Home Mathematics On some new Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in (p, q)-calculus with applications
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On some new Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in (p, q)-calculus with applications

  • Xue-Xiao You , Muhammad Aamir Ali EMAIL logo , Humaira Kalsoom , Jarunee Soontharanon and Thanin Sitthiwirattham EMAIL logo
Published/Copyright: August 26, 2022

Abstract

In this study, we establish some new Hermite-Hadamard type inequalities for s-convex functions in the second sense using the post-quantum calculus. Moreover, we prove a new ( p , q ) -integral identity to prove some new Ostrowski type inequalities for ( p , q ) -differentiable functions. We also show that the newly discovered results are generalizations of comparable results in the literature. Finally, we give application to special means of real numbers using the newly proved inequalities.

MSC 2010: 26D10; 26D15; 26A51

1 Introduction

The Hermite-Hadamard (HH) inequality, which was independently found by Hermite and Hadamard (see, also [1], and [2, p. 137]), is particularly important in convex functions theory:

(1) ϝ π 1 + π 2 2 1 π 2 π 1 π 1 π 2 ϝ ( x ) d x ϝ ( π 1 ) + ϝ ( π 2 ) 2 ,

where ϝ is a convex function on [ π 1 , π 2 ] in this case. The aforementioned inequality is true in reverse order for concave mappings.

In [3], Hudzik and Maligranda defined s-convex functions in the second sense as follows: a mapping ϝ : R + R , where R + = [ 0 , ) is called s-convex in the second sense if

ϝ ( t x + ( 1 t ) y ) t s ϝ ( x ) + ( 1 t ) s ϝ ( y )

for all x , y R + and t [ 0 , 1 ] and s ( 0 , 1 ] . Dragomir and Fitzpatrick [4] then used this newly discovered class of functions to prove the HH inequality on [ π 1 , π 2 ] as follows:

(2) 2 s 1 ϝ π 1 + π 2 2 1 π 2 π 1 π 1 π 2 ϝ ( x ) d x ϝ ( π 1 ) + ϝ ( π 2 ) s + 1 .

On the other hand, several works in the field of q -analysis are being carried out, beginning with Euler, to achieve mastery in the mathematics that underpins quantum computing. The link between physics and mathematics is referred to as q -calculus. It has a wide range of applications in different areas of pure and applied mathematics [5,6]. Euler is thought to be the inventor of this significant branch of mathematics. In Newton’s work on infinite series, he used the q parameter. Later, Jackson [7,8] presented the q -calculus that knew without limits calculus in a logical approach. Al-Salam [9] presented the q -analogue of the q -fractional integral and the q -Riemann-Liouville fractional in 1966. Since then, the amount of study in this area has steadily expanded. In particular, in 2013, Tariboon and Ntouyas introduced D q π 1 -difference operator and q π 1 -integral in [10]. In 2020, Bermudo et al. introduced the notion of D q π 2 derivative and q π 2 -integral in [11]. Sadjang generalized to quantum calculus and introduced the notions of post-quantum calculus or shortly ( p , q ) -calculus in [12]. Soontharanon and Sitthiwirattham [13] introduced the notions of fractional ( p , q ) -calculus later on. In [14], Tunç and Göv gave the post-quantum variant of D q π 1 -difference operator and q π 1 -integral. Recently, in 2021, Vivas-Cortez et al. introduced the notions of D p , q π 2 derivative and ( p , q ) π 2 -integral in [15].

Many integral inequalities have been studied using quantum integrals for various types of functions. For example, in [16,17,18, 19,11,20, 21,22,23], the authors used D q π 1 , D q π 2 -derivatives and q π 1 , q π 2 -integrals to prove HH integral inequalities and their left-right estimates for convex and coordinated convex functions. In [24], Noor et al. presented a generalized version of quantum HH integral inequalities. For generalized quasi-convex functions, Nwaeze and Tameru proved certain parameterized quantum integral inequalities in [25]. Khan et al. proved quantum HH inequality using the green function in [26]. Budak et al. [27], Ali et al. [28,29] and Vivas-Cortez et al. [30] developed new quantum Simpson’s and quantum Newton’s type inequalities for convex and coordinated convex functions. For quantum Ostrowski’s inequalities for convex and co-ordinated convex functions, readers refer to [31,32,33]. Kunt et al. [34] generalized the results of [18] and proved Hermite-Hadamard type inequalities and their left estimates using D p , q π 1 -difference operator and ( p , q ) π 1 -integral. Recently, Latif et al. [35] found the right estimates of Hermite-Hadamard type inequalities proved by Kunt et al. [34].

Inspired by these ongoing studies, in the context of ( p , q ) -calculus, we prove several new Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in the second sense.

The following is the structure of this article: Section 2 provides a brief overview of the fundamentals of q -calculus as well as other related studies in this field. In Section 3, we go over some basic ( p , q ) -calculus notions and inequalities. In Section 4, we show the relationship between the results presented here and related results in the literature by proving post-quantum HH inequalities for s-convex functions in the second sense. Post-quantum Ostrowski type inequalities for s-convex functions in the second are presented in Section 5. In Section 6, we present some applications to special means of real numbers for newly established inequalities. Section 7 concludes with some recommendations for future research.

2 Preliminaries of q -calculus and some inequalities

In this section, we revisit several previously regarded ideas. In addition, throughout the paper, s ( 0 , 1 ] , and we use the following notations (see, [6]):

[ n ] q = 1 q n 1 q = 1 + q + q 2 + + q n 1 , q ( 0 , 1 ) .

In [8], Jackson gave the q -Jackson integral from 0 to π 2 for 0 < q < 1 as follows:

(3) 0 π 2 ϝ ( x ) d q x = ( 1 q ) π 2 n = 0 q n ϝ ( π 2 q n )

provided the sum converge absolutely.

Definition 1

[10] For a function ϝ : [ π 1 , π 2 ] R , the q π 1 -derivative of ϝ at x [ π 1 , π 2 ] is characterized by the expression:

(4) D q π 1 ϝ ( x ) = ϝ ( x ) ϝ ( q x + ( 1 q ) π 1 ) ( 1 q ) ( x π 1 ) , x π 1 .

If x = π 1 , we define D q π 1 ϝ ( π 1 ) = lim x π 1 D q π 1 ϝ ( x ) if it exists, and it is finite.

Definition 2

[11] For a function ϝ : [ π 1 , π 2 ] R , the q π 2 -derivative of ϝ at x [ π 1 , π 2 ] is characterized by the expression:

(5) D q π 2 ϝ ( x ) = ϝ ( q x + ( 1 q ) π 2 ) ϝ ( x ) ( 1 q ) ( π 2 x ) , x π 2 .

If x = π 2 , we define D q π 2 ϝ ( π 2 ) = lim x π 2 D q π 2 ϝ ( x ) if it exists and it is finite.

Definition 3

[10] Let ϝ : [ π 1 , π 2 ] R be a function. Then, the q π 1 -definite integral on [ π 1 , π 2 ] is defined as follows:

(6) π 1 π 2 ϝ ( x ) d q π 1 x = ( 1 q ) ( π 2 π 1 ) n = 0 q n ϝ ( q n π 2 + ( 1 q n ) π 1 ) = ( π 2 π 1 ) 0 1 ϝ ( ( 1 t ) π 1 + t π 2 ) d q t .

