EASL – Vol 3 – Issue 2 (2020) – PISRT https://old.pisrt.org Sun, 05 Jul 2020 10:44:20 +0000 en-US hourly 1 https://wordpress.org/?v=6.7 Intuitionistic fuzzy subgroups with respect to norms (\(T,S\)) https://old.pisrt.org/psr-press/journals/easl-vol-3-issue-2-2020/intuitionistic-fuzzy-subgroups-with-respect-to-norms-ts/ Tue, 30 Jun 2020 21:52:15 +0000 https://old.pisrt.org/?p=4213
EASL-Vol. 3 (2020), Issue 2, pp. 40 - 53 Open Access Full-Text PDF
Rasul Rasuli
Abstract: The purpose of this paper is introduce the notion of intuitionistic fuzzy subgroups with respect to norms (\(t\)-norm \(T\) and \(s\)-norm \(S\)). Also we introduce intersection and normality of them and investigate some properties of them. Finally, we provide some results of them under group homomorphisms.
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Engineering and Applied Science Letter

Intuitionistic fuzzy subgroups with respect to norms (\(T,S\))

Rasul Rasuli
Department of Mathematics, Payame Noor University (PNU), Tehran, Iran.; rasulirasul@yahoo.com

Abstract

The purpose of this paper is introduce the notion of intuitionistic fuzzy subgroups with respect to norms (\(t\)-norm \(T\) and \(s\)-norm \(S\)). Also we introduce intersection and normality of them and investigate some properties of them. Finally, we provide some results of them under group homomorphisms.

Keywords:

Group theory, theory of fuzzy sets, intuitionistic fuzzy groups, norms, homomorphisms, intersection.

1. Introduction

Group theory, in modern algebra, the study of groups, which are systems consisting of a set of elements and a binary operation that can be applied to two elements of the set, which together satisfy certain axioms. Groups are vital to modern algebra; their basic structure can be found in many mathematical phenomena. Groups can be found in geometry, representing phenomena such as symmetry and certain types of transformations. Group theory has applications in physics, chemistry, and computer science, and even puzzles like Rubik's Cube can be represented using group theory.

In 1965, Zadeh [1] introduced the notion of fuzzy sets. In 1971, Rosenfled [2] introduced fuzzy sets in the realm of group theory and formulated the concepts of fuzzy subgroups of a group. An increasing number of properties from classical group theory have been generalized. Many authors have worked on fuzzy group theory [3, 4, 5]. Especially, some authors considered the fuzzy subgroups with respect to a t-norm and gave some results [5, 6, 7]. The concept of intuitionistic fuzzy set was introduced by Atanassov [8], as a generalization of the notion of fuzzy set. The theory of intuitionistic fuzzy set is expected to play an important role in modern mathematics in general as it represents a generalization of fuzzy set. After the concept of intuitionistic fuzzy set was introduced, several papers have been published by mathematicians to extend the classical mathematical concepts and fuzzy mathematical concepts to the case of intuitionistic fuzzy mathematics. In the case of intuitionistic fuzzy mathematics, there were some attempts to establish a significant and rational definition of intuitionistic fuzzy group. Zhan and Tan [9] defined intuitionistic fuzzy subgroup as a generalization of Rosenfeld's fuzzy subgroup.

By starting with a given classical group they define intuitionistic fuzzy subgroup using the classical binary operation defined over the given classical group. The author by using norms, investigated some properties of fuzzy algebraic structures [10]. In this paper, by using norms( \(t\)-norm \(T\) and \(s\)-norm \(S\)) we define intuitionistic fuzzy subgroups of group \(G\) as \(IFGN(G)\) and normality of \(G\) as \(NIFGN(G).\) Also we investigate algebriac structures and some related properties of them and prove that if \( A,B \in IFGN(G)\) and \( A,B \in NIFGN(G),\) then \( A \cap B \in IFGN(G)\) and \( A \cap B \in NIFGN(G).\) Next we define normality between \( A,B \in IFGN(G)\) as \( A \blacktriangleright B \) and give characterizations about them. Later we investigate them under group homomorphism \(\varphi: G \to H\) such that if \( A\in IFGN(G)\) and \( B \in IFGN(H),\) then \( \varphi(A) \in IFGN(H)\) and \( \varphi^{-1}(B) \in IFGN(G).\) Also if \( A\in NIFGN(G)\) and \( B \in NIFGN(H),\) then \( \varphi(A) \in NIFGN(H)\) and \( \varphi^{-1}(B) \in NIFGN(G).\) Finally, if \( A,B \in IFGN(G)\) and \( A \blacktriangleright B,\) then \( \varphi(A) \blacktriangleright \varphi(B) \) and if \( A,B \in IFGN(H)\) and \( A \blacktriangleright B,\) then \( \varphi^{-1}(A) \blacktriangleright \varphi^{-1}(B).\)

2. preliminaries

This section contains some basic definitions and preliminary results which will be needed in the sequel. For details we refer to [6, 8, 11, 12, 13, 14, 15, 16].

Definition 1. A group is a non-empty set \( G\) on which there is a binary operation \((a,b) \to ab\) such that

  • (1) if \( a \) and \( b\) belong to \( G \) then \( \)ab is also in \( G\) (closure),
  • (2) \(a(bc) = (ab)c\) for all \(a,b,c \in G\) (associativity),
  • (3) there is an element \( e_{G} \in G\) such that \(ae_{G} = ee_{G}a = a\) for all \(a \in G\) (identity),
  • (4) if \(a \in G,\) then there is an element \(a^{-1} \in G\) such that \(aa^{-1} = a^{-1}a =e_{G}\) (inverse).

One can easily check that this implies the unicity of the identity and of the inverse. A group \( G \) is called abelian if the binary operation is commutative, i.e., \(ab = ba\) for all \(a,b \in G.\)

Remark 1. There are two standard notations for the binary group operation: either the additive notation, that is \((a,b) \to a + b\) in which case the identity is denoted by \( 0\), or the multiplicative notation, that is \((a,b) \to ab\) for which the identity is denoted by \( e. \)

Proposition 1. Let \( G \) be a group. Let \( H\) be a non-empty subset of \( G. \) The following are equivalent:

  • (1) \( H \) is a subgroup of \( G. \)
  • (2) \(x, y \in H\) implies \(xy^{-1} \in H\) for all \( x,y. \)

Definition 2. Let \(H\) be subgroup of group \(G.\) Then we say that \(H\) is normal subgroup of \(G\) if for all \( g\in G \) and \(h\in H\), we have that \( ghg^{-1} \in H. \)

Definition 3. Let \( G \) and \(H \) be any two groups and \( f: G \to H \) be a function. Then \( f \) is called a homomorphism if \( f(xy) = f(x) f(y) \) for all \( x,y \in G. \)

Definition 4. Let \(G\) be an arbitrary group with a multiplicative binary operation and identity \(e\). A fuzzy subset of \(G\), we mean a function from \(G\) into \( [0,1]\).

Definition 5. For sets \( X,Y \) and \( Z, \) \( f=(f_{1},f_{2}): X \to Y \times Z \) is called a complex mapping if \( f_{1} : X \to Y \) and \( f_{2} : X \to Z \) are mappings.

Definition 6. Let \( X \) be a nonempty set. A complex mapping \( A=(\mu_{A},\nu_{A}) : X \to [0,1] \times [0,1]\) is called an intuitionistic fuzzy set (in short, \(IFS\)) in \( X \) if \( \mu_{A}+\nu_{A} \leq 1 \) where the mappings \( \mu_{A} : X \to [0,1] \) and \( \nu_{A} : X \to [0,1] \) denote the degree of membership (namely \( \mu_{A}(x) \)) and the degree of non-membership (namely \( \nu_{A}(x) \)) for each \( x \in X \) to \( A, \) respectively. In particular \( 0_{\sim} \) and \( 1_{\sim} \) denote the intuitionistic fuzzy empty set and intuitionistic fuzzy whole set in \( X \) defined by \( 0_{\sim}(x)=(0,1)\) and \( 1_{\sim}(x)=(1,0),\) respectively. We will denote the set of all \( IFSs \) in \( X \) as \( IFS(X). \)

Definition 7. Let \( X \) be a nonempty set and let \(A=(\mu_{A},\nu_{A})\) and \(B=(\mu_{B},\nu_{B})\) be \( IFSs \) in \( X. \) Then

  • (1) \( A \subset B \) iff \( \mu_{A} \leq \mu_{B} \) and \( \nu_{A} \geq \nu_{B}.\)
  • (2) \( A=B \) iff \( A \subset B \) and \( B \subset A.\)

Definition 8. A \(t\)-norm \(T\) is a function \(T : [0,1]\times [0,1] \to [0,1]\) having the following four properties:

  • (T1) \(T(x,1)=x\) (neutral element),
  • (T2) \(T(x,y)\leq T(x,z)\) if \(y\leq z\) (monotonicity),
  • (T3) \(T(x,y)= T(y,x)\) (commutativity),
  • (T4) \(T(x,T(y,z))=T(T(x,y),z)\) (associativity),
for all \(x,y,z \in[0,1].\)

It is clear that if \(x_{1}\geq x_{2}\) and \(y_{1}\geq y_{2}\), then \(T(x_{1},y_{1}) \geq T(x_{2},y_{2}).\)

Example 1.

