performed.

    (xρaρ)α+1ba10tαf([txρ+(1t)aρ]1ρ)(txρ+(1t)aρ)11ρdt(bρxρ)α+1ba10tαf([txρ+(1t)bρ]1ρ)(txρ+(1t)bρ)11ρdt=ρf(x)(xρaρ)αbaρα+1Γ(α+1)ρIαxf(a)ba+ρf(x)(bρxρ)αbaρα+1Γ(α+1)ρIαx+f(b)ba.

    With rearranging the last statement

    ρf(x)ba[(xρaρ)α+(bρxρ)α]ρα+1Γ(α+1)ba[ρIαxf(a)+ρIαx+f(b)]=(xρaρ)α+1ba10tαf([txρ+(1t)aρ]1ρ)(txρ+(1t)aρ)11ρdt(bρxρ)α+1ba10tαf([txρ+(1t)bρ]1ρ)(txρ+(1t)bρ)11ρdt

    is obtained, which completes the proof.

    Remark 1. Under necessary conditions of Lemma 3 with choosing ρ=1, we get Lemma 2 which is proven in [13].

    Remark 2. By choosing α=1 in Remark 1, it is easy to obtain Lemma 1 which is proven in [2].

    Theorem 3. Let f:I(0,)R be a differentiable mapping on I and a,bI with a<b such that fL[a,b]. If |f| is pconvex on I and |f(x)|M for all x[a,21ρa) (if 21ρa<b, otherwise x[a,b]), then the following inequality holds

    |Yf(α,ρ;a,x,b)|M(xρaρ)α+1ba {R(a)+S(a)}+M(bρxρ)α+1ba{R(b)+S(b)} (2.4)

    where

    R(λ)=λ1ρα+22F1(α+2,ρ1ρ;α+3;1xρλρ)S(λ)=λ1ρ(α+1)(α+2)[(α+2)2F1(α+1,ρ1ρ;α+2;1xρλρ)(α+1)2F1(α+2,ρ1ρ;α+3;1xρλρ)]

    and ρ>1, α>0, λ{a,b}, 2F1(.,.;.;.) is hypergeometric function and Yf(α,ρ;a,x,b) is as defined in (1.4).

    Proof. By using Lemma 3 and properties of modulus, it can be written

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba10tα|f([txρ+(1t)aρ]1ρ)|(txρ+(1t)aρ)11ρdt+(bρxρ)α+1ba10tα|f([txρ+(1t)bρ]1ρ)|(txρ+(1t)bρ)11ρdt.

    By means of pconvexity of |f|, following computations can be performed

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba10tα[t|f(x)|+(1t)|f(a)|](txρ+(1t)aρ)11ρdt+(bρxρ)α+1ba10tα[t|f(x)|+(1t)|f(b)|](txρ+(1t)bρ)11ρdt=(xρaρ)α+1ba×{|f(x)|10tα+1(txρ+(1t)aρ)1ρ1dt+|f(a)|10(tαtα+1)(txρ+(1t)aρ)1ρ1dt}+(bρxρ)α+1ba×{|f(x)|10tα+1(txρ+(1t)bρ)1ρ1dt+|f(b)|10(tαtα+1)(txρ+(1t)bρ)1ρ1dt}.

    With necessary computations, it is easy to see that

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba {|f(x)|R(a)+|f(a)|S(a)}+(bρxρ)α+1ba{|f(x)|R(b)+|f(b)|S(b)}.

    By using boundedness of f(x), that is, |f(x)|M, it is easy to see

    |Yf(α,ρ;a,x,b)|M(xρaρ)α+1ba {R(a)+S(a)}+M(bρxρ)α+1ba{R(b)+S(b)}

    which completes the proof.

    Remark 3. By choosing ρ=1 in Theorem 2.1, it reduces to Theorem 7 with s=1 in [13] where we used the fact that 2F1(x, 0; y; z)=1.

    Theorem 4. Let f:I(0,)R be a differentiable mapping on I and a,bI with a<b such that fL[a,b]. If |f|q is pconvex on I and |f(x)|M for all xI{a,b}, then the following inequality holds

    |Yf(α,ρ;a,x,b)|Mba(1αq+1)1q[(xρaρ)α+1K1r(a)+(bρxρ)α+1K1r(b)]

    where

    K(λ)=ρ(xr(1ρ)+ρλr(1ρ)+ρ)(xρλρ)(r(1ρ)+ρ)

    and ρ>0, α>0, λ{a,b}, r>1,1r+1q=1, rρρ1 and Yf(α,ρ;a,x,b) is as defined in (1.4).

    Proof. With the help of Lemma 3 and properties of modulus, one can write

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba10tα|f([txρ+(1t)aρ]1ρ)|(txρ+(1t)aρ)11ρdt+(bρxρ)α+1ba10tα|f([txρ+(1t)bρ]1ρ)|(txρ+(1t)bρ)11ρdt.

    By using Hölder inequality, it can be written as

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba(10((txρ+(1t)aρ)1ρ1)rdt)1r×(10tαq|f([txρ+(1t)aρ]1ρ)|qdt)1q+(bρxρ)α+1ba(10((txρ+(1t)bρ)1ρ1)rdt)1r×(10tαq|f([txρ+(1t)bρ]1ρ)|qdt)1q.

