In this study, we use quantum calculus to prove Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in the second sense. The newly proven results are also shown to be an extension of comparable results in the existing literature. Furthermore, it is provided that how the newly discovered inequalities can be applied to special means of real numbers.
Citation: Suphawat Asawasamrit, Muhammad Aamir Ali, Hüseyin Budak, Sotiris K. Ntouyas, Jessada Tariboon. Quantum Hermite-Hadamard and quantum Ostrowski type inequalities for s-convex functions in the second sense with applications[J]. AIMS Mathematics, 2021, 6(12): 13327-13346. doi: 10.3934/math.2021771
[1] | Humaira Kalsoom, Muhammad Amer Latif, Muhammad Idrees, Muhammad Arif, Zabidin Salleh . Quantum Hermite-Hadamard type inequalities for generalized strongly preinvex functions. AIMS Mathematics, 2021, 6(12): 13291-13310. doi: 10.3934/math.2021769 |
[2] | Attazar Bakht, Matloob Anwar . Ostrowski and Hermite-Hadamard type inequalities via $ (\alpha-s) $ exponential type convex functions with applications. AIMS Mathematics, 2024, 9(10): 28130-28149. doi: 10.3934/math.20241364 |
[3] | Nattapong Kamsrisuk, Donny Passary, Sotiris K. Ntouyas, Jessada Tariboon . Quantum calculus with respect to another function. AIMS Mathematics, 2024, 9(4): 10446-10461. doi: 10.3934/math.2024510 |
[4] | Saad Ihsan Butt, Muhammad Nasim Aftab, Hossam A. Nabwey, Sina Etemad . Some Hermite-Hadamard and midpoint type inequalities in symmetric quantum calculus. AIMS Mathematics, 2024, 9(3): 5523-5549. doi: 10.3934/math.2024268 |
[5] | Serap Özcan, Saad Ihsan Butt, Sanja Tipurić-Spužević, Bandar Bin Mohsin . Construction of new fractional inequalities via generalized $ n $-fractional polynomial $ s $-type convexity. AIMS Mathematics, 2024, 9(9): 23924-23944. doi: 10.3934/math.20241163 |
[6] | Bandar Bin-Mohsin, Muhammad Uzair Awan, Muhammad Zakria Javed, Sadia Talib, Hüseyin Budak, Muhammad Aslam Noor, Khalida Inayat Noor . On some classical integral inequalities in the setting of new post quantum integrals. AIMS Mathematics, 2023, 8(1): 1995-2017. doi: 10.3934/math.2023103 |
[7] | Miguel Vivas-Cortez, Muhammad Aamir Ali, Ghulam Murtaza, Ifra Bashir Sial . Hermite-Hadamard and Ostrowski type inequalities in $ \mathfrak{h} $-calculus with applications. AIMS Mathematics, 2022, 7(4): 7056-7068. doi: 10.3934/math.2022393 |
[8] | Muhammad Uzair Awan, Muhammad Aslam Noor, Tingsong Du, Khalida Inayat Noor . On $\mathscr{M}$-convex functions. AIMS Mathematics, 2020, 5(3): 2376-2387. doi: 10.3934/math.2020157 |
[9] | Sevda Sezer . The Hermite-Hadamard inequality for $ s $-Convex functions in the third sense. AIMS Mathematics, 2021, 6(7): 7719-7732. doi: 10.3934/math.2021448 |
[10] | Andrea Aglić Aljinović, Domagoj Kovačević, Mehmet Kunt, Mate Puljiz . Correction: Quantum Montgomery identity and quantum estimates of Ostrowski type inequalities. AIMS Mathematics, 2021, 6(2): 1880-1888. doi: 10.3934/math.2021114 |
In this study, we use quantum calculus to prove Hermite-Hadamard and Ostrowski type inequalities for s-convex functions in the second sense. The newly proven results are also shown to be an extension of comparable results in the existing literature. Furthermore, it is provided that how the newly discovered inequalities can be applied to special means of real numbers.