  • (1) Standard intersection \(T\)-norm \(T_m(x,y) = \min \{ x,y \}.\)
  • (2) Bounded sum \(T\)-norm \(T_b(x,y) = \max\{0, x+y- 1 \}.\)
  • (3) algebraic product \(T\)-norm \(T_p(x, y) = xy. \)
  • (4) Drastic \(T\)-norm \begin{equation*} T_{D}(x,y) = \left\{ \begin{array}{rl} y &\text{if } x=1\\ x &\text{if } y=1\\ 0 &\text{otherwise. } \\ \end{array} \right. \end{equation*}
  • (5) Nilpotent minimum \(T\)-norm \begin{equation*} T_{nM}(x,y) = \left\{ \begin{array}{rl} \min \lbrace x , y \rbrace &\text{if } x+y >1\\ 0 &\text{otherwise. } \\ \end{array} \right. \end{equation*}
  • (6) Hamacher product \(T\)-norm \begin{equation*} T_{H_{0}}(x,y) = \left\{ \begin{array}{rl} 0 &\text{if } x=y =0\\ \frac{xy}{x+y-xy} &\text{otherwise. } \\ \end{array} \right. \end{equation*}

The drastic \(t\)-norm is the pointwise smallest \(t\)-norm and the minimum is the pointwise largest \(t\)-norm: \(T_{D}(x,y) \leq T(x,y) \leq T_{\min} (x ,y)\) for all \( x,y \in [0,1].\)

Recall that \(t\)-norm \(T\) will be idempotent if for all \(x \in [0,1]\) we have \(T(x, x) =x.\)

Lemma 1. Let \(T\) be a \(t\)-norm. Then $$T(T(x,y),T(w,z))= T(T(x,w),T(y,z)),$$ for all \(x,y,w,z\in [0,1].\)

Definition 9. An \(s\)-norm \(S\) is a function \(S : [0,1]\times [0,1] \to [0,1]\) having the following four properties:

  • (1) \(S(x,0)=x\),
  • (2) \(S(x,y)\leq S(x,z)\) if \(y\leq z\),
  • (3) \(S(x,y)= S(y,x)\),
  • (4) \( S(x,S(y,z))=S(S(x,y),z)\),
for all \(x,y,z \in [0,1].\)

We say that \(S\) is idempotent if for all \(x \in [0,1]\), \(S(x, x) =x.\)

Example 2. The basic \(S\)-norms are \(S_m(x,y) = \max \{ x,y \},\) \(S_b(x,y) = \min\{1, x+y \}\) and \(S_p(x, y) = x+y-xy \) for all \(x,y \in [0,1]\), where \(S_m\) is standard union, \(S_b\) is bounded sum and \(S_p\) is algebraic sum.

Lemma 2. Let \(S\) be a \(s\)-norm. Then \(S(S(x,y),S(w,z))= S(S(x,w),S(y,z)),\) for all \(x,y,w,z\in [0,1].\)

Definition 10. Let \( A=(\mu_{A},\nu_{A}) \in IFS(X)\) and \(B=(\mu_{B},\nu_{B}) \in IFS(X).\) Define intesection \(A\) and \(B\) as $$ A \cap B= (\mu_{A},\nu_{A}) \cap (\mu_{B},\nu_{B})=(\mu_{A \cap B},\nu_{A \cap B})$$ such that \( \mu_{A \cap B}(x)=T(\mu_{A}(x),\mu_{B}(x)) \) and \( \nu_{A \cap B}(x)=S( \nu_{A}(x),\nu_{B}(y))\) for all \( x \in X.\)

Definition 11. Let \(\varphi\) be a function from set \(X\) into set \(Y\) such that \(A = (\mu_{A},v_{A} )\) and \(B = (\mu_{B},v_{B} )\) be two intuitionistic fuzzy sets in X and Y respectively. For all \(x \in X\) and \(y \in Y\), we define \(\varphi(A)(y)=(\varphi(\mu_{A})(y),\varphi(\nu_{A})(y))\) \begin{equation*} =\left\{ \begin{array}{rl} (\sup \{ \mu_{A}(x) \hspace{0.1cm}|\hspace{0.1cm} x\in X,\varphi(x)=y\}, \inf \{ \nu_{A}(x) \hspace{0.1cm}|\hspace{0.1cm} x\in X,\varphi(x)=y\})&\text{if } \varphi^{-1}(y)\neq\emptyset;\\ (0,1) &\text{if } \varphi^{-1}(y)=\emptyset. \end{array} \right. \end{equation*} Also \(\varphi^{-1}(B)(x)=(\varphi^{-1}(\mu_{B})(x),\varphi^{-1}(\nu_{B})(x))=(\mu_{B}(\varphi(x)),\nu_{B}(\varphi(x))).\)

3. Intuitionistic fuzzy subgroups with respect to norms (\(t\)-norm \(T\) and \(s\)-norm \(S\))

Definition 12. Let \( G \) be a group. An \( A=(\mu_{A},\nu_{A}) \in IFS(G)\) is said to be intuitionistic fuzzy subgroup with respect to norms( \(t\)-norm \(T\) and \(s\)-norm \(S\)) (in short, \(IFGN(G)\)) of \( G \) if

  • (1) \(A(xy) \supseteq (T(\mu_{A}(x),\mu_{A}(y)),S(\nu_{A}(x),\nu_{A}(y))),\)
  • (2) \(A(x^{-1}) \supseteq A(x),\)
for all \( x,y \in G. \)

Remark 2. Conditions (1) and (2) of Definition 12 are equivalent to following conditions:

  • (1) \(\mu_{A}(xy)\geq T(\mu_{A}(x),\mu_{A}(y)),\)
  • (2) \(\mu_{A}(x^{-1})\geq\mu_{A}(x),\)
  • (3)\(\nu_{A}(xy) \leq S(\nu_{A}(x),\nu_{A}(y)),\)
  • (4) \(\nu_{A}(x^{-1}) \leq\nu_{A} (x),\)
for all \( x,y \in G. \)

Example 3. Let \((\mathbb{Z},+)\) be a group of integers. For all \(x\in G\) we define a fuzzy subset \(\mu_{A}\) and \(\nu_{A}\) of \(G\) as \begin{equation*} \mu_{A}(x) = \left\{ \begin{array}{rl} 0.65 &\text{if } x\in \{0,\pm2,\pm4,... \};\\ 0.35 &\text{if } x\in \{\pm1,\pm3,... \}. \end{array} \right. \end{equation*} \begin{equation*} \nu_{A}(x) = \left\{ \begin{array}{rl} 0.20 &\text{if } x\in \{0,\pm2,\pm4,... \};\\ 0.80 &\text{if } x\in \{\pm1,\pm3,... \}. \end{array} \right. \end{equation*} Let \(T(x,y)=T_p(x,y) =xy\) and \(S(x,y)=S_p(x,y) =x+y-xy\) for all \(x,y\in [0,1]\), then \(A=(\mu_{A},\nu_{A}) \in IFGN(G).\)

Lemma 3. Let \( A=(\mu_{A},\nu_{A})\in IFS(G)\) such that \(G\) is finite group and \(T\) and \(S\) be idempotent. If \(A=(\mu_{A},\nu_{A})\) satisfies condition (1) of Definition 12, then \( A=(\mu_{A},\nu_{A})\in IFGN(G).\)

Proof. As \(G\) is finite so we have an \(x\in G\) such that \(x\neq e\) and \(x\) has finite order, say \(n> 1\) then \(x^n=e\) and \(x^{-1}=x^{n-1}.\) Now by using condition (1) of Definition 12 repeatedly, we get that $$\mu_{A} (x^{-1})=\mu (x^{n-1})=\mu_{A}(x^{n-2}x)\geq T(\mu_{A} (x^{n-1}),\mu_{A}(x))\geq T(\underbrace{\mu_{A}(x),\mu_{A}(x),...,\mu_{A}(x)}_{n})= \mu_{A}(x)$$ and $$\nu_{A} (x^{-1})=\nu_{A} (x^{n-1})= \nu_{A}(x^{n-2}x) \leq ُ(\nu_{A} (x^{n-1}),\nu_{A}(x)) \leq S(\underbrace{\nu_{A}(x),\nu_{A}(x),...,\nu_{A}(x)}_{n})= \nu_{A}(x).$$ Thus $$A(x^{-1})=(\mu_{A}(x^{-1}),\nu_{A}(x^{-1})) \supseteq (\mu_{A}(x),\nu_{A}(x))=A(x).$$ Hence \( A=(\mu_{A},\nu_{A})\in IFGN(G).\)

Proposition 2. Let \(A=(\mu_{A},\nu_{A})\in IFGN(G)\) and \(T\) and \(S\) be idempotent. Then for all \(x \in G \), and \(n\geq 1,\)

  • (1) \(A(e) \supseteq A(x)\);
  • (2) \(A(x^n) \supseteq A(x);\)
  • (3) \(A(x)=A(x^{-1}).\)

Proof. Let \(x \in G \) and \(n\geq 1.\)

  • (1) $$ \mu_{A}(e)=\mu_{A}(xx^{-1})\geq T(\mu_{A}(x),\mu_{A}(x^{-1}))\geq T(\mu_{A}(x),\mu_{A}(x))=\mu_{A}(x)$$ and $$\nu_{A}(e)=\nu_{A}(xx^{-1}) \leq S(\nu_{A}(x),\nu_{A}(x^{-1}))\leq S(\nu_{A}(x),\nu_{A}(x))=\nu_{A}(x).$$ Hence $$A(e)=(\mu_{A}(e),\nu_{A}(e)) \supseteq (\mu_{A}(x),\nu_{A}(x))=A(x).$$
  • (2) $$\mu_{A}(x^n)=\mu_{A}(\underbrace{xx...x}_{n})\geq T(\underbrace{\mu_{A}(x),\mu_{A}(x),...,\mu_{A}(x)}_{n})= \mu_{A}(x)$$ and $$\nu_{A}(x^n)=\nu_{A}(\underbrace{xx...x}_{n})\leq S(\underbrace{\nu_{A}(x),\nu_{A}(x),...,\nu_{A}(x)}_{n})= \nu_{A}(x).$$ Hence $$A(x^n) =(\mu_{A}(x^n),\nu_{A}(x^n)) \supseteq (\mu_{A}(x),\nu_{A}(x))=A(x).$$
  • (3) As $$\mu_{A}(x)=\mu_{A}((x^{-1}))^{-1}\geq \mu_{A}(x^{-1})\geq\mu_{A}(x) $$ and $$\nu_{A}(x)=\nu_{A}((x^{-1}))^{-1} \leq \nu_{A}(x^{-1}) \leq \nu_{A}(x)=\nu_{A}(x ^{-1}).$$ So \( \mu_{A}(x)=\mu_{A}(x^{-1}) \) and \( \nu_{A}(x)=\nu_{A}(x^{-1}) \), therefore $$A(x)=(\mu_{A}(x),\nu_{A}(x))=(\mu_{A}(x^{-1}),\nu_{A}(x^{-1}))=A(x^{-1}).$$

