Abstract
In this paper, we use - and -integrals to establish some quantum Hermite–Hadamard–Fejér-type inequalities for -convex functions. By taking , our results reduce to classical results on Hermite–Hadamard–Fejér-type inequalities for -convex functions. Moreover, we give some examples for quantum Hermite–Hadamard–Fejér-type inequalities for -convex functions. Some results presented here for -convex functions provide extensions of others given in earlier works for convex and -convex functions.
Keywords:
Hermite–Hadamard–Fejér-type integral inequalities; η-convex function; quantum calculus; qa-integral; qb-integral MSC:
05A30; 26D10; 26D15; 26A51; 52A01
1. Introduction
Quantum calculus (sometimes called q-calculus) is known as the study of calculus with no limits. Note that q-calculus can be reduced to ordinary calculus if we stipulate that limit q tends to 1. It was first studied by the famous mathematician Euler (1707–1783). In 1910, F. H. Jackson [1] determined the definite q-integral known as the q-Jackson integral. Quantum calculus has many applications in several mathematical areas such as combinatorics, number theory, orthogonal polynomials, basic hypergeometric functions, mechanics, quantum theory and theory of relativity; see, for instance, refs. [2,3,4,5,6,7] and the references therein. The book by V. Kac and P. Cheung [8] covers the fundamental knowledge and basic theoretical concepts of quantum calculus.
In 2013, J. Tariboon and S. K. Ntouyas [9,10] defined the -derivative and -integral of a continuous function on finite intervals and proved some of its properties. In 2020, S. Bermudo, P. Korus and J. E. Napoles Valdes [11] defined the -derivative and -integral of a continuous function on finite intervals. Many well-known integral inequalities such as Hölder, Hermite–Hadamard, trapezoid, Ostrowski, Cauchy–Bunyakovsky–Schwarz, Grüss and Grüss–Čebyšev inequalities have been studied in the concept of q-calculus. Based on these results, there are many outcomes concerning q-calculus.
The Hermite–Hadamard–Fejér integral inequality has been proven in [12] as follows:
Theorem 1 ([12]).
Let be a convex function. Then
where is integrable and symmetric about , i.e., .
Recently, there have been many works about quantum integral inequalities, especially quantum Hermite–Hadamard–Fejér-type inequalities. Interested readers can see [13,14,15,16,17,18] and the references therein.
Let I be an interval in the real line . Consider for appropriate .
Definition 1.
A function is called convex with respect to η (η-convex), if
for all and .
In fact, the above definition geometrically says that if a function is -convex on I, then it is a graph between any and is on or under the path starting from and ending at . If should be the endpoint of the path for every , then we have and the function reduces to a convex one. Note that by taking in (2), we obtain for any and , which implies that for any . Also, if we take in (2), we obtain
for any
There are simple examples about the -convexity of a function.
Example 1.
- (i)
- Consider a function defined as:and define a bifunction η as , for all It is not hard to check that f is an η-convex function but not a convex one.
- (ii)
- Define a function asand a bifunction asThen f is an η-convex function but is not convex.
In 2017, M. R. Delavar and M. De La Sen [19] presented some generalizations of Fejér-type inequalities related to -convex functions, which improve the right and left sides of (1), respectively.
This paper generalizes and extends some well-known results for Hermite–Hadamard–Fejér integral inequality for -convex functions via quantum integrals. The results presented here would extend some of those in the existing literature.
2. Preliminaries
Now, we recall the following well-known basic concepts of quantum calculus on finite intervals, which are essential in proving our main results.
Let be an interval and be a constant. The - and -derivative of a function at a point is defined as follows:
Definition 2 ([11]).
Let be a continuous function and let . Then the -derivative of f on at x is defined as
It is obvious that
Analogously, the -derivative of f on at x is defined as
It is obvious that
A function f is - and -differentiable on if and exist for all . Also, if in (3) or if in (4), then , where is the q-derivative of the function f defined as
Let us elaborate on the above definitions with the help of examples.
Example 2.
Let and . Then for , we have
Note that when , we have
Moreover, for , we have
Note that when , we have
J. Tariboon and S. K. Ntouyas [9] defined the -integral as follows:
Definition 3 ([9]).
Let be a continuous function. Then the q-integral on is defined as:
for .
S. Bermudo, P. Korus and J. E. Napoles Valdes [11] defined the -integral as follows:
Definition 4 ([11]).
Let be a continuous function. Then the q-integral on is defined as:
for .
If in (5) or in (6), then we have the classical q-integral. Also, taking and in (5), we obtain
Similarly, if and in (6), then
Example 3.
Let . Define a function by for ; we have
and
For some other useful details regarding quantum calculus, interested readers are referred to [8,11].
The following simple lemma is required.
Lemma 1.
Assume that . Then
- (i)
- ;
- (ii)
- If , then .
Proof.
Assertions (i) and (ii) are consequences of this fact
□
Lemma 2.
Let be - and -integrable on and symmetric about . Then
Proof.
Since g is symmetric, we obtain
Therefore,
□
3. Main Results
In this section, we obtain some new quantum analogues of Hermite–Hadamard–Fejér-type inequalities for -convex functions, which improve the right and left sides of Hermite–Hadamard–Fejér-type inequalities.
Theorem 2.