Definition 4

[11] Let ϝ : [ π 1 , π 2 ] R be a function. Then, the q π 2 -definite integral on [ π 1 , π 2 ] is defined as follows:

(7) π 1 π 2 ϝ ( x ) d q π 2 x = ( 1 q ) ( π 2 π 1 ) n = 0 q n ϝ ( q n π 1 + ( 1 q n ) π 2 ) = ( π 2 π 1 ) 0 1 ϝ ( t π 1 + ( 1 t ) π 2 ) d q t .

In [11], Bermudo et al. established the following quantum HH type inequality.

Theorem 1

For the convex mapping ϝ : [ π 1 , π 2 ] R , the following inequality holds

(8) ϝ π 1 + π 2 2 1 2 ( π 2 π 1 ) π 1 π 2 ϝ ( x ) d q π 1 x + π 1 π 2 ϝ ( x ) d q π 2 x ϝ ( π 1 ) + ϝ ( π 2 ) 2 .

In [33], Budak et al. proved the following Ostrowski inequality by using the concepts of quantum derivatives and integrals.

Theorem 2

Let ϝ : [ π 1 , π 2 ] R R be a function and D q π 2 ϝ and d q π 1 ϝ be two continuous and integrable functions on [ π 1 , π 2 ] . If D q π 2 ϝ ( t ) , D q π 1 ϝ ( t ) M for all t [ π 1 , π 2 ] , then we have the following quantum quantum Ostrowski inequality:

(9) ϝ ( x ) 1 π 2 π 1 π 1 x ϝ ( t ) d q π 1 t + x π 2 ϝ ( t ) d q π 2 t q M ( π 2 π 1 ) ( x π 1 ) 2 + ( π 2 x ) 2 [ 2 ] q .

Recently, Asawasamrit et al. [36] gave the following generalizations of inequalities (8) and (9) using the s-convexity.

Theorem 3

Assume that the mapping ϝ : [ 0 , ) R is s-convex in the second sense and π 1 , π 2 [ 0 , ) with π 1 < π 2 , then the following inequality holds for s ( 0 , 1 ] :

(10) 2 s 1 ϝ π 1 + π 2 2 1 2 ( π 2 π 1 ) π 1 π 2 ϝ ( x ) d q π 1 x + π 1 π 2 ϝ ( x ) d q π 2 x ϝ ( π 1 ) + ϝ ( π 2 ) [ s + 1 ] q .

Theorem 4

Let ϝ : [ π 1 , π 2 ] R R be function and D q π 2 ϝ and D q π 1 ϝ be two continuous and integrable functions on [ π 1 , π 2 ] . If D q π 2 ϝ ( t ) , D q π 1 ϝ ( t ) M for all t [ π 1 , π 2 ] , then we have the following quantum Ostrowski inequality for s-convex functions in the second sense:

(11) ϝ ( x ) 1 π 2 π 1 π 1 x ϝ ( t ) d q π 1 t + x π 2 ϝ ( t ) d q π 2 t M q π 2 π 1 1 [ s + 2 ] q + Θ 11 [ ( x π 1 ) 2 + ( π 2 x ) 2 ] ,

where

Θ 11 = 0 1 t ( 1 t ) d q s t .

3 Post-quantum calculus and some inequalities

In this section, we review some fundamental notions and notations of ( p , q ) -calculus.

The [ n ] p , q is said to be ( p , q )-integers and expressed as follows:

[ n ] p , q = p n q n p q

with 0 < q < p 1 . The [ n ] p , q ! and n k ! are called ( p , q )-factorial and ( p , q )-binomial, respectively, and expressed as follows:

[ n ] p , q ! = k = 1 n [ k ] p , q , n 1 , [ 0 ] p , q ! = 1 , n k ! = [ n ] p , q ! [ n k ] p , q ! [ k ] p , q ! .

Definition 5

[12] The ( p , q ) -derivative of mapping ϝ : [ π 1 , π 2 ] R is given as follows:

D p , q ϝ ( x ) = ϝ ( p x ) ϝ ( q x ) ( p q ) x , x 0

with 0 < q < p 1 .

Definition 6

[14] The ( p , q ) π 1 -derivative of mapping ϝ : [ π 1 , π 2 ] R is given as follows:

(12) D p , q π 1 ϝ ( x ) = ϝ ( p x + ( 1 p ) π 1 ) ϝ ( q x + ( 1 q ) π 1 ) ( p q ) ( x π 1 ) , x π 1

with 0 < q < p 1 . For x = π 1 , we state D p , q π 1 ϝ ( π 1 ) = lim x π 1 D p , q π 1 ϝ ( x ) if it exists and it is finite.

Definition 7

[15] The ( p , q ) π 2 -derivative of mapping ϝ : [ π 1 , π 2 ] R is given as follows:

(13) D p , q π 2 ϝ ( x ) = ϝ ( q x + ( 1 q ) π 2 ) ϝ ( p x + ( 1 p ) π 2 ) ( p q ) ( π 2 x ) , x π 2 .

with 0 < q < p 1 . For x = π 2 , we state D p , q π 2 ϝ ( π 2 ) = lim x π 2 D p , q π 2 ϝ ( x ) if it exists and it is finite.

Remark 1

It is clear that if we use p = 1 in (12) and (13), then the equalities (12) and (13) reduce to (4) and (5), respectively.

Definition 8

[14] The definite ( p , q ) π 1 -integral of mapping ϝ : [ π 1 , π 2 ] R on [ π 1 , π 2 ] is stated as follows:

(14) π 1 x ϝ ( τ ) d p , q π 1 τ = ( p q ) ( x π 1 ) n = 0 q n p n + 1 ϝ q n p n + 1 x + 1 q n p n + 1 π 1

with 0 < q < p 1 .

Definition 9

[15] The definite ( p , q ) π 2 -integral of mapping ϝ : [ π 1 , π 2 ] R on [ π 1 , π 2 ] is stated as follows:

(15) x π 2 ϝ ( τ ) d p , q π 2 τ = ( p q ) ( π 2 x ) n = 0 q n p n + 1 ϝ q n p n + 1 x + 1 q n p n + 1 π 2

with 0 < q < p 1 .

Remark 2

It is evident that if we pick p = 1 in (14) and (15), then the equalities (14) and (15) change into (6) and (7), respectively.

Remark 3

If we take π 1 = 0 and x = π 2 = 1 in (14), then we have

0 1 ϝ ( τ ) d p , q 0 τ = ( p q ) n = 0 q n p n + 1 ϝ q n p n + 1 .

Similarly, by taking x = π 1 = 0 and π 2 = 1 in (15), then we obtain that

0 1 ϝ ( τ ) d p , q 1 τ = ( p q ) n = 0 q n p n + 1 ϝ 1 q n p n + 1 .

Lemma 1

[15] We have the following equalities:

π 1 π 2 ( π 2 x ) α d p , q π 2 x = ( π 2 π 1 ) α + 1 [ α + 1 ] p , q

π 1 π 2 ( x π 1 ) α d p , q π 1 x = ( π 2 π 1 ) α + 1 [ α + 1 ] p , q ,

where α R { 1 } .

