Improved artificial bee colony algorithm for air freight station scheduling

Haiquan Wang; Hans-Dietrich Haasis; Menghao Su; Jianhua Wei; Xiaobin Xu; Shengjun Wen; Juntao Li; Wenxuan Yue; Haiquan Wang; Hans-Dietrich Haasis; Menghao Su; Jianhua Wei; Xiaobin Xu; Shengjun Wen; Juntao Li; Wenxuan Yue

doi:10.3934/mbe.2022607

Mathematical Biosciences and Engineering

2022, Volume 19, Issue 12: 13007-13027. doi: 10.3934/mbe.2022607

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Research article Special Issues

Improved artificial bee colony algorithm for air freight station scheduling

1.
Zhongyuan-Petersburg Aviation College, Zhongyuan University of Technology, Zhengzhou 450007, China
2.
Chair in Maritime Business and Logistics, University of Bremen, Max-von-Laue-Str. 1, 28359 Bremen, Germany
3.
Faculty of Information Engineering, Zhengzhou University of Industrial Technology, Xinzheng 451100, China
4.
Zhengzhou Tiamaes Technology Co., Ltd, Zhengzhou 450007, China
5.
School of Automation, Hangzhou Dianzi University, Hangzhou 310018, China
6.
Beijing Key Laboratory of Intelligent Logistics Systems, Beijing Wuzi University, Beijing 100000, China
7.
Faculty of Electrical and Engineering, Zhongyuan University of Technology, 41 Zhongyuan Road, Zhengzhou 450007, China

Academic Editor: Wenqiang Zhang

Received: 13 June 2022 Revised: 26 July 2022 Accepted: 30 August 2022 Published: 05 September 2022

Aiming at improving the operating efficiency of air freight station, the problem of optimizing the sequence of inbound/outbound tasks meanwhile scheduling the actions of elevating transfer vehicles (ETVs) is discussed in this paper. First of all, the scheduling model in airport container storage area, which considers not only the influence of picking sequence, optimal ETVs routing without collision, but also the assignment of input and output ports, is established. Then artificial bee colony (ABC) is proposed to solve the above scheduling issue. For further balancing the abilities of exploration and exploitation, improved multi-dimensional search (IMABC) algorithm is proposed where more dimensions will be covered, and the best dimension of the current optimal solution is used to guide the evolutionary direction in the following exploitation processes. Numerical experiments show that the proposed method can generate optimal solution for the complex scheduling problem, and the proposed IMABC outperforms original ABC and other improved algorithms.

Keywords:

air freight station,
dual elevating transfer vehicles,
cargo flow schedule,
artificial bee colony algorithm,
improved multi-dimensional search strategy

Citation: Haiquan Wang, Hans-Dietrich Haasis, Menghao Su, Jianhua Wei, Xiaobin Xu, Shengjun Wen, Juntao Li, Wenxuan Yue. Improved artificial bee colony algorithm for air freight station scheduling[J]. Mathematical Biosciences and Engineering, 2022, 19(12): 13007-13027. doi: 10.3934/mbe.2022607

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Abstract

1. Introduction

Let $\phi:I \subseteq \Bbb R\rightarrow \Bbb R$ be a convex function and $\alpha, \beta \in I$ with $\alpha < \beta$ , then the following inequality holds,

$\begin{eqnarray} \phi(\frac{{\alpha + \beta}}{2}) \le \frac{1}{{\beta - \alpha}}\int_\alpha^\beta {\phi(x)} dx \le \frac{{\phi(\alpha) + \phi(\beta)}}{2}, \end{eqnarray}$

(1.1)

which is well known as Hermite-Hadamard's inequality ^[1] for convex functions. Both inequalities hold in the reversed direction if $\phi$ is concave.

Convex function is an important function in mathematical analysis and has been applied in many aspects ^[2,3]. With the extension of the definition of convex function, Hermite-Hadamard's inequality has been deeply studied. Some improvement and generalizations for Hermite-Hadamard's inequality (1.1) can been found in the references ^{[4,5,6,7,8,9,10,11,12]}.

In ^[11], İşcan gave the definition of harmonically convexity as follows:

Definition 1. Let $I\subset\mathbb{R}\setminus\{0\}$ be a real interval. A function $\phi:I\rightarrow \mathbb{R}$ is said to be harmonically convex, if

$\begin{align} \phi\left(\frac{xy}{tx+(1-t)y}\right)\leq t\phi(y)+(1-t)\phi(x) \end{align}$

(1.2)

for all $x, y\in I$ and $t\in[0, 1]$ . If the inequality in (1.2) is reversed, then $\phi$ is said to be harmonically concave.

In recent years, many researchers presented many kinds of fractional calculus by different methods and explored their applications. For example, Riemann-Liouville fractional integrals and its applications in inequalities ^{[13,14,15,16]}. Recently, Yang stated the theory of local fractional calculus on Yang's fractal sets systematically in ^[17,18,19]. Local fractional calculus can explain the behavior of continuous but nowhere differentiable function. In view of the special advantages of local fractional calculus, more and more researchers extended their studies to Yang's fractal space, see ^{[20,21,22,23,24,25,26,27,28,29]}.

In ^[22], Sun introduced the definition of the generalized harmonically convex function on Yang's fractal sets as follows:

Definition 2. Let $I\subset\mathbb{R}\setminus\{0\}$ be a real interval. A function $\phi:I\rightarrow \mathbb{R}^{\epsilon}(0 < \epsilon\leq1)$ is said to be generalized harmonically convex, if

$\begin{align} \phi\left(\frac{xy}{tx+(1-t)y}\right)\leq t^{\epsilon}\phi(y)+(1-t)^{\epsilon}\phi(x) \end{align}$

(1.3)

for all $x, y\in I$ and $t\in[0, 1]$ . If the inequality in (1.3) is reversed, then $\phi$ is said to be generalized harmonically concave. The sign $\epsilon$ represents the fractal dimension.

Example 1. Let $\phi:(0, \infty)\rightarrow \mathbb{R}^{\epsilon}$ and $\psi:(-\infty, 0)\rightarrow \mathbb{R}^{\epsilon}$ , then $\phi(x) = x^{\epsilon}$ is a generalized harmonically convex function and $\psi(x) = x^{\epsilon}$ is a generalized harmonically concave function.

The following result related to Hermite-Hadamard's inequalities holds.

Theorem 1. ^[22] Let $\phi: I\subset\mathbb{R}\setminus\{0\}\rightarrow \mathbb{R}^{\epsilon}$ be a generalized harmonically convex function on fractal space and $\alpha, \beta\in I$ with $\alpha < \beta$ . If $\phi(x)\in I_{x}^{(\epsilon)}[\alpha, \beta]$ , then

$\begin{align} \frac{1}{\Gamma(1+\epsilon)} \phi(\frac{2\alpha\beta}{\alpha+\beta}) \le \frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta - \alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}} \le \frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\left[\phi(\alpha) + \phi(\beta)\right]. \end{align}$

(1.4)

Based on the theory of local fractional calculus and the definition of the generalized harmonically convex function on Yang's fractal sets, the main aim of this paper is using a new integral identity and monotonicity of functions to establish some new Hermite-Hadamard type inequalities involving local fractional calculus.