Proposition 3. Let \(A=(\mu_{A},\nu_{A})\in IFGN(G)\) and \(T\) and \(S\) be idempotent. Then \(A (xy)=A(y)\) if and only if \(A (x)=A(e)\) for all \( x,y \in G. \)

Proof. Let \(A(xy)= A(y)\) for all \( x,y \in G. \) If we let \(y=e\), then we get that \(A (x)=A(e). \) Conversely, suppose that \(A (x)=A(e)\) so from Proposition 2(1), we get that \( A(x) \supseteq A(y) \) and \( A(x) \supseteq A(xy)\) which mean that \(\mu_{A}(x) \geq \mu_{A}(y) \) and \(\mu_{A}(x) \geq \mu_{A}(xy) \) and \(\nu_{A}(x) \leq \nu_{A}(y) \) and \(\nu_{A}(x) \leq \nu_{A}(xy).\) Then \begin{align*}\mu_{A}(xy)&\geq T(\mu_{A}(x),\mu_{A}(y))\\ &\geq T(\mu_{A}(y),\mu_{A}(y))\\ &=\mu_{A}(y)\\ &=\mu_{A}(x^{-1}xy)\\ &\geq T(\mu_{A}(x),\mu_{A}(xy))\\ &\geq T(\mu_{A}(xy),\mu_{A}(xy))=\mu_{A}(xy).\end{align*} So \begin{equation}\label{a} \mu_{A}(xy)=\mu_{A}(y).\end{equation} Also \begin{align*}\nu_{A}(xy) &\leq S(\nu_{A}(x),\nu_{A}(y)) \\ &\leq S(\nu_{A}(y),\nu_{A}(y))\\ &=\nu_{A}(y)\\ &=\nu_{A}(x^{-1}xy)\\ &\leq S(\nu_{A}(x),\nu_{A}(xy))\\ &\leq S(\nu_{A}(xy),\nu_{A}(xy))\\ &=\nu_{A}(xy).\end{align*} So \begin{equation}\label{b}\nu_{A}(xy)=\nu_{A}(y).\end{equation} Hence $$A(xy)=(\mu_{A}(xy),\nu_{A}(xy))=(\mu_{A}(y),\nu_{A}(y))=A(y).$$

Definition 13. Let \(A=(\mu_{A},\nu_{A})\in IFS(G)\) and \(B=(\mu_{B},\nu_{B})\in IFS(G).\) We define the composion of \( A \) and \( B \) as \(A \circ B \in IFS(G)\) such that for all \( x \in G \), we have $$(A \circ B)(x)=((\mu_{A},\nu_{A})\circ (\mu_{B},\nu_{B}))(x)=(\mu_{A \circ B}(x),\nu_{A \circ B}(x))$$ such that \begin{equation*} \mu_{A \circ B}(x) = \left\{ \begin{array}{rl} \sup_{x=yz}T((\mu_{A}(y),\mu_{A}(z)) &\text{if } x=yz;\\ 0 &\text{if } x\neq yz, \end{array} \right. \end{equation*} and \begin{equation*} \nu_{A \circ B}(x) = \left\{ \begin{array}{rl} \inf_{x=yz}S((\nu_{A}(y),\nu_{A}(z)) &\text{if } x=yz;\\ 0 &\text{if } x\neq yz. \end{array} \right. \end{equation*}

Proposition 4. Let \(A^{-1}=(\mu^{-1}_{A},\nu^{-1}_{A})\in IFS(G)\) be the inverse of \(A=(\mu_{A},\nu_{A})\in IFS(G)\) such that for all \(x\in G\) $$A^{-1}(x)=(\mu^{-1}_{A}(x),\nu^{-1}_{A}(x))=(\mu_{A}(x^{-1}),\nu_{A}(x^{-1}))=A(x^{-1}).$$ Let \(T\) and \(S\) be idempotent then \(A\in IFGN(G)\) if and only if \(A\) satisfies the following conditions:

  • (1)\(A \circ A \subseteq A;\)
  • (2) \(A^{-1}=A.\)

Proof. Let \(x,y,z \in G\) such that \(x=yz.\) If \(A=(\mu_{A},\nu_{A}) \in IFGN(G)\), then $$\mu_{A} (x)=\mu_{A} (yz)\geq T(\mu_{A}(y),\mu_{A}(z))=\mu_{A \circ A}(x)$$ and $$\nu_{A} (x)=\nu_{A} (yz)\leq S(\nu_{A}(y),\nu_{A}(z))=\nu_{A \circ A}(x).$$ Which yield $$(A \circ A)(x)=(\mu_{A \circ A}(x),\nu_{A \circ A}(x)) \subseteq (\mu_{A}(x),\nu_{A}(x))=A(x).$$ Then \(A \circ A \subseteq A.\) Also \(A^{-1}=A\) comes from Proposition 2(3). Conversely, let \(A \circ A \subseteq A\) and \(A^{-1}=A.\) As \(A \circ A \subseteq A\), so $$\mu_{A}(yz)=\mu_{A}(x)\geq \mu_{A \circ A}(x)=\sup_{x=yz}T(\mu_{A}(y),\mu_{A}(z))\geq T(\mu_{A}(y),\mu_{A}(z))$$ and $$\nu_{A}(yz)=\nu_{A}(x) \leq \nu_{A \circ A}(x)=\inf_{x=yz}S(\nu_{A}(y),\nu_{A}(z)) \leq S(\nu_{A}(y),\nu_{A}(z)).$$ Which mean that \begin{equation}\label{a1}A(yz)=(\mu_{A}(yz),\nu_{A}(yz)) \supseteq (T(\mu_{A}(y),\mu_{A}(z)),S(\nu_{A}(y),\nu_{A}(z))).\end{equation} As \(A^{-1}=A\), so \begin{equation}\label{b1}(x)=(\mu_{A}(x),\nu_{A}(x))=(\mu^{-1}_{A}(x),\nu^{-1}_{A}(x))=A^{-1}(x).\end{equation} Therefore from (3) and (4) we get that \(A\in IFGN(G).\)

Corollary 1. Let \(A=(\mu_{A},\nu_{A})\in IFGN(G)\) and \(B=(\mu_{B},\nu_{B})\in IFGN(G)\) and \(G\) be commutative group. Then \(A \circ B \in IFGN(G)\) if and only if \(A \circ B =B \circ A .\)

Proof. If \(A, B, A \circ B \in IFGN(G)\), then from Proposition 4 we get that \(A^{-1}=A,B^{-1}=B \) and \((B \circ A)^{-1}=B \circ A.\) Now \( A \circ B = A^{-1} \circ B^{-1}=(B \circ A)^{-1}=B \circ A.\) Conversely, since \(A \circ B = B \circ A\) we have $$(A \circ B)^{-1} =(B \circ A)^{-1}=A^{-1} \circ B^{-1}=A \circ B.$$ Also $$(A \circ B) \circ (A \circ B)=A \circ (B \circ A)\circ B= A \circ (A \circ B) \circ B= (A \circ A) \circ (B \circ B)\subseteq B \circ B.$$ Now Proposition 4 gives us that \(A \circ B \in IFGN(G).\)

Proposition 5. Let \(A=(\mu_{A},\nu_{A})\in IFGN(G)\) and \(B=(\mu_{B},\nu_{B})\in IFGN(G).\) Then \(A \cap B =(\mu_{A \cap B},\nu_{A \cap B}) \in IFGN(G).\)

Proof. Let \( x,y \in G. \) Then \begin{align*}\mu_{A \cap B}(xy)&=T(\mu_{A}(xy),\mu_{B}(xy))\\ &\geq T(T(\mu_{A}(x),\mu_{A}(y)),T(\mu_{B}(x),\mu_{B}(y)))\\ &=T(T(\mu_{A}(x),\mu_{B}(x)),T(\mu_{A}(y),\mu_{B}(y)))\\ &=T(\mu_{A \cap B}(x),\mu_{A \cap B}(y)).\end{align*} And \begin{align*}\nu_{A \cap B}(xy)&=S(\nu_{A}(xy),\nu_{B}(xy))\\ &\leq S(S(\nu_{A}(x),\nu_{A}(y)),S(\nu_{B}(x),\nu_{B}(y)))\\ &=S(S(\nu_{A}(x),\nu_{B}(x)),S(\nu_{A}(y),\nu_{B}(y)))\\ &= S(\nu_{A \cap B}(x),\nu_{A \cap B}(y)).\end{align*} Which mean that $$(A \cap B)(xy) =(\mu_{A \cap B}(xy),\nu_{A \cap B}(xy)) \supseteq (T(\mu_{A \cap B}(x),\mu_{A \cap B}(y)),S(\nu_{A \cap B}(x),\nu_{A \cap B}(y))).$$ Also $$\mu_{A \cap B}(x^{-1})=T(\mu_{A}(x^{-1}),\mu_{B}(x^{-1}))\geq T(\mu_{A}(x),\mu_{B}(x))=\mu_{A \cap B}(x)$$ and $$\nu_{A \cap B}(x^{-1})=S(\nu_{A}(x^{-1}),\nu_{B}(x^{-1}))\leq S(\nu_{A}(x),\nu_{B}(x))=\nu_{A \cap B}(x).$$ So $$(A \cap B)(x^{-1}) =(\mu_{A \cap B}(x^{-1}),\nu_{A \cap B}(x^{-1})) \supseteq (\mu_{A \cap B}(x),\nu_{A \cap B}(x))=(A \cap B)(x).$$ Thus \(A \cap B =(\mu_{A \cap B},\nu_{A \cap B}) \in IFGN(G).\)

Corollary 2. Let \(I_{n}=\{1,2,...,n\}.\) If \(\{A_{i}=(\mu_{A_{i}},\nu_{A_{i}})\hspace{0.1cm} | \hspace{0.1cm}i\in I_{n}\} \subseteq IFGN(G).\) Then \(A=\cap_{i\in I_{n}}A_{i}\in IFGN(G).\)

Definition 14 We say that \(A=(\mu_{A},\nu_{A})\in IFGN(G)\) is normal if for all \(x,y\in G\), \(A(xyx^{-1}) = A (y).\) Also we denote by \(NIFGN(G)\) the set of all normal intuitionistic fuzzy groups with respect to norms (\(t\)-norm \(T\) and \(s\)-norm \(S\)).

