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Research article

Fractional version of the Jensen-Mercer and Hermite-Jensen-Mercer type inequalities for strongly h-convex function

  • Received: 13 July 2021 Accepted: 27 September 2021 Published: 18 October 2021
  • MSC : 35A23, 26E70, 34N05

  • In this paper we find further versions of generalized Hadamard type fractional integral inequality for k-fractional integrals. For this purpose we utilize the definition of h-convex function. The presented results hold simultaneously for variant types of convexities and fractional integrals.

    Citation: Fangfang Ma. Fractional version of the Jensen-Mercer and Hermite-Jensen-Mercer type inequalities for strongly h-convex function[J]. AIMS Mathematics, 2022, 7(1): 784-803. doi: 10.3934/math.2022047

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  • In this paper we find further versions of generalized Hadamard type fractional integral inequality for k-fractional integrals. For this purpose we utilize the definition of h-convex function. The presented results hold simultaneously for variant types of convexities and fractional integrals.



    Convex functions and mathematical inequalities play vital role in the advancement of several fields of pure and applied sciences. Various inequalities for convex and related functions have been studied in recent decades, also their variants in fractional calculus are analyzed, see [1,2,3,4,5].

    The employment of fractional integral operators for establishing the generalized versions of classical inequalities become a fashion in the study of mathematical inequalities. In this regard the most celebrated inequality called Hadamard inequality has been studied extensively for fractional integral operators. The presence of Mittag-Leffler function in fractional integral operators produces interesting fractional integral inequalities.

    The purpose of this paper is to present new Hadamard type inequalities for k-fractional integrals of strongly h-convex functions.

    Let f[ϕ,φ] then the Riemann-Liouville fractional integrals Jεϕ+f and Jεφf of order ε with ε>0, 0 ϕ<φ are defined by [6]:

    (Jεϕ+)f(v)=1Γ(ε)vϕ(vt)ε1f(t)dt(v>ϕ), (1.1)

    and

    (Jεφ)f(v)=1Γ(ε)φv(tv)ε1f(t)dt(v<φ). (1.2)

    respectively, where Γ(ε)=0ettϕ1dt is the Gamma function and (J0ϕ+)f(v)=(J0φ)f(v)=f(v).

    In [7], Jarad et al. defined the new fractional integral operator as follows:

    δϕJεt(v)=1Γ(δ)vϕ((vϕ)ε(tϕ)εε)δ1f(t)(tϕ)1εdt, (1.3)

    and

    δJεφt(v)=1Γ(δ)φv((φv)γ(φt)εε)δ1f(t)(φt)1εdt. (1.4)

    Note that, by taking ϕ = 0 and ε0, the new conformable fractional integral operator coincides with the generalized fractional integrals [8], by taking ϕ = 0 and ε = 1, the (1.3) becomes Riemann-Liouville fractional operator (1.1). Furthermore, by taking φ = 0 and ε = 1, the (1.4) reduces to the Riemann-Liouville.

    The generalized k-fractional conformable integrals [9] are defined as follows:

    δkJεϕ+t(v)=1kΓk(δ)vϕ((vϕ)ε(tϕ)εε)δk1f(t)(tϕ)1εdt, (1.5)

    and

    δkJεφt(v)=1kΓk(δ)φv((φv)ε(φt)γε)δk1f(t)(φt)1εdt. (1.6)

    If k > 0, then the k-Gamma function Γk is defined as [10]:

    Γk(ε)=limmm!km(mk)εk1(ε)m,k. (1.7)

    If Re (ε>0), then k-Gamma function in integral form is defined as

    Γk(ε)=0expϕkkϕε1dϕ

    with εΓk(ε)=Γk(ε+k).

    Let f : I R R be a convex function. Then

    f(ϕ+φ2)1φϕφϕf(t)dtf(ϕ)+f(φ)2.

    holds ϕ,φI with ϕφ and is known as Hermite-Hadamard inequality. The above inequality is reversed, if f is a concave function on I, see [11,12,13,14,15].

    In [16], the following generalization of Hermite-Hadamard inequality for strongly h-convex function is established:

    Let f:IRR is Lebesgue integrable and strongly h-convex function with modulus c >0. If h : (0, 1)(0,) be a given function. Then

    12h(12)[f(u+v2)+c12(vu)2]1vuvuf(x)dx(f(u)+f(v))10h(t)dtc6(vu)2.

    holds u, v I, u < v.

    Some further interesting extensions and refinements of the Hermite-Hadamard inequalities for strongly h-convex mappings have been widely studied in the literature, see [17]. The other well known inequality is Jensen inequality and different variants of Jensen-Mercer inequalities are present in literature, see [18,19,20,21].

    In this paper we find further versions of generalized Hadamard type fractional integral inequality for k-fractional integrals. For this purpose we utilize the definition of h-convex function.