2. Preliminaries

Let $\mathbb{R}^{\epsilon}(0 < \epsilon\leq1)$ be $\epsilon$ -type set of the real line numbers on Yang's fractal sets, and give the following operation rules, see^[17,18]. The sign $\epsilon$ represents the fractal dimension, not the exponential sign.

If $\alpha^{\epsilon}, \beta^{\epsilon}, \gamma^{\epsilon}\in\mathbb{R}^{\epsilon}$ , then addition and multiplication operations satisfy

(a) $\alpha^{\epsilon}+\beta^{\epsilon}\in\mathbb{R}^{\epsilon}$ , $\alpha^{\epsilon}\beta^{\epsilon}\in\mathbb{R}^{\epsilon}$ ,

(b) $\alpha^{\epsilon}+\beta^{\epsilon} = \beta^{\epsilon}+\alpha^{\epsilon} = (\alpha+\beta)^{\epsilon} = (\beta+\alpha)^{\epsilon}$ ,

(d) $\alpha^{\epsilon}\beta^{\epsilon} = \beta^{\epsilon} \alpha^{\epsilon} = (\alpha\beta)^{\epsilon} = (\beta\alpha)^{\epsilon}$ ,

(e) $\alpha^{\epsilon}(\beta^{\epsilon}\gamma^{\epsilon}) = (\alpha^{\epsilon}\beta^{\epsilon})\gamma^{\epsilon}$ ,

(f) $\alpha^{\epsilon}(\beta^{\epsilon}+\gamma^{\epsilon}) = \alpha^{\epsilon}\beta^{\epsilon}+\alpha^{\epsilon}\gamma^{\epsilon}$ ,

(g) $\alpha^{\epsilon}+0^{\epsilon} = \alpha^{\epsilon}$ , $\alpha^{\epsilon}+(-\alpha)^{\epsilon} = 0^{\epsilon}$ and $\alpha^{\epsilon}1^{\epsilon} = 1^{\epsilon}\alpha^{\epsilon} = \alpha^{\epsilon}$ ,

(h) $(\alpha-\beta)^{\epsilon} = \alpha^{\epsilon}-\beta^{\epsilon}$ .

Definition 3. ^[18,19] If there exists the relation

$|\phi(x)-\phi(x_{0})| < \varepsilon^{\epsilon}$

with $|x-x_{0}| < \delta$ , for $\varepsilon, \delta > 0$ and $\varepsilon, \delta\in\mathbb{R}$ .Then the function $\phi(x)$ is called local fractional continuous at $x_{0}$ . If $\phi(x)$ is local fractional continuous on $(\alpha, \beta)$ , we denote by $\phi(x)\in C_{\epsilon}(\alpha, \beta)$ .

Definition 4. ^[17,19] Supposing that $\phi(x)\in C_{\epsilon}(\alpha, \beta)$ , the local fractional derivative of $\phi(x)$ of order $\epsilon$ at $x = x_{0}$ is defined by

$\phi^{(\epsilon)}(x_{0}) = \frac{d^{\epsilon}\phi(x)}{dx^{\epsilon}}\bigg|_{x = x_{0}} = \lim\limits_{x\rightarrow x_{0}}\frac{\Gamma(\epsilon+1)(\phi(x)-\phi(x_{0}))}{(x-x_{0})^{\epsilon}}.$

For any $x\in(\alpha, \beta)$ , there exists $\phi^{(\epsilon)}(x) = D_{x}^{(\epsilon)}$ , denoted by $\phi^{(\epsilon)}(x)\in D_{x}^{(\epsilon)}(\alpha, \beta)$ . $D_{\epsilon}(\alpha, \beta)$ is called $\epsilon$ -local fractional derivative set. If there exits $\phi^{((n+1)\epsilon)}(x) = \overbrace{D_{x}^{\epsilon}\cdot\cdot\cdot D_{x}^{\epsilon}}^{(n+1) \rm{times}}\phi(x)$ for any $x\in I\subseteq\mathbb{R}$ , then we denote $\phi\in D_{(n+1)\epsilon}(I)$ , where $n = 0, 1, 2, \cdot\cdot\cdot$

Definition 5. ^[17,19] Let $\phi(x)\in C_{\epsilon}[\alpha, \beta]$ . The local fractional integral of function $\phi(x)$ of order $\epsilon$ is defined by

${}_{\alpha}I_{\beta}^{(\epsilon)}\phi(x) = \frac{1}{\Gamma(\epsilon+1)}\int_{\alpha}^{\beta}\phi(t)(dt)^{\epsilon} = \frac{1}{\Gamma(\epsilon+1)}\lim\limits_{\Delta t\rightarrow 0}\sum\limits_{j = 0}^{N-1}f(t_{j})(\Delta t_{j})^{\epsilon},$

where $\alpha = t_{0} < t_{1} < \cdot\cdot\cdot < t_{N-1} < t_{N} = \beta, [t_{j}, t_{j+1}]$ is a partition of the interval $[\alpha, \beta]$ , $\Delta t_{j} = t_{j+1}-t_{j}, \Delta t = \max\{\Delta t_{0}, \Delta t_{1} \cdot\cdot\cdot\Delta t_{N-1}\}$ .

Note that ${}_{\alpha}I_{\alpha}^{(\epsilon)}\phi(x) = 0$ , and ${}_{\alpha}I_{\beta}^{(\epsilon)}\phi(x) = -{}_{\beta}I_{\alpha}^{(\epsilon)}\phi(x)$ if $\alpha < \beta$ . We denote $\phi(x)\in I_{x}^{(\epsilon)}[\alpha, \beta]$ if there exits ${}_{\alpha}I_{x}^{(\epsilon)}\phi(x)$ for any $x\in(\alpha, \beta)$ .

Lemma 1. ^[17]

(1) Suppose that $\phi(x) = \varphi^{(\epsilon)}(x)\in C_{\epsilon}[\alpha, \beta]$ , then

${}_{\alpha}I_{\beta}^{(\epsilon)}\phi(x) = \varphi(\beta)-\varphi(\alpha).$

(2) (Local fractional integration by parts)

Suppose that $\phi(x), \varphi(x)\in D_{\epsilon}(\alpha, \beta)$ , and $\phi^{(\epsilon)}(x), \varphi^{(\epsilon)}(x)\in C_{\epsilon}[\alpha, \beta]$ , then

${}_{\alpha}I_{\beta}^{(\epsilon)}\phi(x)\varphi^{(\epsilon)}(x) = [\phi(x)\varphi(x)]\bigg |_{\alpha}^{\beta}-{}_{\alpha}I_{\beta}^{(\epsilon)}\phi^{(\epsilon)}(x)\varphi(x).$

Lemma 2. ^[17] Suppose that $\phi(x)\in C_{\epsilon}[\alpha, \beta]$ and $\alpha < \gamma < \beta$ , then