Proposition 6. Let \(A=(\mu_{A},\nu_{A})\in NIFGN(G)\) and \(B=(\mu_{B},\nu_{B})\in NIFGN(G).\) Then \(A \cap B =(\mu_{A \cap B},\nu_{A \cap B})\in NIFGN(G).\)

Proof. As Proposition 5 we have that \(A \cap B =(\mu_{A \cap B},\nu_{A \cap B})\in IFGN(G).\) Let \(x,y,\in G\), then $$\mu_{A \cap B}(xyx^{-1})=T(\mu_{A}(xyx^{-1}),\mu_{B}(xyx^{-1})) =T(\mu_{A}(y),\mu_{B}(y))=\mu_{A \cap B}(y)$$ and $$\nu_{A \cap B}(xyx^{-1})=S(\nu_{A}(xyx^{-1}),\nu_{B}(xyx^{-1})) =S(\nu_{A}(y),\nu_{B}(y))=\nu_{A \cap B}(y).$$ Thus $$(A \cap B)(xyx^{-1})=(\mu_{A \cap B}(xyx^{-1}),\nu_{A \cap B}(xyx^{-1}))=(\mu_{A \cap B}(y),\nu_{A \cap B}(y))=(A \cap B)(y).$$ Therefore \(A \cap B =(\mu_{A \cap B},\nu_{A \cap B})\in NIFGN(G).\)

Corollary 3. Let \(I_{n}=\{1,2,...,n\}.\) If \(\{A_{i}=(\mu_{A_{i}},\nu_{A_{i}})\hspace{0.1cm} | \hspace{0.1cm}i\in I_{n}\} \subseteq NIFGN(G).\) Then \(A=\cap_{i\in I_{n}}\mu_{i}\in NIFGN(G).\)

Definition 15. Let \(A=(\mu_{A},\nu_{A})\in IFGN(G)\) and \(B=(\mu_{B},\nu_{B})\in IFGN(G)\) such that \(A \subseteq B.\) Then \(A\) is called normal of \(B\), written \(A \blacktriangleright B\), if for all \(x,y\in G\) we have $$A(xyx^{-1})=(\mu_{A}(xyx^{-1}),\nu_{A}(xyx^{-1})) \supseteq ( T(\mu_{A}(y), \mu_{B}(x)),S(\nu_{A}(y), \nu_{B}(x))).$$

Proposition 7.

  • (1) Let \(G_{1}\) and \(G_{2}\) are subgroups of \(G.\) Then \(G_{1}\) is a normal subgroup of \(G_{2}\) if and only if \(1_{G_{1}}\blacktriangleright 1_{G_{2}}.\)
  • (2) If \(T\) and \(S\) be idempotent, then every intuitionistic fuzzy subgroup with respect to norms( \(t\)-norm \(T\) and \(s\)-norm \(S\)) is normal fuzzy subgroup of itself.

Proof.

  • (1) Let \(x\in G_{2}\) and \(y\in G_{1}\) then \( 1_{G_{2}}(x)=1 \) and \( 1_{G_{1}}(y)=1.\) If \({G_{1}} \unrhd {G_{2}}\), then \(xyx^{-1}\in G_{1}\) and so \( 1_{G_{1}}(xyx^{-1})=1.\) As \(1_{G}=(1_{G},1_{G}) \in IFGN(G)\), so $$1_{G_{1}}(xyx^{-1})=1 \geq 1=T(1,1)=T(1_{G_{1}}(y),1_{G_{2}}(x))$$ and $$1_{G_{1}}(xyx^{-1})=1 \leq 1=S(1,1)=S(1_{G_{1}}(y),1_{G_{2}}(x)).$$ Then $$1_{G_{1}}(xyx^{-1})=(1_{G_{1}}(xyx^{-1}),1_{G_{1}}(xyx^{-1})) \supseteq (T(1_{G_{1}}(y),1_{G_{2}}(x)),S(1_{G_{1}}(y),1_{G_{2}}(x))).$$ Hence \(1_{G_{1}}\blacktriangleright 1_{G_{2}}.\)
  • (2) Let \( A=(\mu_{A},\nu_{A})\in IFGN(G) \) and \( x,y \in G \) then \begin{align*}\mu_{A} (xyx^{-1})&\geq T(\mu_{A} (xy),\mu_{A} (x^{-1}))\\ &\geq T(T(\mu_{A}(x),\mu_{A}(y)),\mu_{A}(x))\\ &= T(T(\mu_{A}(y),\mu_{A}(x)),\mu_{A}(x))\\ &=T(\mu_{A}(y),T(\mu_{A}(x),\mu_{A}(x))) \\ &= T(\mu_{A}(y),\mu_{A}(x)).\end{align*} And \begin{align*}\nu_{A} (xyx^{-1}) &\leq S(\nu_{A} (xy),\nu_{A} (x^{-1})) \\ &\leq S(S(\nu_{A}(x),\nu_{A}(y)),\nu_{A}(x))\\ &= S(S(\nu_{A}(y),\nu_{A}(x)),\nu_{A}(x))\\ &=S(\nu_{A}(y),S(\nu_{A}(x),\nu_{A}(x))) \\ &= S(\nu_{A}(y),\nu_{A}(x)).\end{align*} Thus $$A(xyx^{-1})=(\mu_{A}(xyx^{-1}),\nu_{A}(xyx^{-1})) \supseteq ( T(\mu_{A}(y), \mu_{A}(x)),S(\nu_{A}(y), \nu_{B}(x))).$$ Hence \(A =(\mu_{A},\nu_{A}) \blacktriangleright A =(\mu_{A},\nu_{A}).\)

Proposition 8. Let \( A=(\mu_{A},\nu_{A})\in NIFGN(G) \) and \(B=(\mu_{B},\nu_{B})\in IFGN(G)\) such that \(T\) and \(S\) be idempotent. Then \( A \cap B \blacktriangleright B. \)

Proof. Using Proposition 5, we get that \( A \cap B \in IFGN(G).\) Let \( x,y \in G \), then \begin{align*}\mu_{A \cap B}(xyx^{-1})&=T(\mu_{A}(xyx^{-1}),\mu_{B}(xyx^{-1}))\\ &=T(\mu_{A}(y),\mu_{B}(xyx^{-1})) \\ &\geq T(\mu_{A}(y),T(\mu_{B}(xy),\mu_{B}(x^{-1}))\\ & \geq T(\mu_{A}(y),T(T(\mu_{B}(x),\mu_{B}(y)),\mu_{B}(x)))\\ &=T(\mu_{A}(y),T(\mu_{B}(y),T(\mu_{B}(x),\mu_{B}(x))))\\ &=T(\mu_{A}(y),T(\mu_{B}(y),\mu_{B}(x)))\\ &=T(T(\mu_{A}(y),\mu_{B}(y)),\mu_{B}(x))\\ &=T(\mu_{A \cap B}(y),\mu_{B}(x)).\end{align*} And \begin{align*}\nu_{A \cap B}(xyx^{-1})&=S(\nu_{A}(xyx^{-1}),\nu_{B}(xyx^{-1}))\\ &=S(\nu_{A}(y),\nu_{B}(xyx^{-1})) \\ &\leq S(\nu_{A}(y),S(\nu_{B}(xy),\nu_{B}(x^{-1})) \\ &\leq S(\nu_{A}(y),S(S(\nu_{B}(x),\nu_{B}(y)),\nu_{B}(x)))\\ &=S(\nu_{A}(y),S(\nu_{B}(y),S(\nu_{B}(x),\nu_{B}(x))))\\ &=S(\nu_{A}(y),S(\nu_{B}(y),\nu_{B}(x)))\\ &=S(S(\nu_{A}(y),\nu_{B}(y)),\nu_{B}(x))\\ &=S(\nu_{A \cap B}(y),\nu_{B}(x)).\end{align*} Thus $$(A \cap B)(xyx^{-1}) =(\mu_{A \cap B}(xyx^{-1}),\nu_{A \cap B}(xyx^{-1})) \supseteq (T(\mu_{A \cap B}(y),\mu_{B}(x)),S(\nu_{A \cap B}(y),\nu_{B}(x))).$$ Which means that \( A \cap B \blacktriangleright B. \)

Proposition 10. Let \( A=(\mu_{A},\nu_{A})\in IFGN(G) \) and \(B=(\mu_{B},\nu_{B})\in IFGN(G)\) and \(C=(\mu_{C},\nu_{C})\in IFGN(G)\) such that \(T\) and \(S\) be idempotent. If \( A \blacktriangleright C\) and \(B \blacktriangleright C, \) then \( A \cap B \blacktriangleright C. \)

