Citation: Yousaf Khurshid, Muhammad Adil Khan, Yu-Ming Chu. Conformable integral version of Hermite-Hadamard-Fejér inequalities via η-convex functions[J]. AIMS Mathematics, 2020, 5(5): 5106-5120. doi: 10.3934/math.2020328
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A real-valued function h:I→R is said to be a convex (concave) function of the interval I⊆R if the inequality
h(λκ1+(1−λ)κ2)≤(≥)λh(κ1)+(1−λ)h(κ2) |
takes place whenever κ1,κ2∈I and λ∈[0,1].
It is well known that convex (concave) function plays an important role in mathematics due to convexity (concavity) is widely used in all branches of pure and applied mathematics [1,2,3,4,5,6,7]. Recently, the generalizations, extensions and invariants for the convex (concave) function have attracted the attention of many researchers, for instance, the quasi-convex function [8], harmonic convex function [9,10], strongly convex function [11,12,13], two-parameter Hölder mean convex function [14,15], exponentially convex function [16,17], GG and GA convex functions [18], and s-convex function [19,20]. In particular, many inequalities can be found in the literature [21,22,23,24,25,26,27,28,29,30,31,32,33,34,35,36] by use of properties of the convex (concave) function.
Let h:I→R be a convex (concave) function. Then the well known HH (Hermite-Hadamard) inequality [37,38,39] states that the double inequality
h(κ1+κ22)≤(≥)1κ2−κ1∫κ2κ1h(x)dx≤(≥)h(κ1)+h(κ2)2 | (1.1) |
is valid for all κ1,κ2∈I with κ1≠κ2.
Fejér generalized the HH inequality (1.1) to the Hermite-Hadamard-Fejér inequality (1.2) as follows:
h(κ1)+h(κ2)2∫κ2κ1g(x)dx≥(≤)1κ2−κ1∫κ2κ1g(x)h(x)dx≥(≤)h(κ1+κ22)∫κ2κ1g(x)dx | (1.2) |
if h:[κ1,κ2]→R is a convex (concave) function and g:[κ1,κ2]→R+ is symmetric with respect to (κ1+κ2)/2.
The following definition for the η-convex function was introduced by Eshaghi Gordji et al. in [40].
Definition 1.1. (See [40]) Let κ1,κ2∈R with κ1<κ2, h:[κ1,κ2]→R be a real-valued function and η:h([κ1,κ2])×h([κ1,κ2])→R be a two bivariate real-valued function. Then h is said to be η-convex (or convex with respect to η) if the inequality
h[sμ1+(1−s)μ2]≤h(μ2)+sη[h(μ1),h(μ2)] | (1.3) |
holds for all μ1,μ2∈[κ1,κ2] and s∈[0,1].
Let η(μ1,μ2)=μ1−μ2 in (1.3). Then Definition 1.1 reduces to the definition of usual convex function.
Eshaghi Gordji et al. [40] established a HH type inequality for the η-convex function.
Theorem 1.1. (See [40]) Let κ1,κ2∈R with κ1<κ2, h:[κ1,κ2]→R be a real-valued function and η:h([κ1,κ2])×h([κ1,κ2])→R be a two bivariate bounded real-valued function. Then one has
h(κ1+κ22)−Mη2≤1κ2−κ1κ2∫κ1h(x)dx |
≤h(κ1)+h(κ2)2+η(h(κ1),h(κ2))+η(h(κ2),h(κ1))4 |
≤h(κ1)+h(κ2)2+Mη2 | (1.4) |
if h is η-convex, where Mη is the upper bound of η on h([κ1,κ2])×h([κ1,κ2]).
Let 0<β≤1, r>0 and g:[0,∞)→R be a real-valued function. Then the conformable derivative Dβ(g)(r) of order β is defined by
Dβ(g)(r)=dβg(r)dβr=limϵ→0g(r+ϵr1−β)−g(r)ϵ, | (1.5) |
g is said to be conformable differentiable at r if the limit of (1.5) exists and is finite. The conformal derivative at 0 is defined by Dβ(g)(0)=limr→0+Dβ(g)(r).