    Next, we recall some basic definitions which will be used in the present article:

    The gamma function is denoted by Γ(.) and is defined as follows:

    Γ(τ)=0ettτ1dt,τ>0,

    The beta function is denoted by β and is defined as follows:

    β(x,y)=10tx1(1t)y1dt,

    where x,y,q are positive real numbers.

    The L1[a,b] is a class of all real-valued functions integrable in [a,b].

    Further, we give definitions of convex and related functions which are useful to understand the inequalities established in this work.

    Definition 2.1. [23] A function f:[a,b]R is said to be convex if

    f(tx+(1t)y)tf(x)+(1t)f(y),x,y[a,b],t[0,1]. (2.1)

    holds. If the inequality in (2.1) is reversed, then f is called concave function.

    Definition 2.2. [24,25] Let I(0,) be an interval and pR{0}. Then a function f:IR is said to be p-convex, if

    f((tap+(1t)bp)1p)tf(a)+(1t)f(b). (2.2)

    holds for a,bI and t[0,1]. If the inequality in (2.2) is reversed, then f is called p-concave function.

    Definition 2.3. [23] Let I,J be intervals in R, (0,1)J and h:JR be a non-negative function and h0. A function f:IR is said to be an h-convex, if

    f(tx+(1t)y)h(t)f(x)+h(1t)f(y). (2.3)

    holds for x,yI and t(0,1). If the inequality in (2.3) is reversed, then f is called h-concave function.

    Definition 2.4. [26] Let h:J(0,1)R be a positive function. Let I(0,) be an interval and pR{0}. A function f:IR is said to be (p, h)-convex, if

    f((tap+(1t)bp)1p)h(t)f(a)+h(1t)f(b). (2.4)

    holds for a,bI and t[0,1]. If the inequality in (2.4) is reversed, then f is called (p, h)-concave function.

    Definition 2.5. A function h : IR R is called superadditive function if

    h(u+v)h(u)+h(v). (2.5)

    u, v I.

    Definition 2.6. [27] Let h:J(0,1)R be a positive function and I(0,) be an interval. A function f:IR R is said to be strongly convex function with modulus c, u, v I and t[0,1] if the following inequality holds

    f(tu+(1t)v)tf(u)+1tf(v)ct(1t)(uv)2. (2.6)

    Definition 2.7. [16] Let h:J(0,1)R be a positive function and I(0,) be an interval. A function f:IR R is said to be strongly convex function with modulus c, u, v I and t[0,1] if the following inequality holds

    f(tu+(1t)v)h(t)f(u)+h(1t)f(v)ct(1t)(uv)2. (2.7)

    Our main purpose of this section is to prove the Jensen-Mercer inequality for strongly h-convex function. To present Jensen-Mercer inequality first we will prove the following lemma:

    Let 0<u1u2...un be real numbers and let tj(1jn) be positive weights associated with these uj and nJ=1uj = 1. let h:I R be a non negative function defined over an interval IR such that (0,1)I.

    Lemma 3.1. Let f:I R be a strongly h-convex function with modulus c > 0, then

    f(u1+unuj)M(f(u1)+f(un))f(uj)2ct(1t)(u1un)2. (3.1)

    for any ujI,(1jn) and for all t(0,1), where M=sup{h(t):t(0,1)}.

    Proof. Write vj=u1+unuj. Then u1+un=uj+vj so that the pairs u1, un and uj, vj posses the same mid point. Since that is the case, there exist a t such that

    uj=tu1+(1t)unandvj=(1t)u1+tun.

    where 0t1 and 1jn. Then, applying strongly h-convexity of f

    f(vj)=f((1t)u1+tun)h(1t)f(u1)+h(t)f(un)ct(1t)(u1un)2=h(1t)f(u1)+h(t)f(un)+h(t)f(u1)+h(1t)f(un)(h(t)f(u1)+h(1t)f(un)ct(1t)(u1un)2)2ct(1t)(u1un)2=(h(t)+h(1t))(f(u1)+f(un))(h(t)f(u1)+h(1t)f(un)ct(1t)(u1un)2)2ct(1t)(u1un)2(h(t)+h(1t))(f(u1)+f(un))f(tu1+(1t)un)2ct(1t)(u1un)22M(f(u1)+f(un))f(uj)2ct(1t)(u1un)2M(f(u1)+f(un))f(uj)2ct(1t)(u1un)2.

    where M=sup{h(t):t(0,1)} and since vj=u1+unuj, then

    f(u1+unuj)M(f(u1)+f(un))f(uj)2ct(1t)(u1un)2.

    This completes the proof.

    Remark 3.2. 1. Taking M = sup {h(t):t(0,1)} = 1 and c = 0 in Lemma 3.1, we get Lemma 1.3 of [20].