In convex functions theory, Hermite-Hadamard (H-H) inequality is very important and was discovered by C. Hermite and J. Hadamard independently (see, also [23], [41,p.137]),
f(a+b2)≤1b−ab∫af(x)dx≤f(a)+f(b)2 | (1.1) |
where f is a convex function. In the case of concave mappings, the above inequality is satisfied in reverse order. For more recent developments, one can consult [17,18,42,48,49].
Hudzik and Maligranda defined s-convex functions in the second sense in [28], which may be expressed as: a mapping f:R+→R, where R+=[0,∞), is called s-convex in the second sense if
f(tx+(1−t)y)≤tsf(x)+(1−t)sf(y) |
for all x,y∈R+, t∈[0,1], s∈(0,1] and these functions are denoted by f∈k2s. After that, Dragomir and Fitzpatrick [22] used this newly class of functions and proved the following H-H inequality:
2s−1f(a+b2)≤1b−a∫baf(x)dx≤f(a)+f(b)s+1. | (1.2) |
For more recent integral inequalities related to the class of s-convex functions and its generalizations via different integral operators, one can consult [11,19,20,24,25,34,36,40].
On the other hand, several studies have been carried out in the domain of q -analysis, beginning with Euler, in order to achieve proficiency in mathematics that constructs quantum computing q-calculus, which is considered a relationship between physics and mathematics. It has a wide range of applications in mathematics, including combinatorics, simple hypergeometric functions, number theory, orthogonal polynomials, and other sciences, as well as mechanics, relativity theory, and quantum theory [27,32]. Euler is thought to be the inventor of this significant branch of mathematics. He used the q-parameter in Newton's work on infinite series. Later, Jackson presented the q-calculus, which knew no limits calculus, in a methodical manner [26,30]. In 1966, Al-Salam [10] introduced a q-analogue of the q-fractional integral and q -Riemann-Liouville fractional. Since then, the related research has gradually increased. In particular, in 2013, Tariboon and Ntouyas introduced aDq-difference operator and qa-integral in [46]. In 2020, Bermudo et al. introduced the notion of bDq derivative and qb-integral in [12].
Many integral inequalities have been studied using quantum integrals for various types of functions. For example, in [3,6,8,9,12,13,14,31,37,43,44,45], the authors used aDq,bDq-derivatives and qa,qb-integrals to prove H-H integral inequalities and their left-right estimates for convex and coordinated convex functions. In [38], Noor et al. presented a generalized version of quantum H-H integral inequalities. For generalized quasi-convex functions, Nwaeze et al. proved certain parameterized quantum integral inequalities in [39]. Khan et al. proved quantum H-H inequality using the green function in [35]. Budak et al. [15], Ali et al. [2,4], Chu et al. [21] and Vivas-Cortez et al. [47] 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, one can consult [5,7,16].
Inspired by these ongoing studies, we offer a variant of quantum H-H inequality (1.2) and Ostrowski type inequalities for s-convex functions in the second sense. Since the s-convexity is the generalization of convexity, therefore the inequalities proved in this paper using the s -convexity are the generalization of already proved inequalities for convexity that is the main motivation of this paper.
The following is the structure of this paper: A brief overview of the concepts of q-calculus, as well as some related works, is given in Section 2. In Section 3, we show the relationship between the results presented here and comparable results in the literature by proving quantum H-H inequalities for s-convex functions in the second sense. Quantum Ostrowski type inequalities for s-convex functions in the second sense are presented in Section 4. Some applications to special means are given in Section 5. Section 6 concludes with some recommendations for future studies.
In this section, we recollect some formerly regarded concepts. Also, here and further we use q∈(0,1) and the following notation (see [32]):
[n]q=1−qn1−q=1+q+q2+…+qn−1,q∈(0,1). |
In [30], Jackson gave the q-Jackson integral from 0 to b as follows:
b∫0f(x)dqx=(1−q)b∞∑n=0qnf(bqn) | (2.1) |
provided the sum converges absolutely.