Let κ1,κ2,λ,c∈R be the constants, and h1 and h2 be differentiable at r>0. Then the following formulas can be found in the literature [41]
dβdβr(rλ)=λrλ−β,dβdβr(c)=0, |
dβdβr(κ1h1(r)+κ2h2(r))=κ1dβdβr(h1(r))+κ2dβdβr(h2(r)), |
dβdβr(h1(r)h2(r))=h1(r)dβdβr(h2(r))+h2(r)dβdβr(h1(r)), |
dβdβr(h1(r)h2(r))=h2(r)dβdβr(h1(r))−h1(r)dβdβr(h2(r))(h2(r))2, |
dβdβr(h1(h2(r)))=h′1(h2(r))dβdβr(h2(r)) |
if h1 differentiable at h2(r). In addition,
dβdβr(h1(r))=r1−βddr(h1(r)) |
if h1 is differentiable.
Let β∈(0,1] and 0≤κ1<κ2. Then the function g:[κ1,κ2]→R is said to be conformable integrable if
∫κ2κ1g(x)dβx=∫κ2κ1g(x)xβ−1dx |
exists and is finite. The set of all conformable integrable functions on [κ1,κ2] is denoted by Lβ([κ1,κ2]). Note that
Iκ1β(h1)(r)=Iκ11(rβ−1h1)=∫rκ1h1(x)x1−βdx |
for all β∈(0,1], where the integral is the usual Riemann improper integral.
For the theory and applications of the conformable integrals and derivatives we recommend the readers to refer the literature [42,43,44,45,46,47,48,49,50].
Anderson [51] established the conformable integral version of the HH type inequality
βκβ2−κβ1∫κ2κ1h(x)dβx≤h(κ1)+h(κ2)2 |
if β∈(0,1] and h:[κ1,κ2]→R is conformable differentiable such that Dβ(h) is increasing. Moreover, if h is decreasing on [κ1,κ2], then
h(κ1+κ22)≤βκβ2−κβ1∫κ2κ1h(x)dβx. |
It is the aim of the article to establish new Hermite-Hadamard-Fejér type inequalities for the η-convex functions via conformable integrals.
Theorem 2.1. Let κ1,κ2∈R+ with κ1<κ2, h:[κ1,κ2]→R be an η-convex function and symmetric with respect to κ1+κ22, ξ:[κ1,κ2]→R be a nonnegative integrable function. Then the inequality
h(κ1+κ22)κ2∫κ1ξ(x)dβx−Mη2κ2∫κ1ξ(x)dβx≤κ2∫κ1h(x)ξ(x)dβx |
≤h(κ1)+h(κ2)2κ2∫κ1ξ(x)dβx+η(h(κ1),h(κ2))+η(h(κ2),h(κ1))4κ2∫κ1ξ(x)dβx |
≤h(κ1)+h(κ2)2κ2∫κ1ξ(x)dβx+Mη2κ2∫κ1ξ(x)dβx | (2.1) |
holds for any β∈(0,1] if η is bounded on h([κ1,κ2])×h([κ1,κ2]), where Mη is the upper bound of η on h([κ1,κ2])×h([κ1,κ2]).
Proof. Let s∈[0,1]. Then it follows from the η-convexity and symmetry of h that
h(κ1+κ22)=h(sκ1−sκ1+κ1+κ2+sκ2−sκ22) |
=h(sκ1+(1−s)κ2+sκ2+(1−s)κ12) |
≤h(sκ2+(1−s)κ1)+12η(h(sκ1+(1−s)κ2)),h(sκ2+(1−s)κ1) |
≤h(sκ2+(1−s)κ1)+12Mη. |
Let x=sκ2+(1−s)κ1. Then we get
h(κ1+κ22)κ2∫κ1ξ(x)dβx=(κ2−κ1)h(κ1+κ22)1∫0ξ(sκ2+(1−s)κ1)(sκ2+(1−s)κ1)β−1ds |
≤1∫0h(sκ2+(1−s)κ1)ξ(sκ2+(1−s)κ1)(κ2−κ1)(sκ2+(1−s)κ1)β−1ds |
+Mη21∫0ξ(sκ2+(1−s)κ1)(κ2−κ1)(sκ2+(1−s)κ1)β−1ds |
=κ2∫κ1h(x)ξ(x)dβx+Mη2κ2∫κ1ξ(x)dβx, |
which gives the proof of the first inequality of (2.1).