    2. Taking c = 0 in Lemma 3.1, we get Lemma 3.1 of [18].

    3. Taking M = sup {h(t):t(0,1)} = 1 in Lemma 3.1, we get Lemma 2.2 of [19].

    Theorem 3.3. Let f:IRR be a strongly h-convex function with modulus c>0 and 0<u1u2...un be real numbers in I. If tj(1jn) be positive numbers such that nj=1tj=1 and ˉu=nj=1tjuj. Then

    f(u1+unnj=1tjuj)M(f(u1)+f(un))nj=1h(tj)f(uj)c(2nj=1h(tj)t(1t)(u1un)2+nj=1tj(ujˉu)2), (3.2)

    where M=sup{h(t):t(0,1)}.

    Proof. Since nj=1tj = 1 we have

    f(u1+unnj=1tjuj)=f(nj=1tj(u1+unuj))nj=1h(tj)f(u1+unuj)cnj=1tj(ujˉu)2.

    By using Lemma 3.1, we have

    f(u1+unnj=1tjuj)nj=1h(tj)f(u1+unuj)cnj=1tj(ujˉu)2nj=1h(tj)[M(f(u1)+f(un))f(uj)2ct(1t)(u1un)2]cnj=1tj(ujˉu)2M(f(u1)+f(un))nj=1h(tj)f(uj)c(2nj=1h(tj)t(1t)(u1un)2+nj=1tj(ujˉu)2).

    This completes the proof.

    Remark 3.4. 1. Taking c=0 in Theorem 3.3, we get Theorem 3.2 of [18].

    2. Taking h(t)=t and M = sup {h(t):t(0,1)} = 1 in Theorem 3.3, we get Theorem 2.2 of [19].

    3. Taking c=0, h(t)=t and M = sup {h(t):t(0,1)} = 1 in Theorem 3.3, we get Theorem 1.2 of [20]).

    Theorem 3.5. Assume f:IR R be a strongly h-convex function with modulus c > 0 and ϕ,φI with ϕ<φ. If h is a super-additive function and take ε,δ> 0. Then

    f(ϕ+φu+v2)h(12)2εδkεδkΓk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}c(14)(δkβ(δk,2ε+1))(uv)2h(12)2M[f(ϕ)+f(φ)]h(12)h(1)[f(u)+f(v)]c(12h(12)(1δkβ(δk,2ε+1))(uv)2+14(δkβ(δk,2ε+1))(uv)2). (3.3)

    holds u, v [ϕ,φ], where M = sup {h(t):t(0,1)}.

    Proof. Since f is strongly h-convex function then we write

    f(ϕ+φu1+v12)=f(ϕ+φu1+ϕ+φv12)h(12)(f(ϕ+φu1)+f(ϕ+φv1))c(14)((ϕ+φu1)(ϕ+φv1))2.

    u1,v1[ϕ,φ].

    If we take u1=t2u+2t2v and v1=2t2u+t2v. Then for u, v [ϕ,φ] and t[0,1], we have

    f(ϕ+φu1+v12)h(12)(f(ϕ+φ(t2u+2t2v))+f(ϕ+φ(2t2u+t2v)))c(14)(1t)2(uv)2. (3.4)

    Multiplying (3.4) by (1(1t)εγ)δk1(1t)ε1 and integrating the resulting inequality with respect to t over [0, 1] and then combining the obtained inequality with the definition of integral operator gives

    f(ϕ+φu+v2)10(1(1t)εε)δk1(1t)ε1dt10(1(1t)εε)δk1(1t)ε1[h(12){f(ϕ+φ(t2u+2t2v))+f(ϕ+φ(2t2u+t2v))}c(14)(1t)2(uv)2]dt=h(12){ϕ+φu+v2ϕ+φv(1((ϕ+φu+v2)t1vu2)εε)δk1((ϕ+φu+v2)t1vu2)ε1f(t1)×(2vudt1)+ϕ+φuϕ+φu+v2(1(t2(ϕ+φu+v2)vu2)ε)δk1(t2(ϕ+φu+v2)vu2)ε1×(f(t2)2vudt2)}c(14)(uv)210(1(1t)εε)δk1(1t)ε+1dt=h(12)(2vu)εδk{kΓk(δ)δkJγ(ϕ+φu+v2)+f(ϕ+φu)+kΓk(δ)δkJγ(ϕ+φu+v2)f(ϕ+φv)}c(14)(1εδkβ(δk,2ε+1))(uv)2.

    Note that

    10(1(1t)εε)δk1(1t)ε1dt=1δkεδk. (3.5)

    By simple calculations, we have

    f(ϕ+φu+v2)h(12)2εδkεδkΓk(δ+k)(vu)γδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}c(14)(δkβ(δk,2ε+1))(uv)2. (3.6)

    which completes the proof of first inequality of (3.3).