${}_{\alpha}I_{\beta}^{(\epsilon)}\phi(x) = {}_{\alpha}I_{\gamma}^{(\epsilon)}\phi(x)+{}_{\gamma}I_{\beta}^{(\epsilon)}\phi(x).$

Lemma 3. ^[17]

$\frac{d^{\epsilon}x^{k\epsilon}}{dx^{\epsilon}} = \frac{\Gamma(1+k\epsilon)}{\Gamma(1+(k-1)\epsilon)}x^{(k-1)\epsilon};$

$\frac{1}{\Gamma(\epsilon+1)}\int_{\alpha}^{\beta}x^{k\epsilon}(dx)^{\epsilon} = \frac{\Gamma(1+k\epsilon)}{\Gamma(1+(k+1)\epsilon)}(\beta^{(k+1)\epsilon}-\alpha^{(k+1)\epsilon}), k > 0.$

Lemma 4. ^[18,30] (Generalized Hölder's inequality) Let $\phi, \varphi\in C_{\epsilon}[\alpha, \beta], p, q > 1$ , with $\frac{1}{p}+\frac{1}{q} = 1$ , then

$\frac{1}{\Gamma(\epsilon+1)}\int_{\alpha}^{\beta}|\phi(x)\varphi(x)|(dx)^{\epsilon}\leq\left(\frac{1}{\Gamma(\epsilon+1)}\int_{\alpha}^{\beta}|\phi(x)|^{p}(dx)^{\epsilon}\right)^{1/p} \left(\frac{1}{\Gamma(\epsilon+1)}\int_{\alpha}^{\beta}|\varphi(x)|^{q}(dx)^{\epsilon}\right)^{1/q}.$

Lemma 5. ^[17]

${}_{\alpha}I_{\beta}^{(\epsilon)}1^{\epsilon} = \frac{(\beta-\alpha)^{\epsilon}}{\Gamma(1+\epsilon)}.$

Let us introduce the special functions on Yang's fractal sets as follows:

(1) The generalized Beta function is given by

$\begin{align*} B_{\epsilon}(x,y) = \frac{1}{\Gamma(1+\epsilon)}\int_{0}^{1}t^{(x-1)\epsilon}(1-t)^{(y-1)\epsilon}(dt)^{\epsilon}, x > 0, y > 0, \end{align*}$

(2) The generalized hypergeometric function is given by

$\begin{align*} {}_{2}F_{1}^{\epsilon}(\alpha,\beta;\gamma;z) = \frac{1}{B_{\epsilon}(\beta,\gamma-\beta)}\frac{1}{\Gamma(1+\epsilon)}\int_{0}^{1}t^{(\beta-1)\epsilon}(1-t)^{(\gamma-\beta-1)\epsilon}(1-zt)^{-\alpha\epsilon}(dt)^{\epsilon}, \gamma > \beta > 0, |z| < 1. \end{align*}$

3. Main results

For convenience, we use the symbol $A_{t}$ to denote $t\alpha+(1-t)\beta$ in the following sections.

Lemma 6. Let $I\subset(0, \infty)$ be an interval, $\phi: I^{\circ}\rightarrow \mathbb{R}^{\epsilon}$ ( $I^{\circ}$ is the interior of $I$ ) such that $\phi\in D_{\epsilon}(I^{\circ})$ and $\phi^{(\epsilon)}\in C_{\epsilon}(\alpha, \beta)$ for $\alpha, \beta\in I^{\circ}$ with $\alpha < \beta$ . Then the following equality holds

$\begin{align} \phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta -\alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}} = I_{1}+I_{2}+I_{3}, \end{align}$

(3.1)

where

$\begin{align*} I_{1}& = \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^{1/2} \phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\frac{(dt)^{\epsilon}}{(A_{t})^{2\epsilon}}, \nonumber\\ I_{2}& = -\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_{1/2}^1 \phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\frac{(dt)^{\epsilon}}{(A_{t})^{2\epsilon}}, \nonumber\\ I_{3}& = -\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^{1} (1-2t)^{\epsilon}\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\frac{(dt)^{\epsilon}}{(A_{t})^{2\epsilon}}. \end{align*}$

Proof. Calculating $I_{1}, I_{2}$ , from Lemma 1(1), we get

$\begin{align*} I_{1} = & \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^{1/2} \phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\frac{(dt)^{\epsilon}}{(A_{t})^{2\epsilon}}\nonumber\\ = &\frac{1^{\epsilon}}{2^{\epsilon}}\phi\left(\frac{\alpha\beta}{A_{t}}\right)\Bigg|_{0}^{1/2} = \frac{1^{\epsilon}}{2^{\epsilon}}\Big[\phi\left(\frac{2\alpha\beta}{\alpha+\beta}\right)-\phi(\alpha)\Big] \end{align*}$

and

$\begin{align*} I_{2} = & -\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_{1/2}^1 \phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\frac{(dt)^{\epsilon}}{(A_{t})^{2\epsilon}}\nonumber\\ = &-\frac{1^{\epsilon}}{2^{\epsilon}}\phi\left(\frac{\alpha\beta}{A_{t}}\right)\Bigg|_{1/2}^1 = \frac{1^{\epsilon}}{2^{\epsilon}}\Big[\phi\left(\frac{2\alpha\beta}{\alpha+\beta}\right)-\phi(\beta)\Big]. \end{align*}$

Calculating $I_{3}$ , by the local fractional integration by parts, we have

$\begin{align*} I_{3}& = \frac{\alpha^{\epsilon}\beta^{\epsilon}(\alpha-\beta)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{(1-2t)^{\epsilon}}{(A_{t})^{2\epsilon}}\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)(dt)^{\epsilon}\\ & = \frac{(2t-1)^{\epsilon}}{2^{\epsilon}}\phi\left(\frac{\alpha\beta}{A_{t}}\right)\Bigg|_{0}^{1}-\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \Gamma(1+\epsilon)\phi\left(\frac{\alpha\beta}{A_{t}}\right)(dt)^{\epsilon}\\ & = \frac{\phi(\alpha)+\phi(\beta)}{2^{\epsilon}}-\frac{\Gamma(1+\epsilon)}{\Gamma(1+\epsilon)}\int_0^1 \phi\left(\frac{\alpha\beta}{t\alpha+(1-t)\beta}\right)(dt)^{\epsilon}. \end{align*}$

Using changing variable with $x = \frac{\alpha\beta}{A_{t}}$ , we have

$\begin{align*} I_{3}& = \frac{\phi(\alpha)+\phi(\beta)}{2^{\epsilon}}-\Gamma(1+\epsilon)\left(\frac{\alpha\beta}{\beta-\alpha}\right)^{\epsilon}\frac{1}{\Gamma(1+\epsilon)}\int_\alpha^\beta \frac{\phi(x)}{x^{2\epsilon}}(dx)^{\epsilon}\\ & = \frac{\phi(\alpha)+\phi(\beta)}{2^{\epsilon}}- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta -\alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}} . \end{align*}$

Adding $I_{1}-I_{3}$ , the desired result is obtained. This completes the proof.