Recently, Vivas-Cortez et al. [15] proved the following HH type inequalities for convex functions using the ( p , q ) π 2 -integral:

Theorem 5

[15] For a convex mapping ϝ : [ π 1 , π 2 ] R , which is differentiable on [ π 1 , π 2 ] , the following inequalities hold for ( p , q ) π 2 -integral:

(16) ϝ p π 1 + q π 2 [ 2 ] p , q 1 p ( π 2 π 1 ) p π 1 + ( 1 p ) π 2 π 2 ϝ ( x ) d p , q π 2 x p ϝ ( π 1 ) + q ϝ ( π 2 ) [ 2 ] p , q ,

where 0 < q < p 1 .

Theorem 6

[15] For a convex function ϝ : [ π 1 , π 2 ] R , the following inequality holds:

(17) ϝ π 1 + π 2 2 1 2 p ( π 2 π 1 ) π 1 p π 2 + ( 1 p ) π 1 ϝ ( x ) d p , q π 1 x + p π 1 + ( 1 p ) π 2 π 2 ϝ ( x ) d p , q π 2 x ϝ ( π 1 ) + ϝ ( π 2 ) 2 ,

where 0 < q < p 1 .

4 Hermite-Hadamard inequalities

In this section, we prove HH inequalities for s-convex functions in the second kind using the post-quantum integrals.

Theorem 7

Assume that the mapping ϝ : [ 0 , ) R is s-convex in the second sense and π 1 , π 2 [ 0 , ) with π 1 < π 2 , then the following inequality holds for s ( 0 , 1 ] :

(18) 2 s 1 ϝ π 1 + π 2 2 1 2 p ( π 2 π 1 ) π 1 π 2 ϝ ( x ) d p , q π 1 x + π 1 π 2 ϝ ( x ) d p , q π 2 x ϝ ( π 1 ) + ϝ ( π 2 ) [ s + 1 ] p , q .

Proof

We have s-convexity, as we know from s-convexity

(19) 2 s ϝ x + y 2 ϝ ( x ) + ϝ ( y ) .

We obtain the following by putting x = t π 2 + ( 1 t ) π 1 and y = t π 1 + ( 1 t ) π 2 in (19)

2 s ϝ π 1 + π 2 2 ϝ ( t π 2 + ( 1 t ) π 1 ) + ϝ ( t π 1 + ( 1 t ) π 2 ) .

From Definitions 8 and 9, we have

2 s 1 ϝ π 1 + π 2 2 1 2 p ( π 2 π 1 ) π 1 p π 2 + ( 1 p ) π 1 ϝ ( x ) d p , q π 1 x + p π 1 + ( 1 p ) π 2 π 2 ϝ ( x ) d p , q π 2 x ,

and the first inequality in (18) is proved.

To prove the second inequality, we use the s-convexity, and we have

(20) ϝ ( t π 2 + ( 1 t ) π 1 ) t s ϝ ( π 2 ) + ( 1 t ) s ϝ ( π 1 )

and

(21) ϝ ( t π 1 + ( 1 t ) π 2 ) t s ϝ ( π 1 ) + ( 1 t ) s ϝ ( π 2 ) .

By adding (20) and (21), from Definitions 8 and 9, we have

1 2 p ( π 2 π 1 ) π 1 p π 2 + ( 1 p ) π 1 ϝ ( x ) d p , q π 1 x + p π 1 + ( 1 p ) π 2 π 2 ϝ ( x ) d p , q π 2 x ϝ ( π 1 ) + ϝ ( π 2 ) [ s + 1 ] p , q ,

and the proof is completed.□

Example 1

For s-convex function f ( x ) = x s , from inequality (18) with a = s = 1 , b = 2 , p = 1 2 , and q = 1 4 , we have

2 s 1 ϝ π 1 + π 2 2 = 3 2 ,

1 2 p ( π 2 π 1 ) π 1 π 2 ϝ ( x ) d p , q π 1 x + π 1 π 2 ϝ ( x ) d p , q π 2 x = 1 2 1 4 n = 0 1 4 n 1 2 n + 1 1 4 n 1 2 n + 1 2 + 1 1 4 n 1 2 n + 1 + 1 2 1 4 n = 0 1 4 n 1 2 n + 1 1 4 n 1 2 n + 1 + 1 1 4 n 1 2 n + 1 2 = 3

and

ϝ ( π 1 ) + ϝ ( π 2 ) [ 1 + s ] p , q = 1 + 2 1 4 + 1 2 = 4 .

Thus,

3 2 < 3 < 4 ,

which shows that the inequality proved in Theorem 7 is true.

Remark 4

If we set s = 1 in Theorem 7, then we recapture the inequality (17).

Remark 5

In Theorem 7, if we take the limit as p = 1 , then inequality (18) becomes the inequality (10).

Remark 6

In Theorem 7, if we take p = 1 and later take the limit as q 1 , then inequality (18) becomes the inequality (2).

5 Ostrowski’s inequalities

In this section, we prove post-quantum Ostrowski type inequalities for s-convex functions in the second sense.

We begin with the following identity.

Lemma 2

Let ϝ : [ π 1 , π 2 ] R R be a function. If D p , q π 2 ϝ and π 1 D p , q ϝ are two continuous and integrable functions on [ π 1 , π 2 ] , then for all x [ π 1 , π 2 ] , we have

(22) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t = q ( x π 1 ) 2 π 2 π 1 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) d p , q 0 t q ( π 2 x ) 2 π 2 π 1 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) d p , q 1 t .

Proof

From Definitions 6 and 7, we have

D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) = ϝ ( p t x + ( 1 p t ) π 1 ) ϝ ( q t x + ( 1 q t ) π 1 ) t ( x π 1 ) ( p q )

and

D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) = ϝ ( q t x + ( 1 q t ) π 2 ) ϝ ( p t x + ( 1 p t ) π 2 ) t ( π 2 x ) ( p q ) .

By using Definition 9, we have

(23) I 1 = 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) d p , q 1 t = 1 ( π 2 x ) ( p q ) 0 1 [ ϝ ( q t x + ( 1 q t ) π 2 ) ϝ ( p t x + ( 1 p t ) π 2 ) ] d p , q 1 t = 1 π 2 x n = 0 q n p n + 1 ϝ q n + 1 p n + 1 x + 1 q n + 1 p n + 1 π 2 n = 0 q n p n + 1 ϝ q n p n x + 1 q n p n π 2 = 1 π 2 x 1 q n = 0 q n + 1 p n + 1 ϝ q n + 1 p n + 1 x + 1 q n + 1 p n + 1 π 2 1 p n = 0 q n p n ϝ q n p n x + 1 q n p n π 2 = 1 π 2 x 1 q 1 p n = 0 q n p n ϝ q n p n x + 1 q n p n π 2 1 q ϝ ( x ) = 1 π 2 x p q p q n = 0 q n p n ϝ q n p n x + 1 q n p n π 2 1 q ϝ ( x ) = 1 π 2 x 1 p q ( π 2 x ) p x + ( 1 p ) π 2 π 2 ϝ ( x ) d p , q π 2 x 1 q ϝ ( x ) .

Similarly, from Definition 8, we have

(24) I 2 = 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) d p , q 0 t = 1 x π 1 1 q ϝ ( x ) 1 p q ( x π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( x ) d p , q π 1 x .