Definition 2.1. [46] The qa-derivative of a mapping f:[a,b]→R at x∈[a,b] is defined as:
aDqf(x)=f(x)−f(qx+(1−q)a)(1−q)(x−a),x≠a. | (2.2) |
If x=a, we define aDqf(a)=limx→aaDqf(x) if it exists and it is finite.
Definition 2.2. [12] The qb-derivative of a mapping f:[a,b]→R at x∈[a,b] is defined as:
bDqf(x)=f(qx+(1−q)b)−f(x)(1−q)(b−x),x≠b. |
If x=b, we define bDqf(b)=limx→bbDqf(x) if it exists and it is finite.
Definition 2.3. [46] The qa-integral of a mapping f:[a,b]→R is defined as:
x∫af(t)adqt=(1−q)(x−a)∞∑n=0qnf(qnx+(1−qn)a), |
where x∈[a,b].
Definition 2.4. [12] The qb-integral of a mapping f:[a,b]→R is defined as:
b∫xf(t)bdqt=(1−q)(b−x)∞∑n=0qnf(qnx+(1−qn)b), |
where x∈[a,b].
In [12], Bermudo et al. established the following quantum H-H type inequality:
Theorem 2.1. For the convex mapping f:[a,b]→R, the following inequality holds
f(a+b2)≤12(b−a)[b∫af(x)adqx+b∫af(x)bdqx]≤f(a)+f(b)2. | (2.3) |
In [16], Budak et al. proved the following Ostrowski inequality by using the concepts of quantum derivatives and integrals:
Theorem 2.2. Let f:[a,b]⊂R→R be a function and bDqf and aDqf be two continuous and integrable functions on [a,b]. If |bDqf(t)|,|aDqf(t)|≤M for all t∈[a,b], then we have the following quantum Ostrowski inequality
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qM(b−a)[(x−a)2+(b−x)2[2]q] | (2.4) |
In this section, we prove H-H inequalities for s-convex functions in the second sense using the quantum integrals.
Theorem 3.1. Assume that the mapping f:R+→R is s-convex in the second sense and a,b∈R+ with a<b. If f∈L1([a,b]), then the following inequality holds for s∈(0,1]:
2s−1f(a+b2)≤12(b−a)[∫baf(x)adqx+∫baf(x)bdqx]≤f(a)+f(b)[s+1]q. | (3.1) |
Proof. As f is s-convex in the second sense on R+ we have
f(tx+(1−t)y)≤tsf(x)+(1−t)sf(y), |
for all x,y∈R+ and t∈[0,1].
Obverse that
2sf(x+y2)≤f(x)+f(y). | (3.2) |
We get the following, by putting x=tb+(1−t)a and y=ta+(1−t)b in (3.2)
2sf(a+b2)≤f(tb+(1−t)a)+f(ta+(1−t)b). |
From Definitions 2.3 and 2.4, we have
2s−1f(a+b2)≤12(b−a)[∫baf(x)adqx+∫baf(x)bdqx] |
and the first inequality in (3.1) is proved.
To proved the second inequality, we use the s-convexity and we have
f(tb+(1−t)a)≤tsf(b)+(1−t)sf(a) | (3.3) |
and
f(ta+(1−t)b)≤tsf(a)+(1−t)sf(b). | (3.4) |
By adding (3.3) and (3.4), from Definition 2.3 and 2.4, we have
12(b−a)[∫baf(x)adqx+∫baf(x)bdqx]≤f(a)+f(b)[s+1]q |
and the proof is completed.
Remark 3.1. If we set s=1 in Theorem 3.1, then we recapture the inequality (2.3).
Remark 3.2. In Theorem 3.1, if we take the limit as q→1−, then inequality (3.1) becomes the inequality (1.2).
In this section, we prove Ostrowski's type inequalities for s-convex functions in the second sense. We use the following lemma to prove the new results.