Theorem 2. Let $I\subset(0, \infty)$ be an interval, $\phi:I^{\circ}\rightarrow \Bbb R^{\epsilon}$ ( $I^{\circ}$ is the interior of $I$ ) is an increasing function on $I^{\circ}$ such that $\phi\in D_{\epsilon}(I^{\circ})$ and $\phi^{(\epsilon)}\in C_{\epsilon}[\alpha, \beta]$ for $\alpha, \beta\in I^{\circ}$ with $\alpha < \beta$ . If $|\phi^{(\epsilon)}|^{q}$ is generalized harmonically convex on $[\alpha, \beta]$ for some fixed $q > 1$ , then for all $x\in[\alpha, \beta]$ , the following local fractional integrals inequality holds,

$\begin{align} &\Bigg|\phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta - \alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}}\Bigg|\\ \leq& \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}+\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Big(K^{\epsilon}_{1}(\alpha,\beta)\Big)^{1-\frac{1}{q}} \Big(K^{\epsilon}_{2}(\alpha,\beta)\big|\phi^{(\epsilon)}(\alpha)\big|^{q}+ K^{\epsilon}_{3}(\alpha,\beta)\big|\phi^{(\epsilon)}(\beta)\big|^{q}\Big)^{\frac{1}{q}}, \end{align}$

(3.2)

where

$\begin{align*} K^{\epsilon}_{1}(\alpha,\beta) = &\beta^{-2\epsilon}\Bigg[{}_{2}F_{1}^{\epsilon}\Big(2,1;3;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}+ {}_{2}F_{1}^{\epsilon}\Big(2,2;3;1-\frac{\alpha}{\beta}\Big)\frac{2^{\epsilon}\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)} \nonumber\\ &-\frac{{}_{2}F_{1}^{\epsilon}\Big(2,1;2;1-\frac{\alpha}{\beta}\Big)}{\Gamma(1+\epsilon)}\Bigg],\nonumber\\ K^{\alpha}_{2}(\alpha,\beta) = &\beta^{-2\epsilon}\Bigg[\frac{1}{2^{\epsilon}}{}_{2}F_{1}^{\epsilon}\Big(2,2;4;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)\Big(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}-\frac{\Gamma(1+2\epsilon)}{\Gamma(1+3\epsilon)}\Big)\nonumber\\ &+2^{\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2,3;4;1-\frac{\alpha}{\beta}\Big)\frac{\Gamma(1+2\epsilon)}{\Gamma(1+3\epsilon)}-{}_{2}F_{1}^{\epsilon}\Big(2,2;3;1-\frac{\alpha}{\beta}\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg],\nonumber\\ K^{\epsilon}_{3}(\alpha,\beta) = &\beta^{-2\epsilon}\Bigg[{}_{2}F_{1}^{\epsilon}\Big(2,1;3;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\nonumber\\ &+2^{\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2,2;4;1-\frac{\alpha}{\beta}\Big)\Bigg(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}-\frac{\Gamma(1+2\epsilon)}{\Gamma(1+3\epsilon)}\Bigg)-{}_{2}F_{1}^{\epsilon} \Big(2,1;3;1-\frac{\alpha}{\beta}\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg]. \end{align*}$

Proof. Since $\phi$ is an increasing function on $I^{\circ}$ , and $0 < \alpha < \frac{2\alpha\beta}{\alpha+\beta} < \beta$ , we can obtain

$\phi(\alpha) < \phi\big(\frac{2\alpha\beta}{\alpha+\beta}\big) < \phi(\beta).$

From the proof of Lemma 6, we have

$\begin{align} |I_{1}|+|I_{2}| = \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}. \end{align}$

(3.3)

Taking modulus in equality (3.1), we obtain

$\begin{align} \left|\phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta-\alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}}\right| & \leq |I_{1}|+|I_{2}|+|I_{3}| \\ & = \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}+|I_{3}|. \end{align}$

(3.4)

From Lemma 6, using the property of the modulus and the generalized Hölder's inequality, we have

$\begin{align} |I_{3}| = &\Bigg|\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^{1} (1-2t)^{\epsilon}\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\frac{(dt)^{\epsilon}}{(A_{t})^{2\epsilon}}\Bigg|\\ \leq& \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \Big|\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon} \\ = & \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \Big|\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|^{(1-\frac{1}{q})+\frac{1}{q}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon} \\ \leq& \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \Big|\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|(dt)^{\epsilon}\Bigg]^{1-\frac{1}{q}}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big|\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q}(dt)^{\epsilon}\Bigg]^{\frac{1}{q}}. \end{align}$

(3.5)

Since $|\phi^{(\epsilon)}|^{q}$ is generalized harmonically convex on $[\alpha, \beta]$ , thus

$\begin{align} &\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big|\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q} (dt)^{\epsilon} \\ \leq&\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big|\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\Big(t^{\epsilon}\big|\phi^{(\epsilon)}(\beta)\big|^{q}+ (1-t)^{\epsilon}\big|\phi^{(\epsilon)}(\alpha)\big|^{q}\Big)(dt)^{\epsilon}\\ = &\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{|1-2t|^{\epsilon}t^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\Bigg)\big|\phi^{(\epsilon)}(\alpha)\big|^{q} \\ &+ \Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{|1-2t|^{\epsilon}(1-t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\Bigg)\big|\phi^{(\epsilon)}(\beta)\big|^{q}. \end{align}$

(3.6)

By calculating, we get

$\begin{align} &\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{|1-2t|^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\frac{1}{\Gamma(1+\epsilon)}\int_0^\frac{1}{2}\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}+\frac{1}{\Gamma(1+\epsilon)}\int_\frac{1}{2}^1\frac{(2t -1)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\frac{2^{\epsilon}}{\Gamma(1+\epsilon)}\int_0^\frac{1}{2}\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon} \\ &+\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{(2t )^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}-\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{1^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\beta^{-2\epsilon}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1(1-u)^{\epsilon}\Big(1-\frac{u}{2}(1-\frac{\alpha}{\beta})\Big)^{-2\epsilon}(du)^{\epsilon} \\ &+\frac{ 2^{\epsilon}}{\Gamma(1+\epsilon)} \int_0^1t^{\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2\epsilon}(dt)^{\epsilon}\\ &-\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2\epsilon}(dt)^{\epsilon}\Bigg]\\ = &\beta^{-2\epsilon}\Big[{}_{2}F_{1}^{\epsilon}\Big(2,1;3;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)B_{\epsilon}(1,2)+ 2^{\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2,2;3;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(2,1) \\ &-{}_{2}F_{1}^{\epsilon}\Big(2,1;2;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(1,1)\Big]\\ = &\beta^{-2\epsilon}\Bigg[{}_{2}F_{1}^{\epsilon}\Big(2,1;3;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}+ {}_{2}F_{1}^{\epsilon}\Big(2,2;3;1-\frac{\alpha}{\beta}\Big)\frac{2^{\epsilon}\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)} \\ &-\frac{{}_{2}F_{1}^{\epsilon}\Big(2,1;2;1-\frac{\alpha}{\beta}\Big)}{\Gamma(1+\epsilon)}\Bigg]\\ = &K^{\epsilon}_{1}(\alpha,\beta). \end{align}$