Proof. By Proposition 5 we will have that \( A \cap B \in IFGN(G).\) Let \( x,y \in G \), then \begin{align*}\mu_{A \cap B}(xyx^{-1})&= T(\mu_{A}(xyx^{-1}),\mu_{B}(xyx^{-1}))\\ &\geq T(T(\mu_{A}(y),\mu_{C}(x)),T(\mu_{B}(y),\mu_{C}(x)))\\ &=T(T(\mu_{A}(y),\mu_{B}(y)),T(\mu_{C}(x),\mu_{C}(x)))\\ &=T(T(\mu_{A}(y),\mu_{B}(y)),\mu_{C}(x))=T(\mu_{A \cap B}(y),\mu_{C}(x)).\end{align*} And \begin{align*}\nu_{A \cap B}(xyx^{-1})&= S(\nu_{A}(xyx^{-1}),\nu_{B}(xyx^{-1}))\\ & \leq S(S(\nu_{A}(y),\nu_{C}(x)),S(\nu_{B}(y),\nu_{C}(x)))\\ &=S(S(\nu_{A}(y),\nu_{B}(y)),S(\nu_{C}(x),\nu_{C}(x)))\\ &=S(S(\nu_{A}(y),\nu_{B}(y)),\nu_{C}(x))=S(\nu_{A \cap B}(y),\nu_{C}(x)).\end{align*} Therefore $$(A \cap B)(xyx^{-1})=(\mu_{A \cap B}(xyx^{-1}),\nu_{A \cap B}(xyx^{-1})) \supseteq (T(\mu_{A \cap B}(y),\mu_{C}(x)),S(\nu_{A \cap B}(y),\nu_{C}(x))).$$ Hence \( A \cap B \blacktriangleright C. \)

Corollary 4. Let \(I_{n}=\{1,2,...,n\}\) and \(\{A_{i}=(\mu_{A_{i}},\nu_{A_{i}})\hspace{0.1cm} | \hspace{0.1cm}i\in I_{n}\} \subseteq IFGN(G)\) such that \(\{A_{i}=(\mu_{A_{i}},\nu_{A_{i}})\hspace{0.1cm} | \hspace{0.1cm}i\in I_{n}\} \blacktriangleright B=(\mu_{B},\nu_{B}).\) Then \(A=\cap_{i\in I_{n}}A_{i} \blacktriangleright B=(\mu_{B},\nu_{B}).\)

4. Homomorphisms of \( IFGN(G) \)

Proposition 10. Let \( A=(\mu_{A},\nu_{A})\in IFGN(G) \) and \( H\) be a group. Suppose that \(\varphi:G \to H\) is a homomorphism. Then \(\varphi(A)\in IFGN(H).\)

Proof. Let \(u,v\in H\) and \(x,y \in G\) such that \(u=\varphi(x)\) and \(v=\varphi(y)\) and \( \varphi(A)=(\varphi(\mu_{A}),\varphi(\nu_{A})).\) Now \begin{align*}\varphi(\mu_{A})(uv)&=\sup \{\mu_{A}(xy)\hspace{0.1cm} |\hspace{0.1cm} u=\varphi(x),v=\varphi(y)\}\\ &\geq \sup\{T(\mu_{A}(x),\mu_{A}(y))\hspace{0.1cm} | \hspace{0.1cm} u=\varphi(x),v=\varphi(y)\}\\ &=T(\sup \{\mu_{A}(x)\hspace{0.1cm} |\hspace{0.1cm} u=f(x)\},\sup \{\mu_{A}(y) \hspace{0.1cm}|\hspace{0.1cm} v=\varphi(y)\})\\ &=T(\varphi(\mu_{A})(u),\varphi(\mu_{A})(v))\end{align*} and \begin{align*}\varphi(\nu_{A})(uv)&=\inf \{\nu_{A}(xy)\hspace{0.1cm} |\hspace{0.1cm} u=\varphi(x),v=\varphi(y)\} \\ &\leq \inf \{S(\nu_{A}(x),\nu_{A}(y))\hspace{0.1cm} | \hspace{0.1cm} u=\varphi(x),v=\varphi(y)\}\\ &=S(\inf \{\nu_{A}(x)\hspace{0.1cm} |\hspace{0.1cm} u=f(x)\},\inf \{\nu_{A}(y) \hspace{0.1cm}|\hspace{0.1cm} v=\varphi(y)\})\\ &=S(\varphi(\nu_{A})(u),\varphi(\nu_{A})(v)).\end{align*} Which mean that $$\varphi(A)(uv) \supseteq (T(\varphi(\mu_{A})(u),\varphi(\mu_{A})(v)),S(\varphi(\nu_{A})(u),\varphi(\nu_{A})(v))).$$ Also \begin{align*}\varphi(\mu_{A})(u^{-1})&=\sup \{\mu_{A}(x^{-1})\hspace{0.1cm} |\hspace{0.1cm} u^{-1}=\varphi(x^{-1}) \}\\ & =\sup \{\mu_{A}(x^{-1})\hspace{0.1cm} |\hspace{0.1cm} u^{-1}=\varphi^{-1}(x) \} \\ & \geq \sup \{\mu_{A}(x)\hspace{0.1cm} |\hspace{0.1cm} u=\varphi(x) \}\\ &=\varphi(\mu_{A})(u)\end{align*} and \begin{align*}\varphi(\nu_{A})(u^{-1})&=\inf \{\nu_{A}(x^{-1})\hspace{0.1cm} |\hspace{0.1cm} u^{-1}=\varphi(x^{-1}) \}\\ & =\inf \{\nu_{A}(x^{-1})\hspace{0.1cm} |\hspace{0.1cm} u^{-1}=\varphi^{-1}(x) \} \\ & \leq \inf \{\nu_{A}(x)\hspace{0.1cm} |\hspace{0.1cm} u=\varphi(x) \}\\ &=\varphi(\nu_{A})(u).\end{align*} Thus $$\varphi(A)(u^{-1})=(\varphi(\mu_{A})(u^{-1}),\varphi(\nu_{A})(u^{-1})) \supseteq (\varphi(\mu_{A})(u),\varphi(\nu_{A})(u))= \varphi(A)(u). $$ Therefore \(\varphi(A)\in IFGN(H).\)

Proposition 11. Let \( H\) be a group and \( B=(\mu_{B},\nu_{B})\in IFGN(H).\) Suppose that \(\varphi:G \to H\) is a homomorphism. Then \(\varphi^{-1}(B)\in IFGN(G).\)

Proof. Let \( x,y \in G \) and \(\varphi^{-1}(B)=(\varphi^{-1}(\mu_{B}),\varphi^{-1}(\nu_{B}))=(\mu_{B}(\varphi),\nu_{B}(\varphi).\) Now $$\varphi^{-1}(\mu_{B})(xy)=\mu_{B}(\varphi(xy))=\mu_{B}(\varphi(x)\varphi(y)) \geq T(\mu_{B}(\varphi(x)),\mu_{B}(\varphi(y)))=T(\varphi^{-1}(\mu_{B})(x),\varphi^{-1}(\mu_{B})(y))$$ and $$\varphi^{-1}(\nu_{B})(xy)=\nu_{B}(\varphi(xy))=\nu_{B}(\varphi(x)\varphi(y)) \leq S(\nu_{B}(\varphi(x)),\nu_{B}(\varphi(y)))=S(\varphi^{-1}(\nu_{B})(x),\varphi^{-1}(\nu_{B})(y)).$$ So $$\varphi^{-1}(B)(xy) \supseteq (T(\varphi^{-1}(\mu_{B})(x),\varphi^{-1}(\mu_{B})(y)),S(\varphi^{-1}(\nu_{B})(x),\varphi^{-1}(\nu_{B})(y))).$$ Also $$\varphi^{-1}(\mu_{B})(x^{-1})=\mu_{B}(\varphi(x^{-1}))=\mu_{B}(\varphi^{-1}(x)) \geq \mu_{B}(\varphi(x))=\varphi^{-1}(\mu_{B})(x)$$ and $$\varphi^{-1}(\nu_{B})(x^{-1})=\nu_{B}(\varphi(x^{-1}))=\nu_{B}(\varphi^{-1}(x)) \leq \nu_{B}(\varphi(x))=\varphi^{-1}(\nu_{B})(x).$$ Thus $$\varphi^{-1}(B)(x^{-1})=(\varphi^{-1}(\mu_{B})(x^{-1}),\varphi^{-1}(\nu_{B})(x^{-1})) \supseteq (\varphi^{-1}(\mu_{B})(x),\varphi^{-1}(\nu_{B})(x))=\varphi^{-1}(B)(x).$$ Hence \(\varphi^{-1}(B)\in IFGN(G).\)

Proposition 12. Let \( A=(\mu_{A},\nu_{A})\in NIFGN(G) \) and \( H\) be a group. Suppose that \(\varphi:G \to H\) is a homomorphism. Then \(\varphi(A)\in NIFGN(H).\)