Lemma 4.1. [16] Let f:[a,b]⊂R→R be a function. If bDqf and aDqf are two continuous and integrable functions on [a,b], then for all x∈[a,b] we have
f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]=q(x−a)2b−a1∫0taDqf(tx+(1−t)a)dqt−q(b−x)2b−a1∫0tbDqf(tx+(1−t)b)dqt. | (4.1) |
Theorem 4.1. Assume that the mapping f:I⊂R+→R is differentiable and a,b∈I with a<b. If |aDqf| and |bDqf| are s-convex mappings in the second sense, then the following inequality holds:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(x−a)2b−a[1[s+2]q|aDqf(x)|+Θ1|aDqf(a)|]+q(b−x)2b−a[1[s+2]q|bDqf(x)|+Θ1|bDqf(b)|] | (4.2) |
where
Θ1=∫10t(1−t)sdqt. |
Proof. From Lemma 4.1 and properties of the modulus, we have
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(x−a)2b−a1∫0t|aDqf(tx+(1−t)a)|dqt+q(b−x)2b−a1∫0t|bDqf(tx+(1−t)b)|dqt. | (4.3) |
Since the mappings |aDqf| and |bDqf| are s-convex in the second sense, therefore
1∫0t|aDqf(tx+(1−t)a)|dqt≤∫10ts+1|aDqf(x)|dqt+∫10t(1−t)s|aDqf(a)|dqt=1[s+2]q|aDqf(x)|+Θ1|aDqf(a)| | (4.4) |
and
1∫0t|bDqf(tx+(1−t)b)|dqt≤∫10ts+1|bDqf(x)|dqt+∫10t(1−t)s|bDqf(b)|dqt=1[s+2]q|bDqf(x)|+Θ1|bDqf(b)|. | (4.5) |
We obtain the resultant inequality (4.2) by putting (4.4) and (4.5) in (4.3).
Remark 4.1. If we set s=1 in Theorem 4.1, then we obtain the following inequality
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(b−a)(1+q)(1+q+q2)[(x−a)2((1+q)|aDqf(x)|+q2|aDqf(a)|)+(b−x)2((1+q)|bDqf(x)|+q2|bDqf(b)|)] |
which is given by Budak et al. in [16].
Corollary 4.1. If we assume |aDqf(x)|, |bDqf(x)|≤M in Theorem 4.1, then we have following quantum Ostrowski's type inequality for s-convex functions in the second sense:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤Mqb−a(1[s+2]q+Θ1)[(x−a)2+(b−x)2]. | (4.6) |
Remark 4.2. If we set s=1 in Corollary 4.1, then we recapture inequality (2.4).
Remark 4.3. In Corollary 4.1, if we take the limit as q→1−, then Corollary 4.1 reduces to [1,Theorem 2].
Theorem 4.2. Assume that the mapping f:I⊂R+→R is differentiable and a,b∈I with a<b. If |aDqf|p1 and |bDqf|p1, p1≥1 are s-convex mappings in the second sense, then the following inequality holds:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qb−a(1[2]q)1−1p1[(x−a)2(1[s+2]q|aDqf(x)|p1+Θ1|aDqf(a)|p1)1p1+(b−x)2(1[s+2]q|bDqf(x)|p1+Θ1|bDqf(b)|p1)1p1]. | (4.7) |
Proof. From Lemma 4.1, using properties of the modulus and power mean inequality, we have
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(x−a)2b−a1∫0t|aDqf(tx+(1−t)a)|dqt+q(b−x)2b−a1∫0t|bDqf(tx+(1−t)b)|dqt≤q(x−a)2b−a(1∫0tdqt)1−1p1(1∫0t|aDqf(tx+(1−t)a)|p1dqt)1p1+q(b−x)2b−a(1∫0tdqt)1−1p1(1∫0t|bDqf(tx+(1−t)b)|p1dqt)1p1. | (4.8) |
Since the mappings |aDqf|p1 and |bDqf|p1 are s -convex in the second sense, therefore
(1∫0tdqt)1−1p1(1∫0t|aDqf(tx+(1−t)a)|p1dqt)1p1≤(1[2]q)1−1p1(1[s+2]q|aDqf(x)|p1+Θ1|aDqf(a)|p1)1p1 | (4.9) |
and
(1∫0tdqt)1−1p1(1∫0t|bDqf(tx+(1−t)b)|p1dqt)1p1≤(1[2]q)1−1p1(1[s+2]q|bDqf(x)|p1+Θ1|bDqf(b)|p1)1p1. | (4.10) |
We obtain the resultant inequality (4.7) by putting (4.9) and (4.10) in (4.8).