Next, we prove the second and third inequalities of (2.1). From the η-convexity of h we know that
h(sκ1+(1−s)κ2)≤h(κ2)+sη(h(κ1),h(κ2)) | (2.2) |
and
h(sκ2+(1−s)κ1)≤h(κ1)+sη(h(κ2),h(κ1)). | (2.3) |
Let x=sκ1+(1−s)κ2. Then from the symmetry of h, inequalities (2.2) and (2.3) lead to
κ2∫κ1h(x)ξ(x)xβ−1dx=(κ2−κ1)1∫0h(sκ1+(1−s)κ2)ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds |
≤(κ2−κ1)[h(κ2)+12η(h(κ1),h(κ2))]1∫0ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds | (2.4) |
and
κ2∫κ1h(x)ξ(x)xβ−1dx=(κ2−κ1)1∫0h(sκ1+(1−s)κ2)ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds |
=(κ2−κ1)1∫0h(sκ2+(1−s)κ1)ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds |
≤(κ2−κ1)[h(κ1)+12η(h(κ2),h(κ1))]1∫0ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds | (2.5) |
Adding (2.4) and (2.5), and letting x=sκ1+(1−s)κ2, we obtain
2κ2∫κ1h(x)ξ(x)dβx≤(κ2−κ1)(h(κ1)+h(κ2))1∫0ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds |
+(κ2−κ1)(η(h(κ1),h(κ2))+η(h(κ2),h(κ1)))21∫0ξ(sκ1+(1−s)κ2)(sκ1+(1−s)κ2)β−1ds |
and
κ2∫κ1h(x)ξ(x)dβx≤h(κ1)+h(κ2)2κ2∫κ1ξ(x)dβx+η(h(κ1),h(κ2))+η(h(κ2),h(κ1))4κ2∫κ1ξ(x)dβx |
≤h(κ1)+h(κ2)2κ2∫κ1ξ(x)dβx+Mη2κ2∫κ1ξ(x)dβx. |
Corollary 2.1. Let ξ(x)=1. Then inequality (2.1) becomes
h(κ1+κ22)−Mη2≤βκβ2−κβ1κ2∫κ1h(x)dβx |
≤h(κ1)+h(κ2)2+η(h(κ1),h(κ2))+η(h(κ2),h(κ1))4 |
≤h(κ1)+h(κ2)2+Mη2. |
In order to establish our main results, we need a key lemma which we present in this section.
Lemma 3.1. Let κ1,κ2∈R+ with κ1<κ2, and h:[κ1,κ2]→R be a differentiable function on (κ1,κ2) such that Dβ(h)∈Lβ([κ1,κ2]). Then the identity
h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx |
=(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κ1+sκ2)2β−1−κβ1((1−s)κ1+sκ2)β−1) |
×Dβ(h)((1−s)κ1+sκ2)s1−βdβs+∫10(((1−s)κ2+sκ1)2β−1−aβ2((1−s)κ2+sκ1)β−1) |
×Dβ(h)((1−s)κ2+sκ1)s1−βdβs]. |
holds for β∈(0,1].
Proof. Integration by parts, we have
∫10(((1−s)κ1+sκ2)2β−1−κβ1((1−s)κ1+sκ2)β−1)Dβ(h)((1−s)κ1+sκ2)ds |
+∫10(((1−s)κ2+sκ1)2β−1−κβ2((1−s)κ2+sκ1)β−1)Dβ(h)((1−s)κ2+sκ1)ds |
=∫10(((1−s)κ1+sκ2)β−κβ1)h′((1−s)κ1+sκ2)ds |
+∫10(((1−s)κ2+sκ1)β−κβ2)h′((1−s)κ2+sκ1)ds |
=[(((1−s)κ1+sκ2)β−κβ1)h((1−s)κ1+sκ2)κ2−κ1|10 |
−∫10β((1−s)κ1+κ2)β−1(κ2−a1)h((1−s)κ1+sκ2)κ2−κ1ds] |
+[(((1−s)κ2+sκ1)β−κβ2)h((1−s)κ2+sκ1)κ1−κ2|10 |
−∫10β((1−s)κ2+sκ1)β−1(κ1−κ2)h((1−s)κ2+sκ1)κ1−κ2ds] |
=[κβ2−κβ1κ2−κ1h(κ2)−βκ2−κ1∫κ2κ1h(x)dβx] |
+[κβ2−κβ1κ2−κ1h(κ1)−βκ2−κ1∫κ2κ1h(x)dβx] |
=κβ2−κβ1κ2−κ1(h(κ1)+h(κ2))−2βκβ2−κβ1∫κ2κ1h(x)dβx. |
Theorem 3.1. Let κ1,κ2∈R+ with κ1<κ2, and h:[κ1,κ2]→R be a differentiable function on (κ1,κ2) such that Dβ(h)∈Lβ([κ1,κ2]). Then the inequality
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(κβ−11κ2+κβ−12κ1+2κβ2−4κβ16)|h′(κ1)|+η(|h′(κ2)|,|h′(κ1)|) |
×(κβ−11κ2+κβ−12κ1+3κβ2−5κβ112)+|h′(κ2)|(κβ2−κβ12)+η(|h′(κ1)|,|h′(κ2)|)(κβ2−κβ16)] | (3.1) |
holds for β∈(0,1] if |h′| is η-convex.
