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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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:I⊆R→R be a differentiable mapping on I∘ and a,b∈I with a<b. If |f′(x)|≤M then,
|f(x)−1b−a∫baf(t)dt|≤M(b−a)[14+(x−a+b2)2(b−a)2] |
holds for all x∈[a,b]. Here 14 is the best possible constant.
Zhang and Wan introduced p−convex 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 p∈R∖{0}. A function f:I→R is said to be a p−convex function, if
f([txp+(1−t)yp]1p)≤tf(x)+(1−t)f(y) | (1.1) |
for all x,y ∈ I and t∈[0,1].
It is easy to see that p−convexity reduces to ordinary convexity for p=1 and harmonically convexity for p=−1.
p−convex 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 f∈L1[a,b]. The Riemann-Liouville integrals Jαa+f and Jαb−f of order α>0 with a⩾0 are defined by
Jαa+f=1Γ(α)∫xa(x−t)α−1f(t)dt, x>a |
and
Jαb−f=1Γ(α)∫bx(t−x)α−1f(t)dt, x<b |
respectively where Γ(α)=∫∞0e−tuα−1du. Here J0a+f(x)=J0b−f(x)=f(x).
Definition 3. [9] The left and right-side Hadamard fractional integrals of order α∈R+ are defined as
ℑαa+φ=1Γ(α)∫xaφ(t)(lnxt)1−αdtt, x>a>0, ℑαb−φ=1Γ(α)∫bxφ(t)(lntx)1−αdtt, 0<x<b. |
where Γ is the gamma function.
Definition 4. [8] Let the space Xpc(a,b) (c∈R, 1≤p≤∞) of those complex-valued Lebesque measurable functions f on [a,b] for which ‖f‖xpc<∞, where the norm is defined by
‖f‖xpc=(∫ba|tcf(t)|pdtt)1p<∞ | (1.2) |
for 1≤p≤∞, c∈R and for the case p=∞,
‖f‖xpc=esssupa≤t≤b[tc|f(t)|] (c∈R). | (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 f∈Xpc(a,b) are defined by
ρIαa+f(x)=ρ1−αΓ(α)∫xatρ−1(xρ−tρ)1−αf(t)dt |
and
ρIαb−f(x)=ρ1−αΓ(α)∫bxtρ−1(tρ−xρ)1−αf(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.limρ→1ρIαa+f(x)=Jαa+f(x)2.limρ→0+ρIαa+f(x)=ℑαa+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,b−c)∫10tb−1(1−t)c−b−1(1−zt)−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)b−a[(xρ−aρ)α+(bρ−xρ)α]−ρα+1Γ(α+1)b−a[ ρIαx−f(a)+ ρIαx+f(b)]. | (1.5) |
where Γ is Euler Gamma function, i.e., Γ(α)=∫∞0e−tuα−1du.
Alomari et al. proved the following lemma in 2010 in [2] to obtain new Ostrowski-type results.
Lemma 1. Let f:I⊂R⟶R be a differentiable mapping on I∘ where a,b∈I with a<b. If f′∈L[a,b], then the following equality holds
f(x)−1b−a∫baf(t)dt=(x−a)2b−a∫10tf′(tx+(1−t)a)dt−(b−x)2b−a∫10tf′(tx+(1−t)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 f′∈L[a,b], then for all x∈[a,b] and α>0 the following identity holds
f(x)b−a[(x−a)α+(b−x)α]−Γ(α+1)b−a[Jαx−f(a)+Jαx+f(b)]=(x−a)α+1b−a∫10tαf′(tx+(1−t)a)dt−(b−x)α+1b−a∫10tαf′(tx+(1−t)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,b∈I with a<b. If f′∈L[a,b], then for all x∈[a,b] the following identity holds
Yf(α,ρ;a,x,b)=(xρ−aρ)α+1b−a∫10tαf′([txρ+(1−t)aρ]1ρ)(txρ+(1−t)aρ)1−1ρdt−(bρ−xρ)α+1b−a∫10tαf′([txρ+(1−t)bρ]1ρ)(txρ+(1−t)bρ)1−1ρdt | (2.1) |
where α>0, ρ>0.