Proof. As Proposition 10 we have that \(\varphi(A)\in IFGN(H).\) Let \( x,y \in H \) such that \( \varphi(u)=x \) and \( \varphi(w)=y \) with \( u,w \in G. \) Then \begin{align*}\varphi(\mu_{A}(xyx^{-1}))&=\sup \{\mu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=xyx^{-1}\}\\ &=\sup \{\mu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=\varphi(u)\varphi(w)\varphi(u^{-1}) \}\\ &=\sup \{\mu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=\varphi(uwu^{-1}) \}\\ &=\sup \{\mu_{A}(uwu^{-1})\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(uwu^{-1})=y \}\\ &=\sup \{\mu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=y \}\\ &=\varphi(\mu_{A}(y))\end{align*} and \begin{align*}\varphi(\nu_{A}(xyx^{-1}))&=\inf \{\nu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=xyx^{-1}\}\\ &=\inf \{\nu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=\varphi(u)\varphi(w)\varphi(u^{-1}) \}\\ &=\inf \{\nu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=\varphi(uwu^{-1}) \}\\ &=\inf \{\nu_{A}(uwu^{-1})\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(uwu^{-1})=y \}\\ &=\inf \{\nu_{A}(w)\hspace{0.1cm} |\hspace{0.1cm} w\in G, \varphi(w)=y \}\\ &=\varphi(\nu_{A}(y)).\end{align*} Which yield $$\varphi(A)(xyx^{-1}))=(\varphi(\mu_{A}(xyx^{-1})),\varphi(\nu_{A}(xyx^{-1})))=(\varphi(\mu_{A}(y)),\varphi(\nu_{A}(y)))=\varphi(A)(y)).$$ Thus \(\varphi(A)\in NIFGN(H).\)

Proposition 13. Let \( H\) be a group and \( B=(\mu_{B},\nu_{B})\in NIFGN(H).\) Suppose that \(\varphi:G \to H\) is a homomorphism. Then \(\varphi^{-1}(B)\in NIFGN(G).\)

Proof. By Proposition 11 we get that \(\varphi^{-1}(B)\in IFGN(G).\) Let \( x,y \in G \), then \begin{align*}\varphi^{-1}(\mu_{B})(xyx^{-1})&=\mu_{B}(\varphi(xyx^{-1}))\\ &=\mu_{B}(\varphi(x)\varphi(y)\varphi(x^{-1}))\\ &=\mu_{B}(\varphi(x)\varphi(y)\varphi^{-1}(x))\\ &=\mu_{B}(\varphi(y))\\ &=\varphi^{-1}(\mu_{B})(y)\end{align*} and \begin{align*}\varphi^{-1}(\nu_{B})(xyx^{-1})&=\nu_{B}(\varphi(xyx^{-1}))\\ &=\nu_{B}(\varphi(x)\varphi(y)\varphi(x^{-1}))\\ &=\nu_{B}(\varphi(x)\varphi(y)\varphi^{-1}(x))\\ &=\nu_{B}(\varphi(y))\\ &=\varphi^{-1}(\nu_{B})(y).\end{align*} Then $$\varphi^{-1}(B)(xyx^{-1})=(\varphi^{-1}(\mu_{B})(xyx^{-1}),\varphi^{-1}(\nu_{B})(xyx^{-1}))=(\varphi^{-1}(\mu_{B})(y),\varphi^{-1}(\nu_{B})(y))=\varphi^{-1}(B)(y).$$ Thus \(\varphi^{-1}(B)\in NIFGN(G).\)

Proposition 14. Let \( A=(\mu_{A},\nu_{A})\in IFGN(G) \) and \(B=(\mu_{B},\nu_{B})\in IFGN(G)\) such that \( A \blacktriangleright B.\) If \(\varphi:G \to H\) is a homomorphism, then \(\varphi(A) \blacktriangleright \varphi(B).\)

Proof. Using Proposition 10 we will have that \( \varphi(A) \in IFGN(H) \) and \( \varphi(B) \in IFGN(H).\) Let \(x,y\in H\) and \(u,v \in G\), then \begin{align*}\varphi(\mu_{A})(xyx^{-1})&= \sup \{\mu_{A}(z)\hspace{0.1cm}|\hspace{0.1cm} z\in G, \varphi(z)=xyx^{-1}\}\\ & =\sup \{\mu_{A}(uvu^{-1})\hspace{0.1cm}|\hspace{0.1cm} u,v\in G, \varphi(u)=x,\varphi(v)=y\}\\ &\geq\sup \{T(\mu_{A}(v),\mu_{B}(u))\hspace{0.1cm}|\hspace{0.1cm}\varphi(u)=x,\varphi(v)=y\}\\ &=T(\sup \{\mu_{A}(v)\hspace{0.1cm} |\hspace{0.1cm} y=\varphi(v)\},\sup \{\mu_{B}(u) \hspace{0.1cm}|\hspace{0.1cm} x=\varphi(u)\})\\ &=T(\varphi(\mu_{A})(y),\varphi(\mu_{B})(x))\end{align*} and \begin{align*}\varphi(\nu_{A})(xyx^{-1})&= \inf \{\nu_{A}(z)\hspace{0.1cm}|\hspace{0.1cm} z\in G, \varphi(z)=xyx^{-1}\}\\ &=\inf \{\nu_{A}(uvu^{-1})\hspace{0.1cm}|\hspace{0.1cm} u,v\in G, \varphi(u)=x,\varphi(v)=y\}\\ &\leq \inf \{S(\nu_{A}(v),\nu_{B}(u))\hspace{0.1cm}|\hspace{0.1cm}\varphi(u)=x,\varphi(v)=y\}\\ &=S(\inf \{\nu_{A}(v)\hspace{0.1cm} |\hspace{0.1cm} y=\varphi(v)\},\inf \{\nu_{B}(u) \hspace{0.1cm}|\hspace{0.1cm} x=\varphi(u)\})\\ &=S(\varphi(\nu_{A})(y),\varphi(\nu_{B})(x)).\end{align*} Then \begin{align*} \varphi(A)(xyx^{-1})&=(\varphi(\mu_{A})(xyx^{-1}),\varphi(\nu_{A})(xyx^{-1}))\\ & \supseteq (T(\varphi(\mu_{A})(y),\varphi(\mu_{B})(x)),S(\varphi(\nu_{A})(y),\varphi(\nu_{B})(x))).\end{align*} Thus \(\varphi(A) \blacktriangleright \varphi(B).\)

Proposition 15. Let \( A=(\mu_{A},\nu_{A})\in IFGN(H) \) and \(B=(\mu_{B},\nu_{B})\in IFGN(H)\) such that \( A \blacktriangleright B.\) If \(\varphi:G \to H\) is a homomorphism, then \(\varphi^{-1}(A) \blacktriangleright \varphi^{-1}(B).\)

Proof. As Proposition 11 we will have that \( \varphi^{-1}(A) \in IFGN(G)\) and \( \varphi^{-1}(B) \in IFGN(G).\) Let \(x,y\in G\), then \begin{align*}\varphi^{-1}(\mu_{A})(xyx^{-1})&=\mu_{A}(\varphi(xyx^{-1}))\\ &=\mu_{A}(\varphi(x)\varphi(y)\varphi(x^{-1}))\\ &=\mu_{A}(\varphi(x)\varphi(y)\varphi^{-1}(x)) \\ &\geq T(\mu_{A}(\varphi(y)),\mu_{B}(\varphi(x)))\\ &=T(\varphi^{-1}(\mu_{A})(y),\varphi^{-1}(\mu_{B})(x)) \end{align*} and \begin{align*}\varphi^{-1}(\nu_{A})(xyx^{-1})&=\nu_{A}(\varphi(xyx^{-1}))\\ &=\nu_{A}(\varphi(x)\varphi(y)\varphi(x^{-1}))\\ &=\nu_{A}(\varphi(x)\varphi(y)\varphi^{-1}(x)) \\ & \leq S(\nu_{A}(\varphi(y)),\nu_{B}(\varphi(x)))\\ &=S(\varphi^{-1}(\nu_{A})(y),\varphi^{-1}(\nu_{B})(x)).\end{align*} Then \begin{align*}\varphi^{-1}(A)(xyx^{-1})&=(\varphi^{-1}(\mu_{A})(xyx^{-1}),\varphi^{-1}(\nu_{A})(xyx^{-1}))\\ &\supseteq (T(\varphi^{-1}(\mu_{A})(y),\varphi^{-1}(\mu_{B})(x)),S(\varphi^{-1}(\nu_{A})(y),\varphi^{-1}(\nu_{B})(x))).\end{align*} Thus \(\varphi^{-1}(A) \blacktriangleright \varphi^{-1}(B).\)

Acknowledgments

I would like to thank the reviewers for carefully reading the manuscript and making several helpful comments to increase the quality of the paper.

Autho Contributions

All authors contributed equally to the writing of this paper. All authors read and approved the final manuscript.

Conflict of Interests

The author declares no conflict of interest.

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On Caputo fractional derivatives via exponential \((s,m)\)-convex functions https://old.pisrt.org/psr-press/journals/easl-vol-3-issue-2-2020/on-caputo-fractional-derivatives-via-exponential-sm-convex-functions/ Tue, 30 Jun 2020 21:15:01 +0000 https://old.pisrt.org/?p=4211
EASL-Vol. 3 (2020), Issue 2, pp. 32 - 39 Open Access Full-Text PDF
Saad Ihsan Butt, Mehroz Nadeem, Ghulam Farid
Abstract: In this paper, we establish several integral inequalities including Caputo fractional derivatives for exponential \((s,m)\)-convex functions. By using convexity for exponential \((s,m)\)-convex functions of any positive integer order differentiable function some novel results are obtained.
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Engineering and Applied Science Letter

On Caputo fractional derivatives via exponential \((s,m)\)-convex functions

Saad Ihsan Butt\(^1\), Mehroz Nadeem, Ghulam Farid
Department of Mathematics, COMSATS University of Islamabad, Lahore Campus, Pakistan.; (S.I.B & M.N)
Department of Mathematics COMSATS University of Islamabad, Attock Campus, Pakistan.; (G.F)

\(^{1}\)Corresponding Author: saadihsanbutt@cuilahore.edu.pk

Abstract

In this paper, we establish several integral inequalities including Caputo fractional derivatives for exponential \((s,m)\)-convex functions. By using convexity for exponential \((s,m)\)-convex functions of any positive integer order differentiable function some novel results are obtained.