    For second part of inequality (3.3) take the definition of strongly h-convex function and by similar discussion, we get

    f(ϕ+φ(t2u+2t2v))M[f(ϕ)+f(φ)](h(t2)f(u)+h(2t2)f(v))c(t2(2t2))(uv)2

    and

    f(ϕ+φ(2t2u+t2v))M[f(ϕ)+f(φ)](h(2t2)f(u)+h(t2)f(v))c((2t2)t2)(uv)2.

    Adding the above two inequalities give

    f(ϕ+φ(t2u+2t2v))+f(ϕ+φ(2t2u+t2v))2M[f(ϕ)+f(φ)][(h(t2)+h(2t2))f(u)+(h(2t2)+h(t2))f(v)]2c((2t2)t2)(uv)2.

    By using super-additivity of function, we have

    f(ϕ+φ(t2u+2t2v))+f(ϕ+φ(2t2u+t2v))2M[f(ϕ)+f(φ)]h(1)[f(u)+f(v)]2c(2tt24)(uv)2. (3.7)

    Multiplying (3.7) by (1(1t)γγ)δk1(1t)γ1 and then integrating the resulting inequality with respect to t over [0, 1], we obtain

    10(1(1t)εε)δk1(1t)ε1{f(ϕ+φ(t2u+2t2v))+f(ϕ+φ(2t2u+t2v))}dt{2M[f(ϕ)+f(φ)]h(1)[f(u)+f(v)]2c(2tt24)(uv)2}(10(1(1t)εε)δk1(1t)ε1dt).

    By computing the above integrals, we have

    (2vu)εδk{kΓk(δ)δkJε(ϕ+φu+v2)+f(ϕ+φu)+kΓk(δ)δkJε(ϕ+φu+v2)f(ϕ+φv)}1δkεδk{2M[f(ϕ)+f(φ)]h(1)[f(u)+f(v)]}12c(1δkεδk1εδkβ(δk,2ε+1))(uv)2.

    that is,

    2εδkεδkΓk(δ+k)(vu)γδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}2M[f(ϕ)+f(φ)]h(1)[f(u)+f(v)]12c(1δkβ(δk,2ε+1))(uv)2. (3.8)

    Multiplying both sides of (3.8) by h(12) and then subtract c(14)(δkβ(δk,2ε+1))(uv)2 leads to the conclusion that

    h(12)2εδkεδkΓk(δ+k)(vu)γδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}c(14)(δkβ(δk,2ε+1))(uv)2h(12)2M[f(ϕ)+f(φ)]h(12)h(1)[f(u)+f(v)]c(12h(12)(1δkβ(δk,2ε+1))(uv)2+14(δkβ(δk,2ε+1))(uv)2). (3.9)

    Combining (3.6) and (3.9) lead to (3.3).

    Remark 3.6. 1. Taking h(t) = t, M = sup {h(t):t(0,1)} = 1 and c = 0 in Theorem 3.5, we get Theorem 2.1 of [28].

    2. Taking h(t) = t, M = sup {h(t):t(0,1)} = 1, c = 0, k = 1, u = ϕ, and v = φ in Theorem 3.5, we get Theorem 2.1 of [29].

    3. Taking (t) = t, M = sup {h(t):t(0,1)} = 1, c = 0, ε=k=1, u=ϕ and v=φ in Theorem 3.5, we get Theorem 2 of [30].

    Theorem 3.7. Let f:IR R be a strongly h-convex function with modulus c > 0 and ϕ,φI with f<φ. If h is a super-additive function and take ε,δ> 0. Then

    f(ϕ+φu+v2)h(12)2M[f(ϕ)+f(φ)]h(12)h(1)εδkΓk(δ+k)(vu)εδk{δkJεu+f(v)+δkJεvf(u)}c[12h(12)(1δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+14(δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2]h(12)2M[f(ϕ)+f(φ)]h(1)f(u+v2)c[14h(1)(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+12h(12)(1δkβ(δk,2ε+1))×(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+14(δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2]. (3.10)

    and

    f(ϕ+φu+v2)h(12)εδkΓk(δ+k)(vu)εδk{δkJε(ϕ+φv)+f(ϕ+φu)+δkJε(ϕ+φu)f(ϕ+φv)}c(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(uv)2h(1)(h(12)2M[f(ϕ)+f(φ)]h(1)h(12)[f(u)+f(v)])c(2h(1)h(12)δk(β(βk,1ε+1)β(βk,2ε+1))(uv)2+2h(12)δk(β(βk,1ε+1)β(βk,2ε+1))(vu)2+(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(uv)2). (3.11)

    holds u, v [ϕ,φ], where M = sup {h(t):t(0,1)}.

    Proof. Employing Jensen-Mercer inequality (3.3), we have

    f(ϕ+φu1+v12)h(12)2M[f(ϕ)+f(φ)]h(12)h(1)[f(u1)+f(v1)]c(12h(12)(1δkβ(δk,2ε+1))(u1v1)2+14(δkβ(δk,2ε+1))(u1v1)2). (3.12)

    u1,v1[ϕ,].