Remark 4.4. If we set s=1 in Theorem 4.2, then we obtain the following inequality
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(b−a)[2]q[(x−a)2([2]q|aDqf(x)|p1+q2|aDqf(a)|p1[3]q)1p1+(b−x)2([2]q|bDqf(x)|p1+q2|bDqf(b)|p1[3]q)1p1] |
which is proved by Budak et al. in [16].
Corollary 4.2. If we assume |aDqf(x), |aDqf(a)|≤M in Theorem 4.2, then we have following quantum Ostrowski's type inequality for s-convex functions in the second sense:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤Mqb−a(1[2]q)1−1p1(1[s+2]q+Θ1)1p1[(x−a)2+(b−x)2]. |
Remark 4.5. In Corollary 4.2, if we take the limit as q→1−, then Corollary 4.2 reduces to [1,Theorem 4].
Theorem 4.3. Assume that the mapping f:I⊂R+→R is differentiable and a,b∈I with a<b. If |aDqf|p1 and |bDqf|p1, p1>1 are s-convex mappings in the second sense, then the following inequality holds:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qb−a(1[r1+1]q)1r1[(x−a)2(1[s+1]q(|aDqf(x)|p1+|aDqf(a)|p1))1p1+(b−x)2(1[s+1]q(|bDqf(x)|p1+|bDqf(b)|p1))1p1], | (4.11) |
where 1r1+1p1=1.
Proof. From Lemma 4.1, using properties of the modulus and Hölder's inequality, we have
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(x−a)2b−a1∫0t|aDqf(tx+(1−t)a)|dqt+q(b−x)2b−a1∫0t|bDqf(tx+(1−t)b)|dqt≤q(x−a)2b−a(1∫0tr1dqt)1r1(1∫0|aDqf(tx+(1−t)a)|p1dqt)1p1+q(b−x)2b−a(1∫0tr1dqt)1r1(1∫0|bDqf(tx+(1−t)b)|p1dqt)1p1. | (4.12) |
Since the mappings |aDqf|p1 and |bDqf|p1 are s -convex in the second sense, therefore
(1∫0tr1dqt)1r1(1∫0|aDqf(tx+(1−t)a)|p1dqt)1p1≤(1[r1+1]q)1r1(1[s+1]q(|aDqf(x)|p1+|aDqf(a)|p1))1p1 | (4.13) |
and
(1∫0tr1dqt)1r1(1∫0|bDqf(tx+(1−t)b)|p1dqt)1p1≤(1[r1+1]q)1r1(1[s+1]q(|bDqf(x)|p1+|bDqf(b)|p1))1p1. | (4.14) |
We obtain the resultant inequality (4.11) by putting (4.13) and (4.14) in (4.12).
Remark 4.6. If we set s=1 in Theorem 4.3, then we obtain the following inequality
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qb−a(1[r1+1]q)1r1[(x−a)2(|aDqf(x)|p1+q|aDqf(a)|p1[2]q)1p1+(b−x)2(|bDqf(x)|p1+q|bDqf(b)|p1[2]q)1p1] |
which is proved by Budak et al. in [16].
Corollary 4.3. If we assume |aDqf(x)|, |bDqf(a)|≤M in Theorem 4.3, then we have the following quantum Ostrowski's type inequality for s-convex functions in the second sense:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤Mqb−a(1[r1+1]q)1r1(2[s+1]q)1p1[(x−a)2+(b−x)2]. | (4.15) |
Remark 4.7. In Corollary 4.3, if we set s=1, then we recapture the following inequality
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qMb−a(1[r1+1]q)1r1[(x−a)2+(b−x)2] |
which is obtained by Budak et al. in [16].
Remark 4.8. In Corollary 4.3, if we take the limit as q→1−, then Corollary 4.3 reduces to [1,Theorem 3].