Keywords:

Convex function, exponential \((s,m)\)-convex functions, Caputo-fractional derivatives.

1. Introduction

Convexity plays an important role in many features of mathematical programming including, for example, sufficient optimality conditions and duality theorems. The topic of convex functions has been treated extensively in the classical book by Hardy, Littlewood and Polya [1]. The study of fractional order derivatives and integrals is called fractional calculus. Fractional calculus have important applications in all fields of applied sciences. Fractional integration and fractional differentiation appear as basic part in the subject of partial differential equations [2, 3]. Many types of fractional integral as well as differential operators have been defined in literature. Classical Caputo-fractional derivatives were introduced by Michele Caputo in [4] in 1967. Toader [5] defined the \(m\)-convexity as follows:

Definition 1. The function \(\Psi:[u,v] \rightarrow\mathbb{R},\) is said to be convex, if we have% \begin{equation*} \Psi\left( \tau z_{1}+(1-\tau) z_{2}\right) \leq \tau \Psi(z_{1}) +\left( 1-\tau\right) \Psi( z_{2}) \end{equation*} for all \(z_{1},z_{2}\in [u,v] \) and \(\tau\in [0,1] .\)

Definition 2.(see[6]) The function \(\Psi:I\subseteq \Re \) is exponential-convex, if \begin{equation*} \Psi\left( \tau z_{1}+(1-\tau) z_{2}\right) \leq \tau e^{-\alpha z_{1}}\Psi(z_{1}) +(1-\tau) e^{-\alpha z_{2}}\Psi( z_{2}) \end{equation*} for all\(\;\tau\in [0,1] \;\)and \(z_{1},z_{2}\in I\) and \(\alpha\in \Re\).

Definition 3.(see[7]) The function \(\Psi:I\subset[0,\infty)\longrightarrow \Re \) is \(s\)-convex in second sense with \(s\in [0,1] ,\;\) if \begin{equation*} \ \Psi\left( \tau z_{1}+(1-\tau) z_{2}\right) \leq \tau^{s}\Psi(z_{1}) +(1-\tau) ^{s}\Psi( z_{2}) \end{equation*} for all\(\;\tau\in [0,1) \;\)and \(z_{1},z_{2}\in I\) and \(\alpha\in \Re.\)

Definition 4.(see[8]) The function \(\Psi:I\subset[0,\infty)\longrightarrow \Re\) is exponential \(s\)-convex in second sense with \(s\in [0,1] ,\;\) if \begin{equation*} \ \Psi\left( \tau z_{1}+(1-\tau) z_{2}\right) \leq \tau^{s}e^{-\beta z_{1}}\Psi(z_{1}) +(1-\tau) ^{s}e^{-\beta z_{2}}\Psi( z_{2}) \ \end{equation*} for\ all\(\;\tau\in [0,1] \;\)and\ \(z_{1},z_{2}\in I\) and \(\beta\in \Re.\)

Definition 5.(see[9]) The function \(\Psi:K\rightarrow \Re \) is \((s,m)\)-convex in second sense with \(s\in [0,1] ,\;\) and \(K\subseteq [0,\infty]\) be an interval, if \begin{equation*} \ \Psi\left( \tau z_{1}+(1-\tau)z_{2} \right) \leq \tau^{s}\Psi(z_{1}) +(1-\tau) ^{s}m \Psi( z_{2}) \end{equation*} for all\(\;\tau\in [0,1] \;\)and \(z_{1},z_{2}\in [0,\infty]\).

Definition 6. The function \(\Psi:K\rightarrow \Re \) is exponential \((s,m)\)-convex in second sense with \(s\in [0,1] ,\;\) and \(K\subseteq [0,\infty]\) be an interval, if \begin{equation*} \Psi\left( \tau z_{1}+(1-\tau) z_{2}\right) \leq \tau^{s}e^{-\beta z_{1}}\Psi(z_{1}) +(1-\tau) ^{s}e^{-\beta z_{2}}m \Psi( z_{2}) \ \end{equation*} for all\(\;\tau\in [0,1] \;\)and\ \(z_{1},z_{2}\in [0,\infty]\) and \(\beta\in \Re.\)

The previous era of fractional calculus is as old as the history of differential calculus. They generalize the differential operators and ordinary integral. However, the fractional derivatives have some basic properties than the corresponding classical ones. On the other hand, besides the smooth requirement, Caputo derivative does not coincide with the classical derivative [10]. We give the following definition of Caputo fractional derivatives, see [2, 11, 12, 13].

Definition 7. let \(\Psi\in AC^n[u,v]\) be a space of functions having \(nth\) derivatives absolutely continuous with \(\lambda>0\) and \(\lambda \notin\{1, 2, 3, . . . \}\), \(n = [\lambda]+1\). The right sided Caputo fractional derivative is as follows:

\begin{align} &({^C}D^{\lambda}_{u+}\Psi)(z)=\frac{1}{\Gamma(n-\lambda)}\int^{z}_{u}\frac{\Psi^{(n)} {(\tau)}}{(z-\tau)^{{\lambda}-n+1}}d\tau , z>u. \end{align}
(1)
The left sided caputo fractional derivative is as follows:
\begin{align} &({^C}D^{\lambda}_{v-}\Psi)(z)=\frac{(-1)^n}{\Gamma(n-\lambda)}\int^{v}_{z}\frac{\Psi^{(n)} {(\tau)}}{(\tau-z)^{{\lambda}-n+1}}d\tau , z< v. \end{align}
(2)
The Caputo fractional derivative \(({^C}D^{n}_{u+}\Psi)(z)\) coincides with \(\Psi^{(n)}(z)\) whereas \(({^C}D^{n}_{v-}\Psi)(z)\) coincides with \(\Psi^{(n)}(z)\) with exactness to a constant multiplier \((-1)^{n}\), if \(\Lambda = n \in \{1, 2, 3, . . . \}\) and usual derivative \(\Psi^{(n)}(z)\) of order \(n\) exists. In particular. we have
\begin{align} &({^C}D^{0}_{u+}\Psi)(z)=({^C}D^{0}_{v-}\Psi)(z)= \Psi(z) \end{align}
(3)
where \(n=1\) and \(\lambda=0\).

In this paper, we establish several new integral inequalities including Caputo fractional derivatives for exponential \((s,m)\)-convex functions. By using convexity for exponential \((s,m)\)-convex functions of any positive integer order differentiable function some novel results are given. The purpose of this paper is to introduce some fractional inequalities for the Caputo-fractional derivatives via \((s,m)\)-convex functions which have derivatives of any integer order.

2. Main Results

First we give the following estimate of the sum of left and right handed Caputo fractional derivatives.

Theorem 1. Let \(f:I\longrightarrow \mathbb{R}\) be a real valued \(n\)-time differentiable function where \(n\) is a positive integer. If \(f^{(n)}\) is a positive \((s,m)\)-convex function, then for \(u,v\in I;u< v\) and \(\lambda_{1},\lambda_{2}\geq1\), the following inequality for Caputo fractional derivatives holds:

\begin{align}\label{0010} &\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}-1}_{u+}f)(u)+\Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}-1}_{v-}f)(u) \\&\leq \dfrac{(z-u)^{n-\lambda_{1}+1}e^{-\beta u}f^{(n)}(u)+(v-z)^{n-\lambda_{2}+1}e^{-\beta v}f^{(n)}(v)}{s+1}+(m)e^{-\beta z}f^{(n)}(z)\bigg[\dfrac{(z-u)^{n-\lambda_{1}+1}+(v-z)^{n-\lambda_{2}+1}}{s+1}\bigg]\notag. \end{align}
(4)

Proof. Let us consider the function \(f\) on the interval \([u,z], z \in [u,v]\) and \(n\) is a positive integer. For \(\tau \in [u,z]\) and \(n>\alpha\), the following inequality holds:

\begin{equation}\label{1} (z-\tau)^{n-\lambda_{1}} \leq (z-u)^{n-\lambda_{1}}. \end{equation}
(5)
Since \(f^{(n)}\) is exponential \((s,m)\)-convex therefore for \(\tau \in [u,z]\), we have
\begin{equation}\label{2} f^{(n)}(\tau) \leq \left(\dfrac{z-\tau}{z-u}\right)^{s}e^{-\beta u}f^{(n)}(u)+m\left(\dfrac{\tau-u}{z-u}\right)^{s}e^{-\beta z}f^{(n)}(z). \end{equation}
(6)
Multiplying inequalities (5) and (6), then integrating with respect to \(\tau\) over \([u,z]\), we have \begin{equation*} \int_{u}^{z} (z-\tau)^{n-\lambda_{1}} f^{(n)}(\tau) d\tau \leq \dfrac{(z-u)^{n-\lambda_{1}}}{(z-u)^{s}}\bigg[e^{-\beta u}f^{(n)}(u)\int_{u}^{z} (z-\tau)^{s}d\tau+me^{-\beta z}f^{(n)}(z)\int_{u}^{z} (\tau-u)^{s}d\tau\bigg]. \end{equation*}
\begin{equation}\label{01} \Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}-1}_{u+}f)(z) \leq \dfrac{(z-u)^{n-\lambda_{1}+1}}{s+1} [e^{-\beta u}f^{(n)}(u)+m e^{-\beta z}f^{(n)}(z)]. \end{equation}
(7)
Now we consider function \(f\) on the interval \([z,v], z\in [u,v]\). For \(\tau\in [z,v]\), the following inequality holds:
\begin{equation}\label{3} (\tau-z)^{n-\lambda_{2}} \leq (v-z)^{n-\lambda_{2}}. \end{equation}
(8)
Since \(f^{(n)}\) is exponential \((s,m)\)-convex on \([u,v]\), therefore for \(\tau \in [z,v]\), we have
\begin{equation}\label{4} f^{(n)}(\tau) \leq \left(\dfrac{\tau-z}{v-z}\right)^{s}e^{-\beta v}f^{(n)}(v)+m\left(\dfrac{v-\tau}{v-z}\right)^{s}e^{-\beta z}f^{(n)}(z). \end{equation}
(9)
Multiplying inequalities (8) and (9), then integrating with respect to \(\tau\) over \([z,v]\), we have \begin{equation*} \int_{z}^{v} (\tau-z)^{n-\lambda_{2}} f^{(n)}(\tau) d\tau \leq \dfrac{(v-z)^{n-\lambda_{2}}}{(v-z)^{s}}\bigg[e^{-\beta v}f^{(n)}(v)\int_{z}^{v} (\tau-z)^{s}d\tau+me^{-\beta z}f^{(n)}(z)\int_{z}^{v} (v-\tau)^{s}d\tau\bigg] \end{equation*}
\begin{equation}\label{02} \Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}-1}_{v-}f)(z) \leq \dfrac{(v-z)^{n-\lambda_{2}+1}}{s+1} [e^{-\beta v}f^{(n)}(v)+me^{-\beta z} f^{(n)}(z)]. \end{equation}
(10)
Adding (7) and (10) we get the required inequality in (4).