    From the pconvexity of |f|q and |f(x)|M, it follows that

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1baK1r(a)×(10tαq+1|f(x)|qdt+10tαq(1t)|f(a)|qdt)1q+(bρxρ)α+1baK1r(b)×(10tαq+1|f(x)|qdt+10tαq(1t)|f(b)|qdt)1q(xρaρ)α+1baK1r(a)(Mq1αq+2+Mq1(αq+1)(αq+2))1q+(bρxρ)α+1baK1r(b)(Mq1αq+2+Mq1(αq+1)(αq+2))1q=Mba(1αq+1)1q[(xρaρ)α+1K1r(a)+(bρxρ)α+1K1r(b)]

    which completes the proof.

    Theorem 5. Let f:I(0,)R be a differentiable mapping on I and a,bI with a<b such that fL[a,b]. If |f|q is pconvex on I and |f(x)|M for all x[a,21ρa) (if 21ρa<b, otherwise x[a,b]), then the following inequality holds

    |Yf(α,ρ;a,x,b)|Mba(xρaρ)α+1L11q(a)(R(a)+S(a))1q+Mba(bρxρ)α+1L11q(b)(R(b)+S(b))1q

    where

    R(λ)=λ1ρα+2 2F1(α+2, ρ1ρ; α+3; 1xρλρ)S(λ)=λ1ρ(α+1)(α+2)[(α+2) 2F1(α+1, ρ1ρ; α+2; 1xρλρ)(α+1) 2F1(α+2, ρ1ρ; α+3; 1xρλρ) ]L(λ)=λ1ρ α+1 2F1(α+1,ρ1ρ;α+2;1xρλρ)

    and ρ>1, α>0, q>1, λ{a,b}, 2F1(.,.;.;.) is hypergeometric function and Yf(α,ρ;a,x,b) is as defined in (1.4).

    Proof. Making use of Lemma 3 and properties of absolute value, it can be seen that

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba10tα|f([txρ+(1t)aρ]1ρ)|(txρ+(1t)aρ)11ρdt + (bρxρ)α+1ba10tα|f([txρ+(1t)bρ]1ρ)|(txρ+(1t)bρ)11ρdt.

    Then, making use of Power-Mean inequality, the following computations can be performed

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1ba(10tα(txρ+(1t)aρ)1ρ1dt)11q×(10tα(txρ+(1t)aρ)1ρ1|f([txρ+(1t)aρ]1ρ)|qdt)1q+(bρxρ)α+1ba(10tα(txρ+(1t)bρ)1ρ1dt)11q×(10tα(txρ+(1t)bρ)1ρ1|f([txρ+(1t)bρ]1ρ)|qdt)1q.

    Hence |f|q is chosen as pconvex on I

    |Yf(α,ρ;a,x,b)|(xρaρ)α+1L11q(a)ba×(10tα+1(txρ+(1t)aρ)1ρ1|f(x)|qdt + 10(tαtα+1)(txρ+(1t)aρ)1ρ1|f(a)|qdt )1q+(bρxρ)α+1L11q(b)ba×(10tα+1(txρ+(1t)bρ)1ρ1|f(x)|qdt + 10(tαtα+1)(txρ+(1t)bρ)1ρ1|f(b)|qdt )1q.

    With necessary computations, it can be easily seen that

    |Yf(α,ρ;a,x,b)|=(xρaρ)α+1L11q(a)ba(|f(x)|qR(a)+|f(a)|qS(a))1q + (bρxρ)α+1L11q(b)ba(|f(x)|qR(b)+|f(b)|qS(b))1q

    With using boundedness of |f(x)|, it can be written that

    |Yf(α,ρ;a,x,b)|M(xρaρ)α+1L11q(a)ba(R(a)+S(a))1q + M(bρxρ)α+1L11q(b)ba(R(b)+S(b))1q.

    So the proof is completed.

    Remark 4. By choosing ρ=1 in Theorem 2.3, it reduces to Theorem 9 with s=1 in [13] where we used the fact that 2F1(x, 0; y; z)=1.

    Let us recall the following means for two positive real numbers.

    (1) The arithmetic mean:

    A=A(a,b)=a+b2; a,b>0; a,bR,

    (2) The logarithmic mean:

    L=L(a,b)=balnblna; a,b>0; a,bR.

    Proposition 1. Let 0<a<b and a+b2<21ρa. Then the following inequality holds

    |4A(a,b)ln(A(a,b))2b(b2)a(a2)baL1(a(a2),b(b2))+2A(a,b)||M|(b2a2)2

    where M=max{|lna|,|lnb|}.

    Proof. The proof follows from Theorem 2.1 on applying α=1, ρ=2, x=a+b2 and f(x)=lnx which is pconvex on (0,) for p1.

    Proposition 2. Let 0<a<b and a+b2<21ρa. Then the following inequality holds

    |4A1(a,b)4L1(a,b)|b2a22a2.

    Proof. The proof is immediate from Theorem 2.1 on applying α=1, ρ=2, x=a+b2 and f(x)=x2 which is p convex on (0,).

    In this study, new lemma and theorems are put forward to obtain new upper bounds for Ostrowski-type inequalities including Katugampola fractional operator. Researchers can obtain new lemmas and theorems by using similar method used in this study or use the obtained results in many fields of science.

    This research received no external funding. The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, or in the decision to publish the results.

    The authors declare no conflict of interest in this paper.



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