Thus, we obtain the resultant equality (22) by subtracting (23) from (24).□

Remark 7

In Lemma 2, if we set p = 1 , then we obtain the equality:

ϝ ( x ) 1 ( π 2 π 1 ) π 1 x ϝ ( t ) d q π 1 t + x π 2 ϝ ( t ) d q π 2 t = q ( x π 1 ) 2 π 2 π 1 0 1 t D q π 1 ϝ ( t x + ( 1 t ) π 1 ) d q 0 t q ( π 2 x ) 2 π 2 π 1 0 1 t D q π 2 ϝ ( t x + ( 1 t ) π 2 ) d q 1 t ,

which is proved by Budak et al. in [33].

Remark 8

In Lemma 2, if we set p = 1 and later taking the limit as q 1 , then we obtain [37, Lemma 1].

Theorem 8

Assume that the mapping ϝ : I [ 0 , ) R is differentiable and π 1 , π 2 I with π 1 < π 2 . If D p , q π 1 ϝ and D p , q π 2 ϝ are s-convex mappings in the second sense, then the following inequality holds:

(25) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t

q ( x π 1 ) 2 π 2 π 1 1 [ s + 2 ] p , q D p , q π 1 ϝ ( x ) + Θ 1 D p , q π 1 ϝ ( π 1 ) + q ( π 2 x ) 2 π 2 π 1 1 [ s + 2 ] p , q D p , q π 2 ϝ ( x ) + Θ 2 D p , q π 2 ϝ ( π 2 ) ,

where

Θ 1 = 0 1 t ( 1 t ) s d p , q 0 t

and

Θ 2 = 0 1 t ( 1 t ) s d p , q 1 t .

Proof

From Lemma 2 and properties of the modulus, we have

(26) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q ( x π 1 ) 2 π 2 π 1 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) d p , q 0 t + q ( π 2 x ) 2 π 2 π 1 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) d p , q 1 t .

Since the mapping D p , q π 1 ϝ and D p , q π 2 ϝ are s-convexities in the second sense, therefore

(27) 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) d p , q 0 t 0 1 t s + 1 D p , q π 1 ϝ ( x ) d p , q 0 t + 0 1 t ( 1 t ) s D p , q π 1 ϝ ( π 1 ) d p , q 0 t = 1 [ s + 2 ] p , q D p , q π 1 ϝ ( x ) + Θ 1 D p , q π 1 ϝ ( π 1 )

and

(28) 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) d p , q 1 t 0 1 t s + 1 D p , q π 2 ϝ ( x ) d p , q 1 t + 0 1 t ( 1 t ) s D p , q π 2 ϝ ( π 2 ) d p , q 1 t = 1 [ s + 2 ] p , q D p , q π 2 ϝ ( x ) + Θ 2 D p , q π 2 ϝ ( π 2 ) .

We obtain the resultant inequality (25) by putting (27) and (28) in (26).□

Corollary 1

If we set s = 1 in Theorem 8, then we obtain the following new Ostrowski type inequality for convex functions:

ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q ( x π 1 ) 2 π 2 π 1 1 [ 3 ] p , q D p , q π 1 ϝ ( x ) + [ 3 ] p , q [ 2 ] p , q [ 3 ] p , q [ 2 ] p , q D p , q π 1 ϝ ( π 1 ) + q ( π 2 x ) 2 π 2 π 1 1 [ 3 ] p , q D p , q π 2 ϝ ( x ) + [ 3 ] p , q [ 2 ] p , q [ 3 ] p , q [ 2 ] p , q D p , q π 2 ϝ ( π 2 ) .

Remark 9

In Theorem 8, if we set p = 1 , then Theorem 8 reduces to [36, Theorem 4.1].

Remark 10

In Corollary 1, if we set p = 1 , then we obtain the following inequality:

ϝ ( x ) 1 π 2 π 1 π 1 x ϝ ( t ) d q π 1 t + x π 2 ϝ ( t ) d q π 2 t q ( π 2 π 1 ) [ 2 ] q [ 3 ] q [ ( x π 1 ) 2 ( [ 2 ] q D q π 1 ϝ ( x ) + q 2 D q π 1 ϝ ( π 1 ) ) + ( π 2 x ) 2 ( [ 2 ] q D q π 2 ϝ ( x ) + q 2 D q π 2 ϝ ( π 2 ) ) ] ,

which is given by Budak et al. in [33].

Corollary 2

If we assume D p , q π 1 ϝ ( x ) , D p , q π 1 ϝ ( x ) M in Theorem 8, then we have following post-quantum Ostrowski type inequality for s-convex functions in the second sense:

(29) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t M q ( x π 1 ) 2 π 2 π 1 1 [ s + 2 ] p , q + Θ 1 + M q ( π 2 x ) 2 π 2 π 1 1 [ s + 2 ] p , q + Θ 2 .

Remark 11

In Corollary 2, if we set p = 1 , then Corollary 2 reduces to [36, Corollary 4.1].

Remark 12

If we set s = p = 1 in Corollary 2, then we recapture inequality (9).

Remark 13

In Corollary 2, if we set p = 1 and later take the limit as q 1 , then Corollary 2 reduces to [38, Theorem 2].

Theorem 9

Assume that the mapping ϝ : I [ 0 , ) R is differentiable and π 1 , π 2 I with π 1 < π 2 . If D p , q π 1 ϝ p 1 and D p , q π 2 ϝ p 1 , p 1 1 are s-convex mappings in the second sense, then the following inequality holds:

(30) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q π 2 π 1 1 [ 2 ] p , q 1 1 p 1 ( x π 1 ) 2 1 [ s + 2 ] p , q D p , q π 1 ϝ ( x ) p 1 + Θ 1 D p , q π 1 ϝ ( π 1 ) p 1 1 p 1 + ( π 2 x ) 2 1 [ s + 2 ] p , q D p , q π 2 ϝ ( x ) p 1 + Θ 2 D p , q π 2 ϝ ( π 2 ) p 1 1 p 1 .

Proof

From Lemma 2, by using properties of the modulus and power mean inequality, we have

(31) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q ( x π 1 ) 2 π 2 π 1 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) d p , q 0 t + q ( π 2 x ) 2 π 2 π 1 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) d p , q 1 t

q ( x π 1 ) 2 π 2 π 1 0 1 t d p , q 0 t 1 1 p 1 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) p 1 d p , q 0 t 1 p 1 + q ( π 2 x ) 2 π 2 π 1 0 1 t d p , q 1 t 1 1 p 1 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) p 1 d p , q 1 t 1 p 1 .

Since the mapping D p , q π 1 ϝ p 1 and D p , q π 2 ϝ p 1 are s-convexities in the second sense, therefore

(32) 0 1 t d p , q 0 t 1 1 p 1 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) p 1 d p , q 0 t 1 p 1 1 [ 2 ] p , q 1 1 p 1 1 [ s + 2 ] p , q D p , q π 1 ϝ ( x ) p 1 + Θ 1 D p , q π 1 ϝ ( π 1 ) p 1 1 p 1

and

(33) 0 1 t d p , q 1 t 1 1 p 1 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) p 1 d p , q 1 t 1 p 1 1 [ 2 ] p , q 1 1 p 1 1 [ s + 2 ] p , q D p , q π 2 ϝ ( x ) p 1 + Θ 2 D p , q π 2 ϝ ( π 2 ) p 1 1 p 1 .