Proof. By integrating by parts, the following statement is obtained
I1=∫10tαf′([txρ+(1−t)aρ]1ρ)(txρ+(1−t)aρ)1−1ρdt=ρf(x)xρ−aρ−αρxρ−aρ∫10tα−1f([txρ+(1−t)aρ]1ρ)dt. |
With changing the variable u=[txρ+(1−t)aρ]1ρ, it is easy to get
I1=ρf(x)xρ−aρ−αρxρ−aρ∫xa(uρ−aρxρ−aρ)α−1ρuρ−1xρ−aρf(u)du=ρf(x)xρ−aρ−αρ2(xρ−aρ)α+1∫xauρ−1(uρ−aρ)1−αf(u)du=ρf(x)xρ−aρ−αρ2Γ(α)(xρ−aρ)α+1ρ1−αρIαx−f(a)=ρf(x)xρ−aρ−ρα+1Γ(α+1)(xρ−aρ)α+1ρIαx−f(a). | (2.2) |
In the same way, integrating by parts I2 can be revealed as
I2=∫10tαf′([txρ+(1−t)bρ]1ρ)(txρ+(1−t)bρ)1−1ρdt=ρf(x)xρ−bρ−αρxρ−bρ∫10tα−1f([txρ+(1−t)bρ]1ρ)dt. |
With same change of variable, it can be seen that
I2=ρf(x)xρ−bρ−αρxρ−bρ∫xb(uρ−bρxρ−bρ)α−1ρuρ−1xρ−bρf(u)du=−ρf(x)bρ−xρ+αρ2(bρ−xρ)α+1∫bxuρ−1(bρ−uρ)1−αf(u)du=−ρf(x)bρ−xρ+αρ2Γ(α)(bρ−xρ)α+1ρ1−αρIαx+f(b)=−ρf(x)bρ−xρ+ρα+1Γ(α+1)(bρ−xρ)α+1ρIαx+f(b). | (2.3) |
Multiplying (2.2) with (xρ−aρ)α+1b−a and (2.3) with (−(bρ−xρ)α+1b−a) and summing them side by side, the following calculations can be performed.
(xρ−aρ)α+1b−a∫10tαf′([txρ+(1−t)aρ]1ρ)(txρ+(1−t)aρ)1−1ρdt−(bρ−xρ)α+1b−a∫10tαf′([txρ+(1−t)bρ]1ρ)(txρ+(1−t)bρ)1−1ρdt=ρf(x)(xρ−aρ)αb−a−ρα+1Γ(α+1)ρIαx−f(a)b−a+ρf(x)(bρ−xρ)αb−a−ρα+1Γ(α+1)ρIαx+f(b)b−a. |
With rearranging the last statement
ρf(x)b−a[(xρ−aρ)α+(bρ−xρ)α]−ρα+1Γ(α+1)b−a[ρIαx−f(a)+ρIαx+f(b)]=(xρ−aρ)α+1b−a∫10tαf′([txρ+(1−t)aρ]1ρ)(txρ+(1−t)aρ)1−1ρdt−(bρ−xρ)α+1b−a∫10tαf′([txρ+(1−t)bρ]1ρ)(txρ+(1−t)bρ)1−1ρdt |
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,b∈I with a<b such that f′∈L[a,b]. If |f′| is p−convex 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(xρ−aρ)α+1b−a {R(a)+S(a)}+M(bρ−xρ)α+1b−a{R(b)+S(b)} | (2.4) |
where
R(λ)=λ1−ρα+22F1(α+2,ρ−1ρ;α+3;1−xρλρ)S(λ)=λ1−ρ(α+1)(α+2)[(α+2)2F1(α+1,ρ−1ρ;α+2;1−xρλρ)−(α+1)2F1(α+2,ρ−1ρ;α+3;1−xρλρ)] |