Proof. Let y>0, φ1(y)=yβ−1 and φ2(y)=−yβ. Then we clearly see that both the functions φ1 and φ2 are convex. It follows from Lemma 3.1 and the convexity of φ1 and φ2 together with the η-convexity of |h′| that
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κ1+sκ2)β−κβ1)|h′((1−s)κ1+sκ2)|ds |
+∫10(((1−s)κ2+sκ1)β−κβ2)|h′((1−s)κ2+sκ1)|ds] |
=(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κ1+sκ2)β+1−1−κβ1)|h′((1−s)κ1+sκ2)|ds |
+∫10(κβ2−((1−s)κ2+sκ1)β)|h′((1−s)κ2+sκ1)|ds] |
≤(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κ1+sκ2)β−1((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|ds |
+∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|ds] |
≤(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|ds |
+∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|ds] |
≤(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1) |
×[|h′(κ1)|+sη(|h′(κ2)|,|h′(κ1)|)]ds+∫10(κβ2−((1−s)κβ2+sκβ1)) |
×[|h′(κ2)|+sη(|h′(κ1)|,|h′(κ2)|)]ds] |
and
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(κβ−11κ2+κβ−12κ1+2κβ2−4κβ16)|h′(κ1)| |
+η(|h′(κ2)|,|h′(κ1)|)(κβ−11κ2+κβ−12κ1+3κβ2−5κβ112) |
+|h′(κ2)|(κβ2−κβ12)+η(|h′(κ1)|,|h′(κ2)|)(κβ2−κβ16)]. |
Corollary 3.1. Let η(κ2,κ1)=κ2−κ1. Then inequality (3.1) reduces to
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(κβ−11κ2+κβ−12κ1+3aβ2−5κβ16)|h′(κ1)| |
+|h′(κ2)|(7κβ2−9κβ1+κβ−11κ2+κβ−12κ112)]. |
Theorem 3.2. Let q>1, κ1,κ2∈R+ with κ1<κ2, and h:[κ1,κ2]→R be a differentiable function on (κ1,κ2) such that Dβ(h)∈Lβ([κ1,κ2]). Then the inequality
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(A1(β))1−1q(|h′(κ1)|q(κβ−11κ2+κβ−12κ1+2κβ2−4κβ16) |
+η(|h′(κ2)|q,|h′(κ1)|q)(κβ−11κ2+κβ−12κ1+3κβ2−5κβ112))+(B1(β))1−1q |
×(|h′(κ2)|q(κβ2−κβ12)+η(|h′(κ1)|q,|h′(κ2)|q)(κβ2−κβ13))] |
takes place for β∈(0,1] if |h′|q is η-convex, where
A1(β)=2κβ1+κβ−11κ2+κβ−12κ1+2κβ2−6κβ16,B1(β)=κβ2−κβ12. |
Proof. We clearly see that
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κ1+sκ2)β−1((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|ds |
+∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|ds]. |
It follows from the power-mean inequality that
∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|ds |
≤(∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)ds)1−1q |
×(∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|qds)1q |
and
∫10(κβ2((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|ds |
≤(∫10(κβ2−((1−s)κβ2+sκβ1))ds)1−1q |
×(∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|qds)1q. |
Making use of the η-convexity of |h′|q and the facts that
∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)dt |
=A1(β)=2κβ1+κβ−11κ2+κβ−12κ1+2κβ2−6κβ16 |
and
∫10(κβ2−((1−s)κβ2+sκβ1))ds=B1(β)=κβ2−κβ12, |
we get
∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|qds |
≤∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)[|h′(κ1)|q+sη(|h′(κ2)|q,|h′(κ1)|q)]ds |
=|h′(κ1)|q∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)ds |
+η(|h′(κ2)|q,|h′(κ1)|q)∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)sds |
=|h′(κ1)|q(κβ−11κ2+κβ−12κ1+2κβ2−4κβ16)+η(|h′(κ2)|q,|h′(κ1)|q) |
×(κβ−11κ2+κβ−12κ1+3κβ2−5κβ112) |
and
∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|qds |
≤∫10(κβ2−((1−s)κβ2+sκβ1))[|h′(κ2)|q+sη(|h′(κ1)|q,|h′(κ2)|q)]ds |
=|h′(κ2)|q(κβ2−κβ12)+η(|h′(κ1)|q,|h′(κ2)|q)(κβ2−κβ13), |
which completes the proof of Theorem 3.2.