We obtain the resultant inequality (30) by putting (32) and (33) in (31).□

Corollary 3

If we set s = 1 in Theorem 9, then we obtain the following new Ostrowski type inequality for convex functions:

ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q π 2 π 1 1 [ 2 ] p , q 1 1 p 1 ( x π 1 ) 2 1 [ 3 ] p , q D p , q π 1 ϝ ( x ) p 1 + [ 3 ] p , q [ 2 ] p , q [ 3 ] p , q [ 2 ] p , q D p , q π 1 ϝ ( π 1 ) p 1 1 p 1 + ( π 2 x ) 2 1 [ 3 ] p , q D p , q π 2 ϝ ( x ) p 1 + [ 3 ] p , q [ 2 ] p , q [ 3 ] p , q [ 2 ] p , q D p , q π 2 ϝ ( π 2 ) p 1 1 p 1 .

Remark 14

In Theorem 9, if we set p = 1 , then Theorem 9 reduces to [36, Theorem 4.2].

Remark 15

In Corollary 3, if we set p = 1 , then we obtain the following inequality:

ϝ ( x ) 1 π 2 π 1 π 1 x ϝ ( t ) d q π 1 t + x π 2 ϝ ( t ) d q π 2 t q ( π 2 π 1 ) [ 2 ] q ( x π 1 ) 2 [ 2 ] q D q π 1 ϝ ( x ) p + q 2 D q π 1 ϝ ( π 1 ) p [ 3 ] q 1 p + ( π 2 x ) 2 [ 2 ] q D q π 2 ϝ ( x ) p + q 2 D q π 2 ϝ ( π 2 ) p [ 3 ] q 1 p ,

which is proved by Budak et al. in [33].

Corollary 4

If we assume D p , q π 1 ϝ ( x ) , D p , q π 1 ϝ ( x ) M in Theorem 9, then we have following post-quantum Ostrowski type inequality for s-convex functions in the second sense:

ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t M q π 2 π 1 1 [ 2 ] p , q 1 1 p 1 ( x π 1 ) 2 1 [ s + 2 ] p , q + Θ 1 1 p 1 + ( π 2 x ) 2 1 [ s + 2 ] p , q + Θ 2 1 p 1 .

Remark 16

In Corollary 4, if we set p = 1 , then Corollary 4 reduces to [36, Corollary 4.2].

Remark 17

In Corollary 4, if we set p = 1 and later take the limit as q 1 , then Corollary 4 reduces to [38, Theorem 4].

Theorem 10

Assume that the mapping ϝ : I [ 0 , ) R is differentiable and π 1 , π 2 I with π 1 < π 2 . If D p , q π 1 ϝ p 1 and D p , q π 2 ϝ p 1 , p 1 > 1 are s-convex mappings in the second sense, then the following inequality holds:

(34) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q π 2 π 1 1 [ r 1 + 1 ] p , q 1 r 1 ( x π 1 ) 2 1 [ s + 1 ] p , q ( D p , q π 1 ϝ ( x ) p 1 + D p , q π 1 ϝ ( π 1 ) p 1 ) 1 p 1 + ( π 2 x ) 2 1 [ s + 1 ] p , q ( D p , q π 2 ϝ ( x ) p 1 + D p , q π 2 ϝ ( π 2 ) p 1 ) 1 p 1 ,

where r 1 1 + p 1 1 = 1 .

Proof

From Lemma 2, by using properties of the modulus and Hölder’s inequality, we have

(35) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q ( x π 1 ) 2 π 2 π 1 0 1 t D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) d p , q 0 t + q ( π 2 x ) 2 π 2 π 1 0 1 t D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) d p , q 1 t q ( x π 1 ) 2 π 2 π 1 0 1 t r 1 d p , q 0 t 1 r 1 0 1 D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) p 1 d p , q 0 t 1 p 1 + q ( π 2 x ) 2 π 2 π 1 0 1 t r 1 d p , q 1 t 1 r 1 0 1 D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) p 1 d p , q 1 t 1 p 1 .

Since the mapping D p , q π 1 ϝ p 1 and D p , q π 2 ϝ p 1 are s-convexities in the second sense, therefore

(36) 0 1 t r 1 d p , q 0 t 1 r 1 0 1 D p , q π 1 ϝ ( t x + ( 1 t ) π 1 ) p 1 d p , q 0 t 1 p 1 1 [ r 1 + 1 ] p , q 1 r 1 1 [ s + 1 ] p , q ( D p , q π 1 ϝ ( x ) p 1 + D p , q π 1 ϝ ( π 1 ) p 1 )

and

(37) 0 1 t r 1 d p , q 1 t 1 r 1 0 1 D p , q π 2 ϝ ( t x + ( 1 t ) π 2 ) p 1 d p , q 1 t 1 p 1 1 [ r 1 + 1 ] p , q 1 r 1 1 [ s + 1 ] p , q ( D p , q π 2 ϝ ( x ) p 1 + D p , q π 2 ϝ ( π 2 ) p 1 ) .

We obtain the resultant inequality (34) by putting (36) and (37) in (35).□

Corollary 5

If we set s = 1 in Theorem 10, then we obtain the following new Ostrowski type inequality for convex functions:

ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t q π 2 π 1 1 [ r 1 + 1 ] p , q 1 r 1 ( x π 1 ) 2 1 [ 3 ] p , q ( D p , q π 1 ϝ ( x ) p 1 + D p , q π 1 ϝ ( π 1 ) p 1 ) 1 p 1 + ( π 2 x ) 2 1 [ 3 ] p , q ( D p , q π 2 ϝ ( x ) p 1 + D p , q π 2 ϝ ( π 2 ) p 1 ) 1 p 1 .

Remark 18

In Theorem 9, if we set p = 1 , then Theorem 9 reduces to [36, Theorem 4.3].

Remark 19

In Corollary 5, if we set p = 1 , then we obtain the following inequality:

ϝ ( x ) 1 π 2 π 1 π 1 x ϝ ( t ) d q π 1 t + x π 2 ϝ ( t ) d q π 2 t q π 2 π 1 1 [ r 1 + 1 ] q 1 r 1 ( x π 1 ) 2 D q π 1 ϝ ( x ) p + q D q π 1 ϝ ( π 1 ) p [ 2 ] q 1 p + ( π 2 x ) 2 D q π 2 ϝ ( x ) p + q D q π 2 ϝ ( π 2 ) p [ 2 ] q 1 p ,

which is proved by Budak et al. in [33].

Corollary 6

If we assume D p , q π 1 ϝ ( x ) , D p , q π 1 ϝ ( x ) M in Theorem 10, then we have following post-quantum Ostrowski type inequality for s-convex functions in the second sense:

(38) ϝ ( x ) 1 p ( π 2 π 1 ) π 1 p x + ( 1 p ) π 1 ϝ ( t ) d p , q π 1 t + p x + ( 1 p ) π 2 π 2 ϝ ( t ) d p , q π 2 t M q π 2 π 1 1 [ r 1 + 1 ] p , q 1 r 1 2 [ s + 1 ] p , q 1 p 1 [ ( x π 1 ) 2 + ( π 2 x ) 2 ] .

Remark 20

In Corollary 6, if we set p = 1 , then Corollary 6 reduces to [36, Corollary 4.3].

Remark 21

In Corollary 6, if we set p = 1 and later take the limit as q 1 , then Corollary 6 reduces to [38, Theorem 3].