(3.7)

Similarly, we get

$\begin{align} &\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{|1-2t|^{\epsilon}t^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\frac{1}{\Gamma(1+\epsilon)}\int_0^\frac{1}{2}\frac{(1-2t)^{\epsilon}t^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}+\frac{1}{\Gamma(1+\epsilon)}\int_\frac{1}{2}^1\frac{(2t -1)^{\epsilon}t^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\frac{2^{\epsilon}}{\Gamma(1+\epsilon)}\int_0^\frac{1}{2}\frac{t^{\epsilon}(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}+\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{2^{\epsilon}t^{2\epsilon} }{A_{t}^{2\epsilon}}(dt)^{\epsilon}-\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{t^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\beta^{-2\epsilon}\Bigg[\frac{1}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1u^{\epsilon}(1-u)^{\epsilon}\Big(1-\frac{u}{2}(1-\frac{\alpha}{\beta})\Big)^{-2\epsilon}(du)^{\epsilon}+\frac{ 2^{\epsilon}}{\Gamma(1+\epsilon)} \int_0^1t^{2\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2\epsilon}(dt)^{\epsilon}\\ &-\frac{1}{\Gamma(1+\epsilon)}\int_0^1t^{\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2\epsilon}(dt)^{\epsilon}\Bigg]\\ = &\beta^{-2\epsilon}\Bigg[\frac{1}{2^{\epsilon}}{}_{2}F_{1}^{\epsilon}\Big(2,2;4;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)\Big(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}-\frac{\Gamma(1+2\epsilon)}{\Gamma(1+3\epsilon)}\Big)\\ &+2^{\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2,3;4;1-\frac{\alpha}{\beta}\Big)\frac{\Gamma(1+2\epsilon)}{\Gamma(1+3\epsilon)}-{}_{2}F_{1}^{\epsilon}\Big(2,2;3;1-\frac{\alpha}{\beta}\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg] = K^{\epsilon}_{2}(\alpha,\beta), \end{align}$

(3.8)

and

$\begin{align} &\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{|1-2t|^{\epsilon}(1-t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\frac{2^{\epsilon}}{\Gamma(1+\epsilon)}\int_0^\frac{1}{2}\frac{(1-2t)^{\epsilon}(1-t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}+\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{(2t -1)^{\epsilon}(1-t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ \leq&\frac{2^{\epsilon}}{\Gamma(1+\epsilon)}\int_0^\frac{1}{2}\frac{(1-2t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}+\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{2^{\epsilon}t^{\epsilon}(1-t)^{\epsilon} }{A_{t}^{2\epsilon}}(dt)^{\epsilon} \\ &-\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{(1-t)^{\epsilon}}{A_{t}^{2\epsilon}}(dt)^{\epsilon}\\ = &\beta^{-2\epsilon}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1(1-u)^{\epsilon}\Big(1-\frac{u}{2}(1-\frac{\alpha}{\beta})\Big)^{-2\epsilon}(du)^{\epsilon} \\ &+\frac{ 2^{\epsilon}}{\Gamma(1+\epsilon)} \int_0^1t^{\epsilon}(1-t)^{\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2\epsilon}(dt)^{\epsilon}\\ &-\frac{1}{\Gamma(1+\epsilon)}\int_0^1(1-t)^{\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2\epsilon}(dt)^{\epsilon}\Bigg]\\ = &\beta^{-2\epsilon}\Bigg[{}_{2}F_{1}^{\epsilon}\Big(2,1;3;\frac{1}{2}(1-\frac{\alpha}{\beta})\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\\ &+2^{\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2,2;4;1-\frac{\alpha}{\beta}\Big)\Bigg(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}-\frac{\Gamma(1+2\epsilon)}{\Gamma(1+3\epsilon)}\Bigg) \\ &-{}_{2}F_{1}^{\epsilon}\Big(2,1;3;1-\frac{\alpha}{\beta}\Big)\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg] = K^{\epsilon}_{3}(\alpha,\beta). \end{align}$

(3.9)

From (3.4)–(3.9), we get inequality (3.2). This completes the proof.

Theorem 3. Let $I\subset(0, \infty)$ be an interval, $\phi:I^{\circ}\rightarrow \Bbb R^{\epsilon}$ is an increasing function on $I^{\circ}$ such that $\phi\in D_{\epsilon}(I^{\circ})$ and $\phi^{(\epsilon)}\in C_{\epsilon}[\alpha, \beta]$ for $\alpha, \beta\in I^{\circ}$ with $\alpha < \beta$ . If $|\phi^{(\epsilon)}|^{q}$ is generalized harmonically convex on $[\alpha, \beta]$ , $q > 1, \frac{1}{p}+\frac{1}{q} = 1$ , then for all $x\in[\alpha, \beta]$ , the following local fractional integrals inequality holds.

$\begin{align} &\Bigg|\phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta - \alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}}\Bigg|\\ \leq& \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}+\frac{\alpha^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}\beta^{\epsilon}}\Bigg[\frac{\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}\Bigg]^{\frac{1}{p}} \Bigg(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg)^{\frac{1}{q}}\\ &\times\Bigg[{}_{2}F_{1}^{\epsilon}\Big(2q,2;3;1-\frac{\alpha}{\beta}\Big)\big|\phi^{(\epsilon)}(\alpha)\big|^{q}+{}_{2}F_{1}^{\epsilon}\Big(2q,1;3;1-\frac{\alpha}{\beta}\Big)\big|\phi^{(\epsilon)}(\beta)\big|^{q}\Bigg]^{\frac{1}{q}}. \end{align}$

(3.10)

Proof. From inequality (3.4), we have

$\begin{align} \left|\phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta - \alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}}\right| \leq\frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}+|I_{3}|. \end{align}$

(3.11)

From Lemma 6, using the property of the modulus and the generalized Hölder's inequality, we have

(3.12)

Since $|\phi^{(\epsilon)}|^{q}$ is generalized harmonically convex on $[\alpha, \beta]$ , we can get

$\begin{align} &\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{1}{A_{t}^{2\epsilon q}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q} (dt)^{\epsilon} \\ \leq&\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{1}{A_{t}^{2q\epsilon }}\Big(t^{\epsilon}\big|\phi^{(\epsilon)}(\beta)\big|^{q}+ (1-t)^{\epsilon}\big|\phi^{(\epsilon)}(\alpha)\big|^{q}\Big)(dt)^{\epsilon}\\ = &\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{t^{\epsilon}}{A_{t}^{2q\epsilon}}(dt)^{\epsilon}\Bigg)\big|\phi^{(\epsilon)}(\beta)\big|^{q}+ \Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{(1-t)^{\epsilon}}{A_{t}^{2q\epsilon}}(dt)^{\epsilon}\Bigg)\big|\phi^{(\epsilon)}(\alpha)\big|^{q}. \end{align}$

(3.13)