    By changing variables u1=tu+(1t)v and v1=(1t)u+tv for all u, v [ϕ,φ] and t[0,1] in (3.12), we get

    f(ϕ+φu+v2)h(12)2M[f(c)+f(φ)]h(12)h(1)[f(tu+(1t)v)+f((1t)u+tv)]c(12h(12)(1δkβ(δk,2ε+1))(12t)2(vu)2+14(δkβ(δk,2ε+1))(12t)2(vu)2). (3.13)

    Multiplying (3.13) by (1(1t)εε)δk1(1t)ε1 and integrating the obtained inequality with respect to t over [0, 1] gives

    f(ϕ+φu+v2)10(1(1t)εε)δk1(1t)ε1dt10(1(1t)εε)δk1(1t)ε1×[(h(12)2M[f(ϕ)+f(φ)]h(12)h(1)[f(tu+(1t)v)+f((1t)u+tv)])c(12h(12)(1δkβ(δk,2ε+1))(12t)2(vu)2+14(δkβ(δk,2ε+1))(12t)2(vu)2)]dt.

    that is,

    f(ϕ+φu+v2)h(12)2M[f(ϕ)+f(φ)]h(12)h(1)εδkΓk(δ+k)(vu)εδk{δkJεu+f(v)+δkJεvf(u)}c[12h(12)(1δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+14(δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2], (3.14)

    this completes the proof of first inequality of (3.10).

    Now for second part of inequality (3.10) take the definition of strongly h-convex function, we have

    f(u+v2)=f(tu+(1t)v+(1t)u+tv2)h(12){f(tu+(1t)v)+f((1t)u+tv)}c(14)((tu+(1t)v)((1t)u+tv))2. (3.15)

    Multiplying (3.15) by (1(1t)εε)δk1(1t)ε1 and then integrating the resulting inequality with respect to t over [0, 1], we obtain

    f(u+v2)10(1(1t)εε)δk1(1t)ε1dt10(1(1t)εε)δk1(1t)ε1(h(12){f(tu+(1t)v)+f((1t)u+tv)}c(14)(12t)2(vu)2)dt.

    By some calculations, we get

    f(u+v2)h(12)εδkΓk(δ+k)(vu)εδk{δkJεu+f(v)+δkJεvf(u)},c(14)(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2f(u+v2)h(12)εδkΓk(δ+k)(vu)εδk{δkJεu+f(v)+δkJεvf(u)}+c(14)(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2. (3.16)

    Multiplying (3.16) by h(1), we have

    h(1)f(u+v2)h(12)h(1)εδkΓk(δ+k)(vu)εδk{δkJεu+f(v)+δkJεvf(u)}+c(14)h(1)(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2. (3.17)

    Adding h(12)2M[f(ϕ)+f(φ)] to both sides of (3.17), we get

    h(12)2M[f(ϕ)+f(φ)]h(1)f(u+v2)h(12)2M[f(ϕ)+f(φ)]h(12)h(1)εδkΓk(δ+k)(nm)εδk{δkJεu+f(v)+δkJεvf(u)}+c(14)h(1)(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2.

    Adding c[12h(12)(1δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+14(δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2] to both sides of above inequality, we have

    h(12)2M[f(ϕ)+f(φ)]h(12)h(1)εδkΓk(δ+k)(vu)εδk{δkJεu+f(v)+δkJεvf(u)}c[12h(12)(1δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+14(δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2]h(12)2M[f(ϕ)+f(φ)]h(1)f(u+v2)c[14h(1)(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+12h(12)(1δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2+14(δkβ(δk,2ε+1))(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(vu)2]. (3.18)

    Combining (3.14) and (3.18) yields (3.10).

    Next, we prove inequality (3.11) by using strong h-convexity of f, we have

    f(ϕ+φu1+v12)=f(ϕ+φu1+ϕ+φv12)h(12){f(ϕ+φu1)+f(ϕ+φv1)}c(14)((ϕ+φu1)+(ϕ+φv1))2. (3.19)

    for all u1,v1[ϕ,φ].

    For u1=tu+(1t)v and v1=(1t)u+tv. Then (3.19) leads to the conclusion that

    f(ϕ+νu+v2)h(12){f(ϕ+ν(tu+(1t)v))+f(c+ν((1t)u+tv))}c(14)(12t)2(uv)2. (3.20)

    Multiplying (3.20) by (1(1t)εε)δk1(1t)ε1 and then integrating the resulting inequality with respect to t over [0, 1], we have

    f(ϕ+φu+v2)10(1(1t)εε)δk1(1t)ε1dt10(1(1t)εε)δk1(1t)ε1×(h(12){f(ϕ+φ(tu+(1t)v))+f(ϕ+φ((1t)u+tv))}c(14)(12t)2(uv)2)dt,

    By computing the above integrals, we get

    f(ϕ+φu+v2)h(12)εδkΓk(δ+k)(vu)εδk{δkJγ(ϕ+φv)+f(ϕ+φu)+δkJε(ϕ+φu)f(ϕ+φv)}.c(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(uv)2. (3.21)

    Employing strong h-convexity of f gives

    f(t(ϕ+φu)+(1t)(ϕ+φv))h(t)f(ϕ+φu)+h(1t)f(ϕ+φv)ct(1t)((ϕ+φu)(ϕ+φv))2,

    and

    f((1t)(ϕ+φu)+t(ϕ+φv))h(1t)f(ϕ+φu)+h(t)f(ϕ+φv)c(1t)t((ϕ+φu)(ϕ+φv))2.