Corollary 3.2. Let η(κ2,κ1)=κ2−κ1. Then Theorem 3.2 leads to the conclusion that
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(A1(β))1−1q(|h′(κ1)|q(κβ−11κ2+κβ−12κ1+κβ2−3κβ16)+|h′(κ2)|q |
×(κβ−11κ2+κβ−12κ1+3κβ2−5κβ112))+(B1(β))1−1q(|h′(κ2)|q(κβ2−κβ16)+|h′(κ1)|q(κβ2−κβ13))]. |
Theorem 3.3. Let p,q>1 with 1/p+1/q=1, κ1,κ2∈R+ with κ1<κ2, and h:[κ1,κ2]→R be a differentiable function on (κ1,κ2) such that Dβ(h)∈Lβ([κ1,κ2]). Then the inequality
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(A1(β,p))1p(2|h′(κ1)|q+η(|h′(κ2)|q,|h′(κ1)|q)2)1q |
+(A2(β,p))1p(2|h′(κ2)|q+η(|h′(κ1)|q,|h′(κ2)|q)2)1q] |
is valid for β∈(0,1] if |h′|q is η-convex, where
A1(β,p)=∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)pds |
and
A2(β,p)=∫10(κβ2−((1−s)κβ2+sκβ1))pds. |
Proof. We clearly see that
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[∫10(((1−s)κ1+sκ2)β−1((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|ds |
+∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|ds]. |
Making use of Hölder inequality, we have
∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)|h′((1−s)κ1+sκ2)|ds |
≤(∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)pds)1p |
×(∫10|h′((1−s)κ1+sκ2)|qds)1q |
≤(∫10(((1−s)κβ−11+sκβ−12)((1−s)κ1+sκ2)−κβ1)pds)1p |
×(∫10|h′(κ1)|q+sη(|h′(κ2)|q,|h′(κ1)|q)ds)1q |
=(A1(β,p))1p(2|h′(κ1)|q+η(|h′(κ2)|q,|h′(κ1)|q)2)1q |
and
∫10(κβ2−((1−s)κβ2+sκβ1))|h′((1−s)κ2+sκ1)|ds |
≤(∫10(κβ2−((1−s)κβ2+sκβ1))pds)1p(|h′((1−s)κ2+sκ1)|qds)1q |
≤(∫10(κβ2−((1−s)κβ2+sκβ1))pds)1p(∫10(|h′(κ2)|q+sη(|h′(κ1)|q,|h′(κ2)|q))ds)1q |
=(A2(β,p))1p(2|h′(κ2)|q+η(|h′(κ1)|q,|h′(κ2)|q)2)1q. |
Corollary 3.3. Let η(κ2,κ1)=κ2−κ1. Then Theorem 3.3 leads to
|h(κ1)+h(κ2)2−βκβ2−κβ1∫κ2κ1h(x)dβx| |
≤(κ2−κ1)2(κβ2−κβ1)[(A1(β,p))1p(|h′(κ1)|q+|h′(κ2)|q2)1q+(A2(β,p))1p(|h′(κ2)|q+|h′(κ1)|q2)1q]. |
We have generalized the Hermite-Hadamard and Hermite-Hadamard-Fejér inequalities for convex functions to the η-convex functions via the conformable integral. Our obtained results are the improvements and generalizations of some previous known results, our ideas and approach may lead to a lot of follow-up research.
The authors would like to thank the anonymous referees for their valuable comments and suggestions, which led to considerable improvement of the article.
The work was supported by the Natural Science Foundation of China (Grant Nos. 61673169, 11971142, 11701176, 11626101, 11601485).
The authors declare no conflict of interest.
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