By calculating, we have

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{t^{\epsilon}}{A_{t}^{2q\epsilon}}(dt)^{\epsilon}& = \beta^{-2q\epsilon}\frac{1}{\Gamma(1+\epsilon)}\int_0^1t^{\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2q\epsilon}(dt)^{\epsilon}\\ & = \beta^{-2q\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2q,2;3;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(2,1),\\ & = \frac{\Gamma(1+\epsilon)}{\beta^{2q\epsilon}\Gamma(1+2\epsilon)}{}_{2}F_{1}^{\epsilon}\Big(2q,2;3;1-\frac{\alpha}{\beta}\Big), \end{align}$

(3.14)

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{(1-t)^{\epsilon}}{A_{t}^{2q\epsilon}}(dt)^{\epsilon}& = \beta^{-2q\epsilon}\frac{1}{\Gamma(1+\epsilon)}\int_0^1(1-t)^{\epsilon}\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2q\epsilon}(dt)^{\epsilon}\\ & = \beta^{-2q\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2q,1;3;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(1,2),\\ & = \frac{\Gamma(1+\epsilon)}{\beta^{2q\epsilon}\Gamma(1+2\epsilon)}{}_{2}F_{1}^{\epsilon}\Big(2q,1;3;1-\frac{\alpha}{\beta}\Big), \end{align}$

(3.15)

and

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1 |1-2t|^{\epsilon p}(dt)^{\epsilon} = \frac{\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}. \end{align}$

(3.16)

Thus, combining (3.11)–(3.16), we obtain the required inequality. The proof is completed.

Theorem 4. Let $I\subset(0, \infty)$ be an interval, $\phi:I^{\circ}\rightarrow \Bbb R^{\epsilon}$ is an increasing function on $I^{\circ}$ such that $\phi\in D_{\epsilon}(I^{\circ})$ and $\phi^{(\epsilon)}\in C_{\epsilon}[\alpha, \beta]$ for $\alpha, \beta\in I^{\circ}$ with $\alpha < \beta$ . If $|\phi^{(\epsilon)}|^{q}$ is generalized harmonically convex on $[\alpha, \beta]$ , $q > 1, \frac{1}{p}+\frac{1}{q} = 1$ , then for all $x\in[\alpha, \beta]$ , the following local fractional integrals inequality holds.

$\begin{align} &\Bigg|\phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta-\alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}}\Bigg|\\ \leq& \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}+\frac{\alpha^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon }\beta^{\epsilon}}\Bigg[\frac{{}_{2}F_{1}^{\epsilon}\Big(2p,1;2;1-\frac{\alpha}{\beta}\Big)}{\Gamma(1+\epsilon)}\Bigg]^{\frac{1}{p}} \Bigg(\frac{\Gamma(1+q\epsilon)}{2^{\epsilon}\Gamma(1+(q+1)\epsilon)}\Bigg)^{\frac{1}{q}}\\ &\times\Bigg[\big|\phi^{(\epsilon)}(\alpha)\big|^{q}+\big|\phi^{(\epsilon)}(\beta)\big|^{q}\Bigg]^{\frac{1}{q}}. \end{align}$

(3.17)

Proof. From Lemma 6, using the generalized Hölder's inequality and the generalized harmonically convexity of $|\phi^{(\epsilon)}|^{q}$ , we have

$\begin{align} \Big|I_{3}\Big| \leq& \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 |1-2t|^{\epsilon}\frac{1}{A_{t}^{2\epsilon}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon} \\ \leq& \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{1}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg]^{\frac{1}{p}}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1|1-2t|^{\epsilon q}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q}(dt)^{\epsilon}\Bigg]^{\frac{1}{q}} \\ \leq& \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{1}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg]^{\frac{1}{p}} \\ &\times\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1|1-2t|^{\epsilon q}\Big(t^{\epsilon}\big|\phi^{(\epsilon)}(\beta)\big|^{q}+ (1-t)^{\epsilon}\big|\phi^{(\epsilon)}(\alpha)\big|^{q}\Big)(dt)^{\epsilon}\Bigg]^{\frac{1}{q}}. \end{align}$

(3.18)

By calculating, we have

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1\frac{1}{A_{t}^{2p\epsilon}}(dt)^{\epsilon}& = \beta^{-2p\epsilon}\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big(1-(1-\frac{\alpha}{\beta})t\Big)^{-2p\epsilon}(dt)^{\epsilon}\\ & = \beta^{-2p\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2p,1;2;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(1,1),\\ & = \frac{{}_{2}F_{1}^{\epsilon}\Big(2p,1;2;1-\frac{\alpha}{\beta}\Big)}{\beta^{2p\epsilon}\Gamma(1+\epsilon)}, \end{align}$

(3.19)

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1|1-2t|^{\epsilon q}t^{\epsilon}(dt)^{\epsilon} & = \frac{1}{\Gamma(1+\epsilon)}\int_0^{1/2}(1-2t)^{\epsilon q}t^{\epsilon}(dt)^{\epsilon} \\ &+\frac{1}{\Gamma(1+\epsilon)}\int_{1/2}^1(2t-1)^{\epsilon q}t^{\epsilon}(dt)^{\epsilon}\\ & = \frac{\Gamma(1+q\epsilon)}{2^{\epsilon}\Gamma(1+(q+1)\epsilon)}, \end{align}$

(3.20)

and

$\begin{align} &\frac{1}{\Gamma(1+\epsilon)}\int_0^1|1-2t|^{\epsilon q}(1-t)^{\epsilon}(dt)^{\epsilon}\\ = &\frac{1}{\Gamma(1+\epsilon)}\int_0^{1/2}(1-2t)^{\epsilon q}(1-t)^{\epsilon}(dt)^{\epsilon}\\ &+\frac{1}{\Gamma(1+\epsilon)}\int_{1/2}^1(2t-1)^{\epsilon q}(1-t)^{\epsilon}(dt)^{\epsilon}\\ = &\frac{\Gamma(1+q\epsilon)}{2^{\epsilon}\Gamma(1+(q+1)\epsilon)}. \end{align}$

(3.21)

From (3.11) in Theorem 3, combining (3.18)–(3.21), we obtain the required inequality. The proof is completed.

Theorem 5. Let $I\subset(0, \infty)$ be an interval, $\phi:I^{\circ}\rightarrow \Bbb R^{\epsilon}$ is an increasing function on $I^{\circ}$ such that $\phi\in D_{\epsilon}(I^{\circ})$ and $\phi^{(\epsilon)}\in C_{\epsilon}[\alpha, \beta]$ for $\alpha, \beta\in I^{\circ}$ with $\alpha < \beta$ . If $|\phi^{(\epsilon)}|^{q}$ is generalized harmonically convex on $[\alpha, \beta]$ , $q > 1, \frac{1}{p}+\frac{1}{q} = 1$ , then for all $x\in[\alpha, \beta]$ , the following local fractional integrals inequality holds.