    Adding above two inequalities and employing supper-additivity of function, we have

    f(t(ϕ+φu)+(1t)(ϕ+φv))+f((1t)(ϕ+φu)+t(ϕ+φv))f(ϕ+φu)(h(t)+h(1t))+f(ϕ+φv)(h(1t)+h(t))2ct(1t)(vu)2h(1)(f(ϕ+φu)+f(c+φv))2ct(1t)(vu)2.

    Now employing the Jensen-Mercer inequality, we get

    f(t(ϕ+φu)+(1t)(ϕ+φv))+f((1t)(ϕ+φu)+t(ϕ+φv))h(1)(2M[f(ϕ)+f(φ)]h(1)[f(u)+f(v)]2ct(1t)(uv)2)2ct(1t)(vu)2. (3.22)

    Multiplying (3.22) by (1(1t)εε)δk1(1t)ε1 and integrate the resulting inequality with respect to t over [0, 1], we have

    10(1(1t)εε)δk1(1t)ε1{f(t(ϕ+φu)+(1t)(ϕ+φv))+f((1t)(ϕ+φu)+t(ϕ+φv))}dt(h(1)(2M[f(ϕ)+f(φ)]h(1)[f(u)+f(v)]2ct(1t)(uv)2)2ct(1t)(vu)2)10(1(1t)εε)δk1(1t)ε1dt.

    Adding c(1+4δk(β(δk,2ε+1)β(δk,1ε+1)))(uv)2 to both sides of above inequality and combining the result with (3.21) yields (3.11).

    Remark 3.8. 1. Taking h(t) = t, c = 0 and M = sup {h(t):t(0,1)} = 1 in Theorem 3.7, we get Theorem 2.3 of [28].

    2. Taking ε=δ=k=1, c = 0, h(t) = t and M = sup {h(t):t(0,1)} = 1 in Theorem 3.7, we get Theorem 2.1 of [31].

    Lemma 3.9. [28] Let ε,δ>0,ϕ<φ and f:[ϕ,φ] R be a differentiable mapping such that fL[ϕ,φ]. Then the inequality

    2εδk1Γk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)=(vu)εδk410(1(1t)εε)δk{f(ϕ+φ(2t2u+t2v))f(ϕ+φ(t2u+2t2v))}dt. (3.23)

    holds for all u,v[ϕ,φ].

    Theorem 3.10. Let f:IR R ba a differentiable function on I, ϕ,φI with ϕ<φ and fL[ϕ,φ]. If |f| is a strongly h-convex function with modulus c> 0 on [ϕ,φ] and take ε,δ> 0. Then

    |2εδk1εk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)|(vu)εδk4[{M[|f(ϕ)|+|f(φ)|](1εδk+1β(δk+1,1ε))(|f(u)|β1(h,2t2)+|f(v)|β2(h,t2))c14εδk+1(β(δk+1,1ε)β(δk+1,3ε))(uv)2}+{M[|f(ϕ)|+|f(φ)|](1εδk+1β(δk+1,1ε))(|f(u)|β2(h,t2)+|f(v)|β1(h,2t2))c14εδk+1(β(δk+1,1ε)β(δk+1,3ε))(uv)2}], (3.24)

    holds u,v[ϕ,φ], where β1(h,2t2)=10(1(1t)εε)δkh(2t2)dt, β2(h,t2)=10(1(1t)εε)δkh(t2)dt and M=sup{h(t):t(0,1)}.

    Proof. Employing Lemma 3.9, inequality (3.2) and definition of strong h-convexity of |f| yield the desired result.

    Remark 3.11. 1. Taking h(t) = t, M = sup {h(t):t(0,1)} = 1 and c = 0 in Theorem 3.10, we get Theorem 2.10 of [28].

    2. Taking h(t) = t, M = sup{h(t):t(0,1)} = 1, c = 0, k = 1, u = ϕ and v = φ in Theorem 3.10, we get Theorem 3.1 of [29].

    3. Taking ε=k=1, h(t) = t, M = sup {h(t):t(0,1)} = 1, c = 0, u = ϕ and v = φ in Theorem 3.10, we get Theorem 5 of [32] in the case of q = 1.