Theorem 4.4. Assume that the mapping f:I⊂R+→R is differentiable and a,b∈I with a<b. If |aDqf|p1 and |bDqf|p1, p1≥1 are s-convex mappings in the second sense, then the following inequality holds:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(b−a)(q2[2]q[3]q)1−1p1×[(x−a)2((1[s+2]q−1[s+3]q)|aDqf(x)|p1+Θ2|aDqf(a)|p1)1p1+(b−x)2((1[s+2]q−1[s+3]q)|bDqf(x)|p1+Θ2|bDqf(b)|p1)1p1]+q(b−a)(1[3]q)1−1p1[(x−a)2(1[s+3]q|aDqf(x)|p1+Θ3|aDqf(a)|p1)1p1+(b−x)2(1[s+3]q|bDqf(x)|p1+Θ3|bDqf(b)|p1)1p1], | (4.16) |
where
Θ2=∫10t(1−t)s+1dqt,Θ3=∫10t2(1−t)sdqt. |
Proof. From Lemma 4.1, using properties of the modulus and improved power mean inequality (see [33]), we have
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(x−a)2b−a1∫0t|aDqf(tx+(1−t)a)|dqt+q(b−x)2b−a1∫0t|bDqf(tx+(1−t)b)|dqt≤q(x−a)2b−a(1∫0t(1−t)dqt)1−1p1(1∫0t(1−t)|aDqf(tx+(1−t)a)|p1dqt)1p1+q(x−a)2b−a(1∫0t2dqt)1−1p1(1∫0t2|aDqf(tx+(1−t)a)|p1dqt)1p1+q(b−x)2b−a(1∫0t(1−t)dqt)1−1p1(1∫0t(1−t)|bDqf(tx+(1−t)b)|p1dqt)1p1+q(b−x)2b−a(1∫0t2dqt)1−1p1(1∫0t2|bDqf(tx+(1−t)b)|p1dqt)1p1. | (4.17) |
Since the mappings |aDqf|p1 and |bDqf|p1 are s -convex in the second sense, therefore
(1∫0t(1−t)dqt)1−1p1(1∫0t(1−t)|aDqf(tx+(1−t)a)|p1dqt)1p1≤(q2[2]q[3]q)1−1p1((1[s+2]q−1[s+3]q)|aDqf(x)|p1+Θ2|aDqf(a)|p1)1p1, | (4.18) |
(1∫0t2dqt)1−1p1(1∫0t2|aDqf(tx+(1−t)a)|p1dqt)1p1≤(1[3]q)1−1p1(1[s+3]q|aDqf(x)|p1+Θ3|aDqf(a)|p1)1p1, | (4.19) |
(1∫0t(1−t)dqt)1−1p1(1∫0t(1−t)|bDqf(tx+(1−t)b)|p1dqt)1p1≤(q2[2]q[3]q)1−1p1((1[s+2]q−1[s+3]q)|bDqf(x)|p1+Θ2|bDqf(b)|p1)1p1 | (4.20) |
and
(1∫0t2dqt)1−1p1(1∫0t2|bDqf(tx+(1−t)b)|p1dqt)1p1≤(1[3]q)1−1p1(1[s+3]q|bDqf(x)|p1+Θ3|bDqf(b)|p1)1p1. | (4.21) |
We obtain the resultant inequality (4.16) by putting (4.18), (4.19), (4.20) and (4.21) in (4.17).