$\begin{align} &\Bigg|\phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big)- \Gamma(1+\epsilon)\frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta - \alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}}\Bigg|\\ \leq& \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}}+\frac{\alpha^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}\beta^{\epsilon}}\Bigg[\frac{\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}\Bigg]^{\frac{1}{p}}\Bigg[\Bigg({}_{2}F_{1}^{\epsilon}\Big(2p,1;p+2;1-\frac{\alpha}{\beta}\Big)\Bigg)^{\frac{1}{p}}\\ &+\Bigg({}_{2}F_{1}^{\epsilon}\Big(2p,p+1;p+2;1-\frac{\alpha}{\beta}\Big) \Bigg)^{\frac{1}{p}} \Bigg] \Bigg(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg)^{\frac{1}{q}} \Bigg[\big|\phi^{(\epsilon)}(\alpha)\big|^{q}+\big|\phi^{(\epsilon)}(\beta)\big|^{q}\Bigg]^{\frac{1}{q}}. \end{align}$

(3.22)

Proof. Note that $(\alpha-\beta)^{\epsilon} = \alpha^{\epsilon}-\beta^{\epsilon}$ . From Lemma 6, using the generalized Hölder's inequality and the generalized harmonically convexity of $|\phi^{(\epsilon)}|^{q}$ , we have

$\begin{align} \Big|I_{3}\Big| \leq& \frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{|1-2t|^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon} \\ = &\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{|(1-t)^{\epsilon}-t^{\epsilon}|}{A_{t}^{2\epsilon}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon} \\ \leq&\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{(1-t)^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon} \\ &+\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{t^{\epsilon}}{A_{t}^{2\epsilon}}\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|(dt)^{\epsilon}\Bigg] \\ \leq&\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{(1-t)^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg)^{1/p}\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q}(dt)^{\epsilon}\Bigg)^{1/q} \\ &+\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{t^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg)^{1/p}\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q}(dt)^{\epsilon}\Bigg)^{1/q}\Bigg] \\ = &\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{(1-t)^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg)^{1/p} \\ &+\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{t^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg)^{1/p}\Bigg] \\ &\times\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big|\phi^{(\epsilon)}\left(\frac{\alpha\beta}{A_{t}}\right)\Big|^{q}(dt)^{\epsilon}\Bigg)^{1/q} \\ \leq&\frac{\alpha^{\epsilon}\beta^{\epsilon}(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}\Bigg[\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{(1-t)^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg)^{1/p} \\ &+\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{t^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}\Bigg)^{1/p}\Bigg] \\ &\times\Bigg(\frac{1}{\Gamma(1+\epsilon)}\int_0^1\Big[t^{\epsilon}\big|\phi^{(\epsilon)}(\beta)\big|^{q}+(1-t)^{\epsilon}\big|\phi^{(\epsilon)}(\alpha)\big|^{q}\Big](dt)^{\epsilon}\Bigg)^{1/q}. \end{align}$

(3.23)

By calculating, we have

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{(1-t)^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}& = \beta^{-2 p\epsilon}\frac{1}{\Gamma(1+\epsilon)}\int_0^1 (1-t)^{\epsilon p}\Big[1-(1-\frac{\alpha}{\beta})t\Big]^{-2 p\epsilon}(dt)^{\epsilon} \\ & = \beta^{-2 p\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2p,1;p+2;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(1,p+1) \\ & = \frac{\beta^{-2 p\epsilon}\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}{}_{2}F_{1}^{\epsilon}\Big(2p,1;p+2;1-\frac{\alpha}{\beta}\Big). \end{align}$

(3.24)

Similarly,

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1 \frac{t^{\epsilon p}}{A_{t}^{2\epsilon p}}(dt)^{\epsilon}& = \beta^{-2 p\epsilon}{}_{2}F_{1}^{\epsilon}\Big(2p,p+1;p+2;1-\frac{\alpha}{\beta}\Big)B_{\epsilon}(p+1,1) \\ & = \frac{\beta^{-2 p\epsilon}\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}{}_{2}F_{1}^{\epsilon}\Big(2p,p+1;p+2;1-\frac{\alpha}{\beta}\Big). \end{align}$

(3.25)

And

$\begin{align} \frac{1}{\Gamma(1+\epsilon)}\int_0^1 t^{\epsilon }(dt)^{\epsilon} = \frac{1}{\Gamma(1+\epsilon)}\int_0^1 (1-t)^{\epsilon }(dt)^{\epsilon} = \frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}. \end{align}$

(3.26)

From (3.11) in Theorem 3, combining (3.23)–(3.26), we obtain the required inequality. The proof is completed.

4. Applications to special means

We consider the following $\epsilon$ -type generalized special means of the real line numbers $\alpha^{\epsilon}, \beta^{\epsilon}$ with $\alpha < \beta$ on Yang's fractal sets.

(1) The generalized arithmetic mean

$\begin{align*} A_{\epsilon}(\alpha,\beta) = \frac{\alpha^{\epsilon}+\beta^{\epsilon}}{2^{\epsilon}}; \end{align*}$

(2) The generalized p-logarithmic mean

$\begin{align*} L_{p\epsilon}(\alpha,\beta) = \left[\frac{\Gamma(1+p\epsilon) }{\Gamma(1+(p+1)\epsilon)}\frac{\beta^{(p+1)\epsilon}-\alpha^{(p+1)\epsilon}}{(\beta-\alpha)^{\epsilon}}\right]^{1/p} ,p\in \mathbb{R}\backslash\{-1,0\}; \end{align*}$

(3) The generalized geometric mean

$\begin{align*} G_{\epsilon}(\alpha,\beta) = (\alpha^{\epsilon}\beta^{\epsilon})^{\frac{1}{2}}; \end{align*}$

(4) The generalized harmonic mean

$\begin{align*} H_{\epsilon}(\alpha,\beta) = \frac{(2\alpha\beta)^{\epsilon}}{\alpha^{\epsilon}+\beta^{\epsilon}}. \end{align*}$

Consider the function $\phi: (0, \infty)\rightarrow \mathbb{R}^{\epsilon}$ , $\phi(x) = \frac{\Gamma(1+k\epsilon)}{\Gamma(1+(k+1)\epsilon)}x^{(k+1)\epsilon}$ , $x > 0, k\geq1$ and $q\geq1$ . Because the function $\varphi(x) = |\phi^{(\epsilon)}(x)|^{q} = x^{kq\epsilon}$ is generalized convex and nondecreasing on $(0, \infty)$ , by Proposition 3.3 in ^[22], the function $\varphi(x)$ is generalized harmonically convex on $(0, \infty)$ .