    Theorem 3.12. Let f:IR R be a differentiable function on I, ϕ,φI with ϕ<φ and fL[ϕ,φ]. If |f|q is a strongly h-convex function with modulus c> 0 on [ϕ,φ] for q> 1 and take ε,δ> 0. Then

    |2εδk1εk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)(vu)εδk4[{(1εδk+1β(δk+1,1ε))11q{M[|f(ϕ)|q+|f(φ)|q](1εδk+1β(δk+1,1ε))|((|f(u)|qβ2(h,t2)+|f(v)|qβ1(h,2t2))c14εδk+1(β(δk+1,1ε)β(δk+1,3ε))(uv)2)1q}}+{(1εδk+1β(δk+1,1ε))11q{M[|f(ϕ)|q+|f(φ)|q](1εδk+1β(δk+1,1ε))((|f(u)|qβ1(h,2t2)+|f(v)|qβ2(h,t2))c14εδk+1(β(δk+1,1ε)β(δk+1,3ε))(uv)2)1q}}], (3.25)

    holds u, v [ϕ,φ], where β1(h,2t2), β2(h,t2) and M are same as in Theorem 3.10.

    Proof. Employing Lemma 3.9, inequality (3.2), power-mean inequality and definition of strongly h-convex function of |f| yield the desired result.

    Remark 3.13. Taking h(t) = t, M = sup {h(t):t(0,1)} = 1 and c = 0 in Theorem 3.12, we get Theorem 2.12 of [28].

    Theorem 3.14. Let f:IR R be a differentiable function on I, ϕ,φI with ϕ<φ and fL[ϕ,φ]. If |f|q is a strongly h-convex function with modulus c> 0 on [ϕ,φ] for p,q> 1 with 1p+1q=1 and take ε,δ> 0. Then

    |2εδk1εk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)|(vu)εδk4(1εδkp+1β(δkp+1,1ε))1p{(M[|f(ϕ)|q+|f(φ)|q](|f(u)|qC1(h,2t2)+|f(v)|q C2(h,t2))c16(uv)2)1q+(M[|f(ϕ)|q+|f(φ)|q](|f(u)|qC2(h,t2)+|f(v)|qC1(h,2t2))c16(uv)2)1q}, (3.26)

    holds u,v[ϕ,φ], where C1(h,2t2)=10h(2t2)dt, C2(h,t2)=10h(t2)dt and M=sup{h(t):t(0,1)}.

    Proof. From applying Lemma 3.9, inequality 3.2, Hölder integral inequalities and definition of strongly h-convex function simultaneously give the desired result.

    Remark 3.15. Taking h(t) = t, M = sup {h(t):t(0,1)} = 1 and c = 0 in Theorem 3.14, we get Theorem 2.14 of [28].

    Theorem 3.16. Assume f:IR R be a differentiable function on I, ϕ,φI with ϕ<φ and fL[ϕ,φ]. If |f|q is a strongly h-convex function with modulus c> 0 on [ϕ,φ] for p,q> 1 with 1p+1q=1 and take ε,δ> 0. Then

    |2εδk1εk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)|(vu)εδk4{(M(|f(ϕ)|q+|f(φ)|q)(β(δk+1,1ε)εδk+1)(β1(h,2t2)|f(u)|q+β2(h,t2)|f(v)|q)c14εδk+1(β(δk+1,1ε)β(δk+1,3ε))(uv)2)1q+(M(|f(ϕ)|q+|f(φ)|q)(β(δk+1,1ε)εδk+1)(β2(h,t2)|f(u)|q+β1(h,2t2)|f(v)|q)c14εδk+1(β(δk+1,1ε)β(δk+1,3ε))(uv)2)1q}, (3.27)

    holds u,v[ϕ,φ], where β1(h,2t2), β2(h,t2) and M are same as in Theorem 3.10.

    Proof. Using Lemma 3.9, inequality (3.2), Hölder integral inequalities and definition of strongly h-convex function, we obtain our desired result.

    Remark 3.17. Taking h(t) = t, M = sup {h(t):t(0,1)} = 1 and c = 0 in Theorem 3.16, we get Theorem 2.16 of [28].

    Theorem 3.18. Let f:IR R be a differentiable function on I, ϕ,φI with ϕ<φ and fL[ϕ,φ]. If |f|q is a strongly h-convex function with modulus c> 0 on [ϕ,φ] for p,q> 1 with 1p+1q=1 and take ε,δ> 0. Then