Corollary 4.4. If we assume |aDqf(x)|, |bDqf(x)|≤M in Theorem 4.4, then we have the following quantum Ostrowski's type inequality for s-convex functions in the second sense:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qM(b−a)[(q2[2]q[3]q)1−1p1[(x−a)2+(b−x)2](1[s+2]q−1[s+3]q+Θ2)1p1+(1[3]q)1−1p1[(x−a)2+(b−x)2](1[s+3]q+Θ3)1p1]. | (4.22) |
Corollary 5. In Corollary 4.4, if we set s=1, then we obtain the following new Ostrowski type inequality:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qM(b−a)[(q2[2]q[3]q)1−1p1[(x−a)2+(b−x)2](q2[2]q[3]q)1p1+(1[3]q)1−1p1[(x−a)2+(b−x)2](1[3]q)1p1]. |
Theorem 4.5. Assume that the mapping f:I⊂R+→R is differentiable and a,b∈I with a<b. If |aDqf|p1 and |bDqf|p1, p1>1 are s-convex mappings in the second sense, then the following inequality holds:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤qb−a(1[r1+1]q−1[r1+2]q)1r1×[(x−a)2((1[s+1]q−1[s+2]q)|aDqf(x)|p1+1[s+2]q|aDqf(a)|p1)1p1+(b−x)2((1[s+1]q−1[s+2]q)|bDqf(x)|p1+1[s+2]q|bDqf(b)|p1)1p1]+qb−a(1[r1+1]q)1r1×[(x−a)2(1[s+2]q|aDqf(x)|p1+Θ1|aDqf(a)|p1)1p1+(b−x)2(1[s+2]q|bDqf(x)|p1+Θ1|bDqf(b)|p1)1p1], | (4.23) |
where 1r1+1p1=1.
Proof. From Lemma 4.1, using properties of the modulus and Hölder's İşcan inequality (see [29]), we have
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤q(x−a)2b−a1∫0t|aDqf(tx+(1−t)a)|dqt+q(b−x)2b−a1∫0t|bDqf(tx+(1−t)b)|dqt≤q(x−a)2b−a(1∫0(1−t)tr1dqt)1r1(1∫0(1−t)|aDqf(tx+(1−t)a)|p1dqt)1p1+q(x−a)2b−a(1∫0tr1+1dqt)1r1(1∫0t|aDqf(tx+(1−t)a)|p1dqt)1p1+q(b−x)2b−a(1∫0(1−t)tr1dqt)1r1(1∫0(1−t)|bDqf(tx+(1−t)b)|p1dqt)1p1+q(b−x)2b−a(1∫0tr1+1dqt)1r1(1∫0t|bDqf(tx+(1−t)b)|p1dqt)1p1. | (4.24) |
Since the mappings |aDqf|p1 and |bDqf|p1 are s -convex in the second sense, therefore
(1∫0(1−t)tr1dqt)1r1(1∫0(1−t)|aDqf(tx+(1−t)a)|p1dqt)1p1≤(1[r1+1]q−1[r1+2]q)1r1×((1[s+1]q−1[s+2]q)|aDqf(x)|p1+1[s+2]q|aDqf(a)|p1)1p1, | (4.25) |
(1∫0tr1+1dqt)1r1(1∫0t|aDqf(tx+(1−t)a)|p1dqt)1p1≤(1[r1+2]q)1r1(1[s+2]q|aDqf(x)|p1+Θ1|aDqf(a)|p1)1p1, | (4.26) |
(1∫0(1−t)tr1dqt)1r1(1∫0(1−t)|bDqf(tx+(1−t)b)|p1dqt)1p1≤(1[r1+1]q−1[r1+2]q)1r1×((1[s+1]q−1[s+2]q)|bDqf(x)|p1+1[s+2]q|bDqf(b)|p1)1p1 | (4.27) |
and
(1∫0tr1+1dqt)1r1(1∫0t|bDqf(tx+(1−t)b)|p1dqt)1p1≤(1[r1+2]q)1r1(1[s+2]q|bDqf(x)|p1+Θ1|bDqf(b)|p1)1p1. | (4.28) |
We obtain the resultant inequality (4.23) by putting (4.25), (4.26), (4.27) and (4.28) in (4.24).