6 Applications to special means

For arbitrary positive numbers π 1 , π 2 ( π 1 π 2 ) , we consider the means as follows:

  1. The arithmetic mean

    A = A ( π 1 , π 2 ) = π 1 + π 2 2 .

  2. The logarithmic mean

    σ σ = σ σ ( π 1 , π 2 ) = π 2 σ + 1 π 1 σ + 1 ( σ + 1 ) ( π 2 π 1 ) .

Proposition 1

For 0 < π 1 < π 2 and 0 < q < p 1 , the following inequality is true:

1 s + 1 [ A s + 1 ( π 1 , π 2 ) A ( k 1 , k 2 ) ] q ( π 2 π 1 ) 2 1 [ s + 2 ] p , q s s q π 2 π 1 2 + π 1 , p π 2 π 1 2 + π 1 + s s π 2 q π 2 π 1 2 , π 2 p π 2 π 1 2 + Θ 1 A ( π 1 s , π 2 s ) + Θ 2 A ( π 1 s , π 2 s ) ,

where

k 1 = ( p q ) n = 0 q n p n + 1 q n p n π 2 π 1 2 + π 1 s + 1 , k 2 = ( p q ) n = 0 q n p n + 1 π 2 q n p n π 2 π 1 2 s + 1 .

Proof

The inequality (25) in Theorem 8 with x = π 1 + π 2 2 for ϝ ( x ) = x s + 1 s + 1 , where x > 0 leads to this conclusion.□

Proposition 2

For 0 < π 1 < π 2 and 0 < q < p 1 , the following inequality is true:

1 s + 1 [ A s + 1 ( π 1 , π 2 ) A ( k 1 , k 2 ) ] M q ( π 2 π 1 ) 4 2 [ s + 2 ] p , q + Θ 1 + Θ 2 .

Proof

The inequality (29) in Corollary 2 with x = π 1 + π 2 2 for ϝ ( x ) = x s + 1 s + 1 , where x > 0 leads to this conclusion.□

Proposition 3

For 0 < π 1 < π 2 and 0 < q < p 1 , the following inequality is true:

1 s + 1 [ A s + 1 ( π 1 , π 2 ) A ( k 1 , k 2 ) ] q ( π 2 π 1 ) 2 1 [ 2 ] p , q 1 1 p 1 1 [ s + 2 ] p , q s s q π 2 π 1 2 + π 1 , p π 2 π 1 2 + π 1 p 1 + Θ 1 π 1 s p 1 1 p 1 + 1 [ s + 2 ] p , q s s π 2 q π 2 π 1 2 , π 2 p π 2 π 1 2 p 1 + Θ 2 π 2 s p 1 1 p 1 .

Proof

The inequality (30) in Theorem 9 with x = π 1 + π 2 2 for ϝ ( x ) = x s + 1 s + 1 , where x > 0 leads to this conclusion.□

Proposition 4

For 0 < π 1 < π 2 and 0 < q < p 1 , the following inequality is true:

1 s + 1 [ A s + 1 ( π 1 , π 2 ) A ( k 1 , k 2 ) ] q ( π 2 π 1 ) 2 1 [ r 1 + 1 ] p , q 1 r 1 1 [ s + 1 ] p , q s s q π 2 π 1 2 + π 1 , p π 2 π 1 2 + π 1 p 1 + π 1 s p 1 1 p 1 + 1 [ s + 1 ] p , q s s π 2 q π 2 π 1 2 , π 2 p π 2 π 1 2 p 1 + π 2 s p 1 1 p 1 .

Proof

The inequality (34) in Theorem 10 with x = π 1 + π 2 2 for ϝ ( x ) = x s + 1 s + 1 , where x > 0 leads to this conclusion.□

Proposition 5

For 0 < π 1 < π 2 and 0 < q < p 1 , the following inequality is true:

1 s + 1 [ A s + 1 ( π 1 , π 2 ) A ( k 1 , k 2 ) ] M q ( π 2 π 1 ) 2 1 [ r 1 + 1 ] p , q 1 r 1 2 [ s + 1 ] p , q 1 p 1 .

Proof

The inequality (38) in Corollary 6 with x = π 1 + π 2 2 for ϝ ( x ) = x s + 1 s + 1 , where x > 0 leads to this conclusion.□

7 Conclusion

In this work, we proved some new variants of post-quantum Hermite-Hadamard and Ostrowski type inequalities using the ( p , q ) -differentiable s-convex functions in the second sense. We also proved that the newly established results are strong generalizations of the related existing results. Finally, we presented various applications based on the newly established inequalities to demonstrate the utility of our findings. It is a new and interesting problem that upcoming researchers can obtain similar inequalities for different kinds of convexity in their future work.

Acknowledgements

The authors are thankful to the Nanjing Normal University for wonderful research environment provided to the researchers.

  1. Funding information: The work was supported by Philosophy and Social Sciences of Educational Commission of Hubei Province of China (20Y109), and Foundation of Hubei Normal University (2021YJSKCSZY06, 2021056). This work was also supported by King Mongkut’s University of Technology North Bangkok (Contract no. KMUTNB-63-KNOW-021).

  2. Author contributions: All authors contributed equally to the writing of this article. All authors read and approved the final manuscript.

  3. Conflict of interest: The authors declare that they do not have any conflict of interests.

  4. Data availability statement: Data sharing not applicable to this article as no data sets were generated or analyzed during the current study.

References

[1] S. S. Dragomir and C. E. M. Pearce, Selected Topics on Hermite-Hadamard Inequalities and Applications, RGMIA Monographs, Victoria University, 2000. Search in Google Scholar

[2] J. E. Pečarić, F. Proschan, and Y. L. Tong, Convex Functions, Partial Orderings and Statistical Applications, Academic Press, Boston, 1992. Search in Google Scholar

[3] H. Hudzik and L. Maligranda, Some remarks on s-convex functions, Aequationes Math. 48 (1994), 100–11110.1007/BF01837981Search in Google Scholar

[4] S. S. Dragomir and S. Fitzpatrick, The Hadamard inequalities for s-convex functions in the second sense, Demonstr. Math. 32 (1999), 68–696. 10.1515/dema-1999-0403Search in Google Scholar

[5] T. Ernst, A Comprehensive Treatment of q-Calculus, Springer, Basel, 2012. 10.1007/978-3-0348-0431-8Search in Google Scholar

[6] V. Kac and P. Cheung, Quantum Calculus, Springer, New York, 2002. 10.1007/978-1-4613-0071-7Search in Google Scholar

[7] T. Ernst, The History of q-Calculus and New Method, Department of Mathematics, Uppsala University, Sweden, 2000. Search in Google Scholar

[8] F. H. Jackson, On a q-definite integrals, Quarterly J. Pure Appl. Math. 41 (1910), 193–203. Search in Google Scholar

[9] W. Al-Salam, Some fractional q-integrals and q-derivatives, Proc. Edinburgh Math. Soc. 15 (1966), 135–140. 10.1017/S0013091500011469Search in Google Scholar

[10] J. Tariboon and S. K. Ntouyas, Quantum calculus on finite intervals and applications to impulsive difference equations, Adv. Differ. Equ. 2013 (2013), 282. 10.1186/1687-1847-2013-282Search in Google Scholar