    |2εδk1εk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)|(vu)εδk4[{(β(2ε,δk+1)εδk+1)1p(M(|f(ϕ)|q+|f(φ)|q)2(β1((1t)h,2t2)|f(u)|q+β2((1t)h,t2)|f(v)|q)c16(uv)2)1q+(β(1ε,δkp+1)β(2ε,δkp+1)εδkp+1)1p(M(|f(ϕ)|q+|f(φ)|q)2(β3(th,2t2)|f(u)|q+β4(th,t2)|f(v)|q)c548(uv)2)1q}+{(β(2ε,δkp+1)εδkp+1)1p(M(|f(ϕ)|q+|f(φ)|q)2(β2((1t)h,t2)|f(u)|q+β1((1t)h,2t2)|f(v)|q)c16(uv)2)1q+(β(1ε,δkp+1)β(2ε,δkp+1)εδkp+1)1p(M(|f(ϕ)|q+|f(φ)|q)2(β4(th,t2)|f(u)|q+β3(th,2t2)|f(v)|q)c548(uv)2)1q}], (3.28)

    holds for all u, v [ϕ,φ], where β1((1t)h,2t2)=10(1t)h(2t2)dt, β2((1t)h,t2)=10(1t)h(t2)dt, β3(th,2t2)=10th(2t2)dt, β4(th,t2)=10th(t2)dt and M=sup{h(t):t(0,1)}.

    Proof. Using Lemma 3.9, inequality (3.2), Hölder-Íscan integral inequality given in Theorem 1.4 of [33] and definition of strongly h-convex function of |f|q yield the desired result.

    Remark 3.19. Taking h(t) = t, c = 0 and M=sup{h(t):t(0,1)} = 1 in Theorem 3.18, we get Theorem 3.1 of [28].

    Theorem 3.20. Let f:IR R be a differentiable function on I, ϕ,φI with ϕ<φ and fL[ϕ,φ]. If |f|q is a strongly h-convex function with modulus c on [ϕ,φ], where p,q> 1 with 1p+1q=1 and take ε,δ> 0. Then

    |2εδk1εk(δ+k)(vu)εδk{δkJε(ϕ+φu+v2)+f(ϕ+φu)+δkJε(ϕ+φu+v2)f(ϕ+φv)}f(ϕ+φu+v2)|(vu)εδk4[{(β(2ε,δk+1)εδk+1)11q(M(|f(ϕ)|q+|f(φ)|q)(β(2ε,δk+1)εδk+1)(β1((1t)h,2t2)|f(u)|q+β2((1t)h,t2)|f(v)|q)c14εδk+1(β(δk+1,2ε)β(δk+1,4ε))(uv)2)1q+(β(1ε,δk+1)β(2ε,δk+1)εδk+1)11q(M(|f(ϕ)|q+|f(φ)|q)(β(1ε,δk+1)β(2ε,δk+1)εδk+1)(β3(th,2t2)|f(u)|q+β4(th,t2)|f(v)|q)c14εδk+1(β(δk+1,4ε)β(δk+1,3ε)β(δk+1,2ε)+β(δk+1,1ε))(uv)2)1q}+{(β(2ε,δk+1)εδk+1)11q(M(|f(ϕ)|q+|f(φ)|q)(β(2ε,δk+1)εδk+1)(β2((1t)h,t2)|f(u)|q+β1((1t)h,2t2)|f(v)|q)c14εδk+1(β(δk+1,2ε)β(δk+1,4ε))×(uv)2)1q+(β(1ε,δk+1)β(2ε,δk+1)εδk+1)11q(M(|f(ϕ)|q+|f(φ)|q)(β(1ε,δk+1)β(2ε,δk+1)εδk+1)(β4(th,t2)|f(u)|q+β3(th,2t2)|f(v)|q)c14εδk+1(β(δk+1,4ε)β(δk+1,3ε)β(δk+1,2ε)+β(δk+1,1ε))(uv)2)1q}], (3.29)

    holds for all u, v [ϕ,φ], where β1((1t)h,2t2)=10(1t)(1(1t)εε)δkh(2t2)dt, β2((1t)h,t2)=10(1t)(1(1t)εε)δkh(t2)dt, β3(th,2t2)=10t(1(1t)εε)δkh(2t2)dt, β4(th,t2)=10t(1(1t)εε)δkh(t2)dt and M=sup{h(t):t(0,1)}.

    Proof. Employing Lemma 3.9, inequality (3.2), improved power-mean integral inequality given in Theorem 1.5 of [33] and definition of strong h-convexity of |f|q yield the required result.

    Remark 3.21. Taking h(t) = t, c = 0 and M = sup {h(t):t(0,1)} = 1 in Theorem 3.20, we get Theorem 3.2 of [28].

    The convex functions play an important role in applied mathematics as well as in optimization theory. In past years, researchers paid a huge attention to establish properties of different variants of convex functions. In this paper, we studied h-convex functions in the setting of k-fractional integrals. We established various important versions of Hermite-Hadamard type inequalities for h-convex. Our results generalize and extend many existing results in literature.

    The study was supported by Fundamental Research Funds for the Central Universities (Grant No. 2020RC14) and Young teachers undergraduate teaching top talents Project of Shandong University of Science and Technology (No. BJRC20190508).

    The author declares no conflict of interests.



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