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)|≤(xρ−aρ)α+1b−a∫10tα|f′([txρ+(1−t)aρ]1ρ)|(txρ+(1−t)aρ)1−1ρdt+(bρ−xρ)α+1b−a∫10tα|f′([txρ+(1−t)bρ]1ρ)|(txρ+(1−t)bρ)1−1ρdt. |
By means of p−convexity of |f′|, following computations can be performed
|Yf(α,ρ;a,x,b)|≤(xρ−aρ)α+1b−a∫10tα[t|f′(x)|+(1−t)|f′(a)|](txρ+(1−t)aρ)1−1ρdt+(bρ−xρ)α+1b−a∫10tα[t|f′(x)|+(1−t)|f′(b)|](txρ+(1−t)bρ)1−1ρdt=(xρ−aρ)α+1b−a×{|f′(x)|∫10tα+1(txρ+(1−t)aρ)1ρ−1dt+|f′(a)|∫10(tα−tα+1)(txρ+(1−t)aρ)1ρ−1dt}+(bρ−xρ)α+1b−a×{|f′(x)|∫10tα+1(txρ+(1−t)bρ)1ρ−1dt+|f′(b)|∫10(tα−tα+1)(txρ+(1−t)bρ)1ρ−1dt}. |
With necessary computations, it is easy to see that
|Yf(α,ρ;a,x,b)|≤(xρ−aρ)α+1b−a {|f′(x)|R(a)+|f′(a)|S(a)}+(bρ−xρ)α+1b−a{|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(xρ−aρ)α+1b−a {R(a)+S(a)}+M(bρ−xρ)α+1b−a{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,b∈I with a<b such that f′∈L[a,b]. If |f′|q is p−convex on I and |f′(x)|≤M for all x∈I−{a,b}, then the following inequality holds
|Yf(α,ρ;a,x,b)|≤Mb−a(1αq+1)1q[(xρ−aρ)α+1K1r(a)+(bρ−xρ)α+1K1r(b)] |
where
K(λ)=ρ(xr(1−ρ)+ρ−λr(1−ρ)+ρ)(xρ−λρ)(r(1−ρ)+ρ) |
and ρ>0, α>0, λ∈{a,b}, r>1,1r+1q=1, r≠ρρ−1 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)|≤(xρ−aρ)α+1b−a∫10tα|f′([txρ+(1−t)aρ]1ρ)|(txρ+(1−t)aρ)1−1ρdt+(bρ−xρ)α+1b−a∫10tα|f′([txρ+(1−t)bρ]1ρ)|(txρ+(1−t)bρ)1−1ρdt. |
By using Hölder inequality, it can be written as
|Yf(α,ρ;a,x,b)|≤(xρ−aρ)α+1b−a(∫10((txρ+(1−t)aρ)1ρ−1)rdt)1r×(∫10tαq|f′([txρ+(1−t)aρ]1ρ)|qdt)1q+(bρ−xρ)α+1b−a(∫10((txρ+(1−t)bρ)1ρ−1)rdt)1r×(∫10tαq|f′([txρ+(1−t)bρ]1ρ)|qdt)1q. |
From the p−convexity of |f′|q and |f′(x)|≤M, it follows that
|Yf(α,ρ;a,x,b)|≤(xρ−aρ)α+1b−aK1r(a)×(∫10tαq+1|f′(x)|qdt+∫10tαq(1−t)|f′(a)|qdt)1q+(bρ−xρ)α+1b−aK1r(b)×(∫10tαq+1|f′(x)|qdt+∫10tαq(1−t)|f′(b)|qdt)1q≤(xρ−aρ)α+1b−aK1r(a)(Mq1αq+2+Mq1(αq+1)(αq+2))1q+(bρ−xρ)α+1b−aK1r(b)(Mq1αq+2+Mq1(αq+1)(αq+2))1q=Mb−a(1αq+1)1q[(xρ−aρ)α+1K1r(a)+(bρ−xρ)α+1K1r(b)] |
which completes the proof.