Corollary 4.6. If we assume |aDqf(x)|, |bDqf(x)|≤M in Theorem 4.5, then we have the following quantum Ostrowski's type inequality for s-convex functions in the second sense:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤Mqb−a×[(1[r1+1]q−1[r1+2]q)1r1[(x−a)2+(b−x)2](1[s+1]q)1p1+(1[r1+1]q)1r1[(x−a)2+(b−x)2](1[s+2]q+Θ1)1p1]. | (4.29) |
Corollary 4.7. In Corollary 4.6, if we use s=1, then we obtain the following new Ostrowski type inequality:
|f(x)−1b−a[x∫af(t)adqt+b∫xf(t)bdqt]|≤Mqb−a(1[2]q)1p1[(x−a)2+(b−x)2]×[(1[r1+1]q−1[r1+2]q)1r1+(1[r1+1]q)1r1]. |
For arbitrary positive numbers κ1,κ2 (κ1≠κ2), we consider the means as follows:
1.The arithmetic mean
A=A(κ1,κ2)=κ1+κ22. |
2.The logarithmic mean
Lpp=Lpp(κ1,κ2)=κp+12−κp+11(p+1)(κ2−κ1). |
Proposition 5.1. For 0<a<b and 0<q<1, the following inequality is true:
|1s+1[As+1(a,b)−A(k1,k2)]|≤q(b−a)2[1[s+2]q{Lss(qa+b2+(1−q)a,a+b2)+Lss(qa+b2+(1−q)b,a+b2)}+2Θ1A(as,bs)], |
where
k1=(1−q)∞∑n=0qn(qna+b2+(1−qn)a)s+1,k2=(1−q)∞∑n=0qn(qna+b2+(1−qn)b)s+1. |
Proof. The inequality (4.2) in Theorem 4.1 with x=a+b2 for f(x)=xs+1s+1, where x>0 and s∈(0,1) leads to this conclusion.
Proposition 5.2. For 0<a<b and 0<q<1, the following inequality is true:
|1s+1[As+1(a,b)−A(k1,k2)]|≤Mq(b−a)2[1[s+2]q+Θ1]. |
Proof. The inequality (4.6) in Corollary 4.1 with x=a+b2 for f(x)=xs+1s+1, where x>0 and s∈(0,1) leads to this conclusion.
Proposition 5.3. For 0<a<b and 0<q<1, the following inequality is true:
|1s+1[As+1(a,b)−A(k1,k2)]|≤q(b−a)2(1[2]q)1−1p1[(1[s+2]q|Lss(qa+b2+(1−q)a,a+b2)|p1+Θ1|as|p1)1p1+(1[s+2]q|Lss(qa+b2+(1−q)b,a+b2)|p1+Θ1|bs|p1)1p1]. |
Proof. The inequality (4.7) in Theorem 4.2 with x=a+b2 for f(x)=xs+1s+1, where x>0 and s∈(0,1) leads to this conclusion.
Proposition 5.4. For 0<a<b and 0<q<1, the following inequality is true:
|1s+1[As+1(a,b)−A(k1,k2)]|≤q(b−a)2(1[r1+1]q)1r1[(1[s+1]q(|Lss(qa+b2+(1−q)a,a+b2)|p1+|as|p1))1p1+(1[s+1]q(|Lss(qa+b2+(1−q)b,a+b2)|p1+|bs|p1))1p1]. |
Proof. The inequality (4.11) in Theorem 4.3 with x=a+b2 for f(x)=xs+1s+1, where x>0 and s∈(0,1) leads to this conclusion.
Proposition 5.5. For 0<a<b and 0<q<1, the following inequality is true:
|1s+1[As+1(a,b)−A(k1,k2)]|≤Mq(b−a)2(1[r1+1]q)1r1(2[s+1]q)1p1. |
Proof. The inequality (4.15) in Corollary 4.3 with x=a+b2 for f(x)=xs+1s+1, where x>0 and s∈(0,1) leads to this conclusion.
In this investigation, Hermite-Hadamard and Ostrowski type inequalities for s-convex mappings in the second sense are derived, by applying quantum integrals. It is also showed that the results established in this paper are potential generalization of the existing comparable results in the literature. As future directions, one can find similar inequalities for co-ordinated s-convex functions in the second sense.
This research was funded by King Mongkut's University of Technology North Bangkok. Contract no. KMUTNB-61-KNOW-015. The work of second author is partially supported by the National Natural Science Foundation of China (Grant No. 11971241).
The authors declare that they have no competing interest.
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