[11] S. Bermudo, P. Kórus, and J. N. Valdés, On q-Hermite-Hadamard inequalities for general convex functions, Acta Math. Hungar. 162 (2020), 364–374. 10.1007/s10474-020-01025-6Search in Google Scholar

[12] P. N. Sadjang, On the fundamental theorem of (p,q)-calculus and some (p,q)-Taylor formulas, Results Math. 73 (2018), 1–21. 10.1007/s00025-018-0773-1Search in Google Scholar

[13] J. Soontharanon and T. Sitthiwirattham, On Fractional (p,q)-Calculus, Adv. Differ. Equ. 2020 (2020), 1–18. 10.1186/s13662-019-2438-0Search in Google Scholar PubMed PubMed Central

[14] M. Tunç and E. Göv, Some integral inequalities via (p,q)-calculus on finite intervals, RGMIA Res. Rep. Coll. 19 (2016), 1–12. Search in Google Scholar

[15] M. Vivas-Cortez, M. A. Ali, H. Budak, H. Kalsoom, and P. Agarwal, Some new Hermite-Hadamard and related inequalities for convex functions via (p,q)-integral, Entropy 23 (2021), 828. 10.3390/e23070828Search in Google Scholar PubMed PubMed Central

[16] M. A. Ali, H. Budak, H. M. Abbas, and Y.-M. Chu, Quantum Hermite–Hadamard-type inequalities for functions with convex absolute values of second qπ2-derivatives, Adv. Differ. Equ. 2021 (2021), 1–12. 10.1186/s13662-020-03162-2Search in Google Scholar

[17] M. A. Ali, N. Alp, H. Budak, Y-M. Chu, and Z. Zhang, On some new quantum midpoint type inequalities for twice quantum differentiable convex functions, Open Math. 19 (2021), 427–439. 10.1515/math-2021-0015Search in Google Scholar

[18] N. Alp, M. Z. Sarikaya, M. Kunt, and İ. İşcan, q-Hermite Hadamard inequalities and quantum estimates for midpoint type inequalities via convex and quasi-convex functions, J. King Saud Univ. Sci. 30 (2018), 193–203. 10.1016/j.jksus.2016.09.007Search in Google Scholar

[19] N. Alp and M. Z. Sarikaya, Hermite Hadamardas type inequalities for co-ordinated convex functions on quantum integral, Appl. Math. E-Notes 20 (2020), 341–356. Search in Google Scholar

[20] H. Budak, Some trapezoid and midpoint type inequalities for newly defined quantum integrals, Proyecciones 40 (2021), 199–215. 10.22199/issn.0717-6279-2021-01-0013Search in Google Scholar

[21] H. Budak, M. A. Ali, and M. Tarhanaci, Some new quantum Hermite-Hadamard-like inequalities for coordinated convex functions, J. Optim. Theory Appl. 186 (2020), 899–910. 10.1007/s10957-020-01726-6Search in Google Scholar

[22] S. Jhanthanam, J. Tariboon, S. K. Ntouyas, and K. Nonlaopon, On q-Hermite-Hadamard inequalities for differentiable convex functions, Mathematics 7 (2019), 632. 10.3390/math7070632Search in Google Scholar

[23] M. A. Noor, K. I. Noor, and M. U. Awan, Some quantum estimatesfor Hermite-Hadamard inequalities, Appl. Math. Comput. 251 (2015), 675–679. 10.1016/j.amc.2014.11.090Search in Google Scholar

[24] M. A. Noor, K. I. Noor, and M. U. Awan, Some quantum integral inequalities via preinvex functions, Appl. Math. Comput. 269 (2015), 242–251. 10.1016/j.amc.2015.07.078Search in Google Scholar

[25] E. R. Nwaeze and A. M. Tameru, New parameterized quantumintegral inequalities via η-quasiconvexity, Adv. Differ. Equ. 2019 (2019), 1–12. 10.1186/s13662-018-1939-6Search in Google Scholar

[26] M. A. Khan, M. Noor, E. R. Nwaeze, and Y-M. Chu, Quantum Hermite-Hadamard inequality by means of a Green function, Adv. Differ. Equ. 2020 (2020), 1–20. 10.1186/s13662-019-2438-0Search in Google Scholar PubMed PubMed Central

[27] H. Budak, S. Erden, and M. A. Ali, Simpson and Newton type in equalities for convex functions via newly defined quantum integrals, Math. Methods Appl. Sci. 44 (2020), 378–390. 10.1002/mma.6742Search in Google Scholar

[28] M. A. Ali, H. Budak, Z. Zhang, and H. Yildrim, Some new Simpson’s type inequalities for co-ordinated convex functions in quantum calculus, Math. Methods Appl. Sci. 44 (2021), 4515–4540. 10.22541/au.159440598.88087022Search in Google Scholar

[29] M. A. Ali, M. Abbas, H. Budak, P. Agarwal, G. Murtaza, and Y.-M. Chu, New quantum boundaries for quantum Simpson’s and quantum Newton’s type inequalities for preinvex functions, Adv. Differ. Equ. 2021 (2021), 1–21. 10.1186/s13662-021-03226-xSearch in Google Scholar

[30] M. Vivas-Cortez, M. A. Ali, A. Kashuri, I. B. Sial, and Z. Zhang, Some new Newton’s type integral inequalities for co-ordinated convex functions in quantum calculus, Symmetry 12 (2020), 1476. 10.3390/sym12091476Search in Google Scholar

[31] M. A. Ali, Y.-M. Chu, H. Budak, A. Akkurt, and H. Yildrim, Quantum variant of Montgomery identity and Ostrowski-type inequalities for the mappings of two variables, Adv. Differ. Equ. 2021 (2021), 1–26. 10.1186/s13662-020-03195-7Search in Google Scholar

[32] M. A. Ali, H. Budak, A. Akkurt, and Y-M. Chu, Quantum Ostrowskitype inequalities for twice quantum differentiable functions in quantum calculus, Open Math. 19 (2021), 440–449. 10.1515/math-2021-0020Search in Google Scholar

[33] H. Budak, M. A. Ali, N. Alp, and Y.-M. Chu, Quantum Ostrowski type integral inequalities, J. Math. Inequal. 2021 (2021). Search in Google Scholar

[34] M. Kunt, İ. İşcan, N. Alp, and M. Z. Sarikaya, (p,q)-Hermite-Hadamard inequalities and (p,q)-estimates for midpoint inequalities via convex quasi-convex functions, Rev. R. Acad. Cienc. Exactas Fís. Nat. Ser. A Mat. RACSAM. 112 (2018), 969–992. 10.1007/s13398-017-0402-ySearch in Google Scholar

[35] M. A. Latif, M. Kunt, S. S. Dragomir, and İ. İşcan, Postquantum trapezoid type inequalities, AIMS Math. 5 (2020), 4011–4026. 10.3934/math.2020258Search in Google Scholar

[36] S. Asawasamrit, M. A. Ali, H. Budak, S. K. Ntouyas, and J. Tariboon, Quantum Hermite-Hadamard and quantum Ostrowski type inequalities for s-convex functions in the second sense with applications, AIMS Math. 6 (2021), 13327–13346. 10.3934/math.2021771Search in Google Scholar

[37] P. Cerone and S. S. Dragomir, Ostrowski type inequalities for functions whose derivatives satisfy certain convexity assumptions, Demonstratio Math. 37 (2004), 299–308. 10.1515/dema-2004-0208Search in Google Scholar