Let $\phi(x) = \frac{\Gamma(1+k\epsilon)}{\Gamma(1+(k+1)\epsilon)}x^{(k+1)\epsilon}$ , $x > 0, k > 1$ and $q > 1$ . Then

$\begin{align*} \phi\Big(\frac{2\alpha\beta}{\alpha+\beta}\Big) = \frac{\Gamma(1+k\epsilon)}{\Gamma(1+(k+1)\epsilon)}H_{\epsilon}^{k+1}(\alpha,\beta), \end{align*}$

$\begin{align*} \frac{\alpha^{\epsilon}\beta^{\epsilon}}{(\beta -\alpha)^{\epsilon}}{}_{\alpha}I_{\beta}^{(\epsilon)} \frac{\phi(x)}{x^{2\epsilon}} = \frac{\Gamma(1+k\epsilon)}{\Gamma(1+(k+1)\epsilon)} L_{(k-1)\epsilon}^{k-1}(\alpha,\beta)G_{\epsilon}^{2}(\alpha,\beta), \end{align*}$

$\begin{align*} \frac{\phi(\beta)-\phi(\alpha)}{2^{\epsilon}} = \frac{(\beta-\alpha)^{\epsilon}}{2^{\epsilon}}L_{k\epsilon}^{k}(\alpha,\beta). \end{align*}$

Proposition 1. From Theorem 2, we obtain the following inequality

$\begin{align*} &\Bigg|H_{\epsilon}^{k+1}(\alpha,\beta)- \Gamma(1+\epsilon)L_{(k-1)\epsilon}^{k-1}(\alpha,\beta)G_{\epsilon}^{2}(\alpha,\beta)\Bigg|\nonumber\\ \leq&\frac{(\beta-\alpha)^{\epsilon}\Gamma(1+(k+1)\epsilon)}{2^{\epsilon}\Gamma(1+k\epsilon)}\Bigg[ L_{k\epsilon}^{k}(\alpha,\beta)+\alpha^{\epsilon}\beta^{\epsilon}\Big(K^{\epsilon}_{1}(\alpha,\beta)\Big)^{1-\frac{1}{q}} \Big(K^{\epsilon}_{2}(\alpha,\beta)\alpha^{kq\epsilon}+ K^{\epsilon}_{3}(\alpha,\beta)\beta^{kq\epsilon}\Big)^{\frac{1}{q}}\Bigg], \end{align*}$

where $K^{\epsilon}_{1}(\alpha, \beta), K^{\epsilon}_{2}(\alpha, \beta)$ and $K^{\epsilon}_{3}(\alpha, \beta)$ as in Theorem 2.

Proposition 2. From Theorem 3, we obtain the following inequality

$\begin{align*} &\Bigg|H_{\epsilon}^{k+1}(\alpha,\beta)- \Gamma(1+\epsilon)L_{(k-1)\epsilon}^{k-1}(\alpha,\beta)G_{\epsilon}^{2}(\alpha,\beta)\Bigg|\nonumber\\ \leq&\frac{(\beta-\alpha)^{\epsilon}\Gamma(1+(k+1)\epsilon)}{2^{\epsilon}\Gamma(1+k\epsilon)}\Bigg[ L_{k\epsilon}^{k}(\alpha,\beta)+\frac{\alpha^{\epsilon}}{\beta^{\epsilon}}\Bigg( \frac{\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}\Bigg)^{\frac{1}{p}} \Bigg(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg)^{\frac{1}{q}}\nonumber\\ &\times\Bigg({}_{2}F_{1}^{\epsilon}\Big(2q,2;3;1-\frac{\alpha}{\beta}\Big)\alpha^{kq\epsilon}+{}_{2}F_{1}^{\epsilon}\Big(2q,1;3;1-\frac{\alpha}{\beta}\Big)\beta^{kq\epsilon}\Bigg)^{\frac{1}{q}}\Bigg], \end{align*}$

where $\frac{1}{p}+\frac{1}{q} = 1, q > 1$ .

Proposition 3. From Theorem 4, we obtain the following inequality

$\begin{align*} &\Bigg|H_{\epsilon}^{k+1}(\alpha,\beta)- \Gamma(1+\epsilon)L_{(k-1)\epsilon}^{k-1}(\alpha,\beta)G_{\epsilon}^{2}(\alpha,\beta)\Bigg|\nonumber\\ \leq&\frac{(\beta-\alpha)^{\epsilon}\Gamma(1+(k+1)\epsilon)}{2^{\epsilon}\Gamma(1+k\epsilon)}\Bigg[ L_{k\epsilon}^{k}(\alpha,\beta)+\frac{\alpha^{\epsilon}}{\beta^{\epsilon}}\Bigg(\frac{{}_{2}F_{1}^{\epsilon}\Big(2p,1;2;1-\frac{\alpha}{\beta}\Big)}{\Gamma(1+\epsilon)}\Bigg)^{\frac{1}{p}} \Bigg(\frac{\Gamma(1+q\epsilon)}{2^{\epsilon}\Gamma(1+(q+1)\epsilon)}\Bigg)^{\frac{1}{q}}\nonumber\\ &\times\Big(\alpha^{kq\epsilon}+\beta^{kq\epsilon}\Big)^{\frac{1}{q}}\Bigg], \end{align*}$

where $\frac{1}{p}+\frac{1}{q} = 1, q > 1$ .

Proposition 4. From Theorem 5, we obtain the following inequality

$\begin{align*} &\Bigg|H_{\alpha}^{k+1}(\alpha,\beta)- \Gamma(1+\epsilon)L_{(k-1)\epsilon}^{k-1}(\alpha,\beta)G_{\epsilon}^{2}(\alpha,\beta)\Bigg|\nonumber\\ \leq&\frac{(\beta-\alpha)^{\epsilon}\Gamma(1+(k+1)\epsilon)}{2^{\epsilon}\Gamma(1+k\epsilon)}\Bigg\{ L_{k\epsilon}^{k}(\alpha,\beta)+\frac{\alpha^{\epsilon}}{\beta^{\epsilon}}\Bigg(\frac{\Gamma(1+p\epsilon)}{\Gamma(1+(p+1)\epsilon)}\Bigg)^{\frac{1}{p}}\Bigg[\Bigg({}_{2}F_{1}^{\epsilon}\Big(2p,1;p+2;1-\frac{\alpha}{\beta}\Big)\Bigg)^{\frac{1}{p}}\nonumber\\ &+\Bigg({}_{2}F_{1}^{\epsilon}\Big(2p,p+1;p+2;1-\frac{\alpha}{\beta}\Big) \Bigg)^{\frac{1}{p}} \Bigg] \Bigg(\frac{\Gamma(1+\epsilon)}{\Gamma(1+2\epsilon)}\Bigg)^{\frac{1}{q}} \Big(\alpha^{kq\epsilon}+\beta^{kq\epsilon}\Big)^{\frac{1}{q}}\Bigg\}, \end{align*}$

where $\frac{1}{p}+\frac{1}{q} = 1, q > 1$ .

5. Conclusions

In this paper, the research on Hermite-Hadamard type inequalities is extended to Yang's fractal space. By using the definitions of generalized harmonically convex function and the theory of local fractional calculus, we construct some new Hermite-Hadamard type integral inequalities for monotonically increasing functions with generalized harmonically convexity. Some applications related to the special mean are established by using the obtained inequalities, which shows that our results have certain application significance. Our research may inspire more scholars to further explore Hermite-Hadamard type integral inequalities on Yang's fractal sets.

Acknowledgments

This work is supported by the Natural Science Foundation of Hunan Province (No. 2020JJ4554) and Scientific Research Project of Hunan Provincial Education Department (No. 18B433).

Conflict of interest

This work does not have any conflicts of interest.

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