Theorem 5. Let f:I⊂(0,∞)→R be a differentiable mapping on I∘ and a,b∈I with a<b such that f′∈L[a,b]. If |f′|q is p−convex 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)|≤Mb−a(xρ−aρ)α+1L1−1q(a)(R(a)+S(a))1q+Mb−a(bρ−xρ)α+1L1−1q(b)(R(b)+S(b))1q |
where
R(λ)=λ1−ρα+2 2F1(α+2, ρ−1ρ; α+3; 1−xρλρ)S(λ)=λ1−ρ(α+1)(α+2)[(α+2) 2F1(α+1, ρ−1ρ; α+2; 1−xρλρ)−(α+1) 2F1(α+2, ρ−1ρ; α+3; 1−xρλρ) ]L(λ)=λ1−ρ α+1 2F1(α+1,ρ−1ρ;α+2;1−xρλρ) |
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)|≤(xρ−aρ)α+1b−a∫10tα|f′([txρ+(1−t)aρ]1ρ)|(txρ+(1−t)aρ)1−1ρdt + (bρ−xρ)α+1b−a∫10tα|f′([txρ+(1−t)bρ]1ρ)|(txρ+(1−t)bρ)1−1ρdt. |
Then, making use of Power-Mean inequality, the following computations can be performed
|Yf(α,ρ;a,x,b)|≤(xρ−aρ)α+1b−a(∫10tα(txρ+(1−t)aρ)1ρ−1dt)1−1q×(∫10tα(txρ+(1−t)aρ)1ρ−1|f′([txρ+(1−t)aρ]1ρ)|qdt)1q+(bρ−xρ)α+1b−a(∫10tα(txρ+(1−t)bρ)1ρ−1dt)1−1q×(∫10tα(txρ+(1−t)bρ)1ρ−1|f′([txρ+(1−t)bρ]1ρ)|qdt)1q. |
Hence |f′|q is chosen as p−convex on I
|Yf(α,ρ;a,x,b)|≤(xρ−aρ)α+1L1−1q(a)b−a×(∫10tα+1(txρ+(1−t)aρ)1ρ−1|f′(x)|qdt + ∫10(tα−tα+1)(txρ+(1−t)aρ)1ρ−1|f′(a)|qdt )1q+(bρ−xρ)α+1L1−1q(b)b−a×(∫10tα+1(txρ+(1−t)bρ)1ρ−1|f′(x)|qdt + ∫10(tα−tα+1)(txρ+(1−t)bρ)1ρ−1|f′(b)|qdt )1q. |
With necessary computations, it can be easily seen that
|Yf(α,ρ;a,x,b)|=(xρ−aρ)α+1L1−1q(a)b−a(|f′(x)|qR(a)+|f′(a)|qS(a))1q + (bρ−xρ)α+1L1−1q(b)b−a(|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(xρ−aρ)α+1L1−1q(a)b−a(R(a)+S(a))1q + M(bρ−xρ)α+1L1−1q(b)b−a(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,b∈R, |
(2) The logarithmic mean:
L=L(a,b)=b−alnb−lna; a,b>0; a,b∈R. |
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)b−aL−1(a(a2),b(b2))+2A(a,b)|≤|M|(b2−a2)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 p−convex on (0,∞) for p≥1.
Proposition 2. Let 0<a<b and a+b2<21ρa. Then the following inequality holds
|4A−1(a,b)−4L−1(a,b)|≤b2−a22a2. |
Proof. The proof is immediate from Theorem 2.1 on applying α=1, ρ=2, x=a+b2 and f(x)=x−2 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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