[38] M. Alomari, M. Daus, and S. S. Dragomir, Ostrowski type inequalities for functions whose derivatives are s-convex in the second sense, Appl. Math. Lett. 23 (2010), 1071–1076. 10.1016/j.aml.2010.04.038Search in Google Scholar

Received: 2021-09-23
Revised: 2022-03-24
Accepted: 2022-04-08
Published Online: 2022-08-26

© 2022 Xue-Xiao You et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

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  62. Approximations related to the complete p-elliptic integrals
  63. A note on commutators of strongly singular Calderón-Zygmund operators
  64. Generalized Munn rings
  65. Double domination in maximal outerplanar graphs
  66. Existence and uniqueness of solutions to the norm minimum problem on digraphs
  67. On the p-integrable trajectories of the nonlinear control system described by the Urysohn-type integral equation
  68. Robust estimation for varying coefficient partially functional linear regression models based on exponential squared loss function
  69. Hessian equations of Krylov type on compact Hermitian manifolds
  70. Class fields generated by coordinates of elliptic curves
  71. The lattice of (2, 1)-congruences on a left restriction semigroup
  72. A numerical solution of problem for essentially loaded differential equations with an integro-multipoint condition
  73. On stochastic accelerated gradient with convergence rate
  74. Displacement structure of the DMP inverse
  75. Dependence of eigenvalues of Sturm-Liouville problems on time scales with eigenparameter-dependent boundary conditions
  76. Existence of positive solutions of discrete third-order three-point BVP with sign-changing Green's function
  77. Some new fixed point theorems for nonexpansive-type mappings in geodesic spaces
  78. Generalized 4-connectivity of hierarchical star networks
  79. Spectra and reticulation of semihoops
  80. Stein-Weiss inequality for local mixed radial-angular Morrey spaces
  81. Eigenvalues of transition weight matrix for a family of weighted networks
  82. A modified Tikhonov regularization for unknown source in space fractional diffusion equation
  83. Modular forms of half-integral weight on Γ0(4) with few nonvanishing coefficients modulo
  84. Some estimates for commutators of bilinear pseudo-differential operators
  85. Extension of isometries in real Hilbert spaces
  86. Existence of positive periodic solutions for first-order nonlinear differential equations with multiple time-varying delays
  87. B-Fredholm elements in primitive C*-algebras
  88. Unique solvability for an inverse problem of a nonlinear parabolic PDE with nonlocal integral overdetermination condition
  89. An algebraic semigroup method for discovering maximal frequent itemsets
  90. Class-preserving Coleman automorphisms of some classes of finite groups
  91. Exponential stability of traveling waves for a nonlocal dispersal SIR model with delay
  92. Existence and multiplicity of solutions for second-order Dirichlet problems with nonlinear impulses
  93. The transitivity of primary conjugacy in regular ω-semigroups
  94. Stability estimation of some Markov controlled processes
  95. On nonnil-coherent modules and nonnil-Noetherian modules
  96. N-Tuples of weighted noncommutative Orlicz space and some geometrical properties
  97. The dimension-free estimate for the truncated maximal operator
  98. A human error risk priority number calculation methodology using fuzzy and TOPSIS grey
  99. Compact mappings and s-mappings at subsets
  100. The structural properties of the Gompertz-two-parameter-Lindley distribution and associated inference
  101. A monotone iteration for a nonlinear Euler-Bernoulli beam equation with indefinite weight and Neumann boundary conditions
  102. Delta waves of the isentropic relativistic Euler system coupled with an advection equation for Chaplygin gas
  103. Multiplicity and minimality of periodic solutions to fourth-order super-quadratic difference systems
  104. On the reciprocal sum of the fourth power of Fibonacci numbers
  105. Averaging principle for two-time-scale stochastic differential equations with correlated noise
  106. Phragmén-Lindelöf alternative results and structural stability for Brinkman fluid in porous media in a semi-infinite cylinder
  107. Study on r-truncated degenerate Stirling numbers of the second kind
  108. On 7-valent symmetric graphs of order 2pq and 11-valent symmetric graphs of order 4pq
  109. Some new characterizations of finite p-nilpotent groups
  110. A Billingsley type theorem for Bowen topological entropy of nonautonomous dynamical systems
  111. F4 and PSp (8, ℂ)-Higgs pairs understood as fixed points of the moduli space of E6-Higgs bundles over a compact Riemann surface
  112. On modules related to McCoy modules
  113. On generalized extragradient implicit method for systems of variational inequalities with constraints of variational inclusion and fixed point problems
  114. Solvability for a nonlocal dispersal model governed by time and space integrals
  115. Finite groups whose maximal subgroups of even order are MSN-groups
  116. Symmetric results of a Hénon-type elliptic system with coupled linear part
  117. On the connection between Sp-almost periodic functions defined on time scales and ℝ
  118. On a class of Harada rings
  119. On regular subgroup functors of finite groups
  120. Fast iterative solutions of Riccati and Lyapunov equations
  121. Weak measure expansivity of C2 dynamics
  122. Admissible congruences on type B semigroups
  123. Generalized fractional Hermite-Hadamard type inclusions for co-ordinated convex interval-valued functions
  124. Inverse eigenvalue problems for rank one perturbations of the Sturm-Liouville operator
  125. Data transmission mechanism of vehicle networking based on fuzzy comprehensive evaluation
  126. Dual uniformities in function spaces over uniform continuity
  127. Review Article
  128. On Hahn-Banach theorem and some of its applications
  129. Rapid Communication
  130. Discussion of foundation of mathematics and quantum theory
  131. Special Issue on Boundary Value Problems and their Applications on Biosciences and Engineering (Part II)
  132. A study of minimax shrinkage estimators dominating the James-Stein estimator under the balanced loss function
  133. Representations by degenerate Daehee polynomials
  134. Multilevel MC method for weak approximation of stochastic differential equation with the exact coupling scheme
  135. Multiple periodic solutions for discrete boundary value problem involving the mean curvature operator
  136. Special Issue on Evolution Equations, Theory and Applications (Part II)
  137. Coupled measure of noncompactness and functional integral equations
  138. Existence results for neutral evolution equations with nonlocal conditions and delay via fractional operator
  139. Global weak solution of 3D-NSE with exponential damping
  140. Special Issue on Fractional Problems with Variable-Order or Variable Exponents (Part I)
  141. Ground state solutions of nonlinear Schrödinger equations involving the fractional p-Laplacian and potential wells
  142. A class of p1(x, ⋅) & p2(x, ⋅)-fractional Kirchhoff-type problem with variable s(x, ⋅)-order and without the Ambrosetti-Rabinowitz condition in ℝN
  143. Jensen-type inequalities for m-convex functions
  144. Special Issue on Problems, Methods and Applications of Nonlinear Analysis (Part III)
  145. The influence of the noise on the exact solutions of a Kuramoto-Sivashinsky equation
  146. Basic inequalities for statistical submanifolds in Golden-like statistical manifolds
  147. Global existence and blow up of the solution for nonlinear Klein-Gordon equation with variable coefficient nonlinear source term
  148. Hopf bifurcation and Turing instability in a diffusive predator-prey model with hunting cooperation
  149. Efficient fixed-point iteration for generalized nonexpansive mappings and its stability in Banach spaces
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