Let be a q-integrable on and an η-convex function with η bounded from above on . If is a q-integrable on , then the following inequalities hold:
and
Proof.
Since f is an -convex function on , we have
for all .
We put t instead of in (10) and then add that inequality with (10); we obtain
Equivalently,
In (11), we replace a with b; we obtain
From inequalities (11), (12) and using assertion (i) of Lemma 1, we have
Now, if in (10) we put a instead of b and add that inequality with (10), then
for all , which is equivalent to
If we change a with b and t with in (10), then add that inequality with (10), we obtain
for all .
Equivalently,
By multiplying inequality (13) with and then -integrating with respect to t over , we obtain
That is,
which is inequality (7).
From this theorem, we can state the following corollary.
Corollary 1.
Let be a q-integrable on and η-convex function with η bounded from above on . If is a q-integrable on , then the following inequalities hold:
and
Proof.
Theorem 3.
Let be a q-integrable on and η-convex function with η bounded from above on . If is a q-integrable on and symmetric about , then the following inequalities hold:
and
Proof.
From Corollary 1, Theorem 3 and Lemma 2, we can state the following corollary.
Corollary 2.
Let be a q-integrable on and η-convex function with η bounded from above on . If is a q-integrable on and symmetric about , then the following inequalities hold:
and
Proof.
Remark 1.
Inequalities (19)–(22) give a refinement for the right side of Theorem 1 in quantum integral inequalities. The following statements hold:
- (i)
- If , then Theorems 2 and 3 reduce to ([19], Theorem 2.1);
- (ii)
- If and , then we recapture the right side of Theorem 1.
Theorem 4.
Let be a q-integrable on and η-convex function with η bounded from above on . If is a q-integrable on , then the following inequalities hold:
Proof.
From this theorem, we can state the following corollary.
Corollary 3.
Let be a q-integrable on and η-convex function with η bounded from above on . If is a q-integrable on , then the following inequalities hold:
Proof.
Theorem 5.
Let be a q-integrable on and η-convex function with η bounded from above on . If is a q-integrable and symmetric on , then the following inequalities hold:
Proof.
Assume that g is symmetric on ; it is clear that
and
We applied these relations to Theorem 4; we completed the proof. □
Remark 2.
Inequality (26) gives a refinement for the left side of Theorem 1 in quantum integral inequalities. The following statements hold:
- (i)
- If , then Theorems 4 and 5 reduce to ([19], Theorem 2.3);
- (ii)
- If and , then we recapture the left side of Theorem 1.
4. Example
In this section, we give some examples to demonstrate our main results.
Example 4.
Define functions by and by . Consider a bifunction as
Then f is an η-convex function.
The right side of inequality (7) becomes
and the right side of the inequality (8) becomes
We use Matlab software to calculate the left term and right term, as shown in Figure 1 and Figure 2, which demonstrates the results described in inequalities (7) and (8) of Theorem 2.
Figure 1.
Plot illustration for the left term and the right term for inequality (7).
Figure 2.
Plot illustration for the left term and the right term for inequality (8).
From Theorem 2, the left side of inequality (9) becomes
and the right side of inequality (9) becomes
We use Matlab software to calculate the left term and right term, as shown in Figure 3, which demonstrates the results described in inequality (9) of Theorem 2.
Figure 3.
Plot illustration for the left term and the right term for inequality (9).
Example 5.
Define functions by and by . Consider a bifunction as
Then f is an η-convex function and g is symmetric about .
From Theorem 3, the left side of inequalities (19) becomes
and the right side of inequality (19) becomes
We use Matlab software to calculate the left term and right term, as shown in Figure 4, which demonstrates the results described in inequality (19) of Theorem 3.
Figure 4.
Plot illustration for the left term and the right term for inequality (19).
From Theorem 3, the left side of inequalities (20) becomes
and the right side of inequality (20) becomes
We use Matlab software to calculate the left term and right term, as shown in Figure 5, which demonstrates the result described in inequality (20) of Theorem 3.
Figure 5.
Plot illustration for the left term and the right term for inequality (20).
5. Conclusions
The convexity of a function is a basis for many inequalities in mathematics. It should be noted that in new problems related to convexity, a general idea of the convex function is required to obtain relevant results. One of these overviews is the concept of the -convex function, which can be summarized by many inequalities associated with convex functions, especially the famous Fejér inequality, by evaluating the difference between the left and middle terms and between the right and middle terms of this inequality. Moreover, we derived some new quantum analogues of Hermite–Hadamard–Fejér-type inequalities for -convex functions. It is expected that this paper may stimulate further research in this field.
Author Contributions
Conceptualization, K.N. and H.B.; investigation, N.A., K.N. and H.B.; formal analysis, N.A., K.N. and H.B.; funding acquisition, K.N.; software, N.A. and K.N.; validation, N.A., K.N. and H.B.; visualization, K.N. and H.B.; writing—original draft, N.A. and K.N.; writing—review and editing, K.N. All authors have read and agreed to the published version of the manuscript.
Funding
This work has received scholarship under the Post-Doctoral Training Program from Khon Kaen University, Thailand (Grant no. PD2565-02-05).
Data Availability Statement
Not applicable.
Conflicts of Interest
The authors declare no conflict of interest.
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