Corollary 1. By setting \(\lambda_{1}=\lambda_{2}\) in (4) we get the following fractional integral inequality:

\begin{align} &\Gamma(n-\lambda_{1}+1)\left(({^C}D^{\lambda_{1}-1}_{u+}f)(z)+({^C}D^{\lambda_{1}-1}_{v-}f)(z) \right)\notag\\&\leq \dfrac{(z-u)^{n-\lambda_{1}+1}e^{-\beta u}f^{(n)}(u)+(v-z)^{n-\lambda_{1}+1}e^{-\beta v}f^{(n)}(v)}{s+1}+me^{-\beta z}f^{(n)}(z)\bigg[\dfrac{(z-u)^{n-\lambda_{1}+1}+(v-z)^{n-\lambda_{1}+1}}{s+1}\bigg]. \end{align}
(11)

Remark 1. By setting \(s=1\) the inequality will be of the form:

\begin{align} &\Gamma(n-\lambda_{1}+1)\left(({^C}D^{\lambda_{1}-1}_{u+}f)(z)+({^C}D^{\lambda_{1}-1}_{v-}f)(z) \right)\notag\\&\leq \dfrac{(z-u)^{n-\lambda_{1}+1}e^{-\beta u}f^{(n)}(u)+(v-z)^{n-\lambda_{1}+1}e^{-\beta v}f^{(n)}(v)}{2}+me^{-\beta z}f^{(n)}(z)\bigg[\dfrac{(z-u)^{n-\lambda_{1}+1}+(v-z)^{n-\lambda_{1}+1}}{2}\bigg]. \end{align}
(12)

Remark 2. By setting \(\lambda_{1}=\lambda_{2}\), \(\beta=0\), \(s=1\) and \(m=1\), we will get Corollary 2.1 of [14].

Now, we give the next result stated in the following theorem.

Theorem 2. Let \(f:I\longrightarrow \mathbb{R}\) be a real valued \(n\)-time differentiable function where \(n\) is a positive integer. If \(|f^{(n+1)}|\) is exponential (s,m)-convex function, then for \(u,v\in I;u0\), the following inequality for Caputo fractional derivatives holds

\begin{align}\label{0} &\left|\Gamma(n-\lambda_{1} + 1)({^C}D^{\lambda_{1}}_{u+}f)(z) + \Gamma(n-\lambda_{2} + 1)({^C}D^{\lambda_{2}}_{v-}f)(z)\right.\left. -\left((z-u)^{n-\lambda_{1}}f^{(n)}(u) +(v-z)^{n-\lambda_{2}}f^{(n)}(v)\right)\right|\nonumber\\&\leq\frac{(z-u)^{\lambda_{1}+1}e^{-\beta u}|f^{(n+1)}(u)| +(v-z)^{\lambda_{2}+1}e^{-\beta v}|f^{(n+1)}(v)|}{s+1}+m\frac{e^{-\beta z}|f^{(n+1)}(z)|\left((z-u)^{\lambda_{1}+1}+(v-z)^{\lambda_{2}+1}\right)}{s+1}. \end{align}
(13)

Proof. Since \(|f^{(n+1)}|\) is exponential \((s,m)\)-convex function and \(n\) is a positive integer, therefore for \(\tau \in [u,z]\) and \(n>\alpha\), we have \begin{equation*} |f^{(n+1)}(\tau)|\leq\left(\dfrac{z-\tau}{z-u}\right)^{s}e^{-\beta u}|f^{(n+1)}(u)|+m\left(\dfrac{\tau-u}{z-u}\right)^{s}e^{-\beta z}|f^{(n+1)}(z)| \end{equation*} from which we can write

\begin{align}\label{a} &-\left(\left(\frac{z-\tau}{z-u}\right)^{s}e^{-\beta u}|f^{(n+1)}(u)|+m\left(\frac{\tau-u}{z-u}\right)^{s}e^{-\beta z}|f^{(n+1)}(z)|\right)\leq f^{(n+1)}(\tau) \nonumber\\&\leq \left(\frac{z-\tau}{z-u}\right)^{s}e^{-\beta u}|f^{(n+1)}(u)|+m\left(\frac{\tau-u}{z-u}\right)^{s}e^{-\beta z}|f^{(n+1)}(z)|. \end{align}
(14)
We consider the second inequality of inequality (14)
\begin{equation}\label{s} f^{(n+1)}(\tau) \leq \left(\frac{z-\tau}{z-u}\right)^{s}e^{-\beta u}|f^{(n+1)}(u)|+m\left(\frac{\tau-u}{z-u}\right)^{s}e^{-\beta z}|f^{(n+1)}(z)|. \end{equation}
(15)
Now for \(\lambda_{1}>0\), we have
\begin{equation}\label{m} (z-\tau)^{n-\lambda_{1}} \leq (z-u)^{n-\lambda_{1}}, \tau\in[u,z]. \end{equation}
(16)
The product of last two inequalities give \begin{equation*} (z-\tau)^{n-\lambda_{1}}f^{(n+1)}(\tau)\leq (z-u)^{n-\lambda_{1}-s}\left((z-\tau)^{s}e^{-\beta u}|f^{(n+1)}(u)|+m(\tau-u)^{s}e^{-\beta z}|f^{(n+1)}(z)|\right). \end{equation*} Integrating with respect to \(\tau\) over \([u,z]\), we have
\begin{align}\label{b} &\int_{u}^{z}(z-\tau)^{n-\lambda_{1}}f^{(n+1)}(\tau)d\tau\notag\\&\leq(z-u)^{n-\lambda_{1}-s}\left[e^{-\beta u}|f^{(n+1)}(u)|\int_{u}^{z}(z-t\tau)^{s}d\tau+me^{-\beta z}|f^{(n+1)}(z)|\int_{u}^{z}(\tau-u)^{s}d\tau\right]\nonumber\\&=(z-u)^{n-\lambda_{1}+1}\left[\frac{e^{-\beta u}|f^{(n+1)}(u)|+me^{-\beta z}|f^{(n+1)}(z)|}{s+1}\right], \end{align}
(17)
and \begin{align*} \int_{u}^{z}(z-\tau)^{n-\lambda_{1}}f^{(n+1)}(\tau)d\tau&=f^{(n)}(\tau)(z-\tau)^{n-\lambda_{1}}|^{z}_{u}+(n-\lambda_{1}) \int_{u}^{z}(z-\tau)^{n-\lambda_{1}-1}f^{(n)}(\tau)d\tau\\&=-f^{(n)}(u)(z-u)^{n-\lambda_{1}}+\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}}_{u+}f)(z). \end{align*} Therefore (17) takes the form:
\begin{align}\label{x} &\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}}_{u+}f)(z)-f^{(n)}(u)(z-u)^{n-\lambda_{1}}\leq(z-u)^{n-\lambda_{1}+1}\left[\frac{e^{-\beta u}|f^{(n+1)}(u)|+me^{-\beta z}|f^{(n+1)}(z)|}{s+1}\right]. \end{align}
(18)
If one consider from (14) the first inequality and proceed as we did for the second inequality, then following inequality can be obtained:
\begin{align}\label{c} &f^{(n)}(u)(z-u)^{n-\lambda_{1}}-\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}}_{u+}f)(z)\leq(z-u)^{n-\lambda_{1}+1}\left[\frac{e^{-\beta u}|f^{(n+1)}(u)|+me^{-\beta z}|f^{(n+1)}(z)|}{s+1}\right]. \end{align}
(19)
From (18) and (19), we get
\begin{align}\label{0001} &\left|\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}}_{u+}f)(z)-f^{(n)}(u)(z-u)^{n-\lambda_{1}}\right|&\leq(z-u)^{n-\lambda_{1}+1}\left[\frac{e^{-\beta u}|f^{(n+1)}(u)|+me^{-\beta z}|f^{(n+1)}(z)|}{s+1}\right]. \end{align}
(20)
On the other hand, for \(\tau\in[z,v]\), using convexity of \(|f^{(n+1)}|\) as a exponential \((s,m)\)-convex function, we have
\begin{equation}\label{001} |f^{(n+1)}(\tau)|\leq\left(\dfrac{\tau-z}{v-z}\right)^{s}e^{-\beta v}|f^{(n+1)}(v)|+m\left(\dfrac{v-\tau}{v-z}\right)^{s}e^{-\beta z}|f^{(n+1)}(z)|. \end{equation}
(21)
Also for \(\tau\in[z,v]\) and \(\beta>0\), we have
\begin{equation}\label{002} (\tau-z)^{n-\lambda_{2}}\leq(v-z)^{n-\lambda_{2}}. \end{equation}
(22)
By adopting the same treatment as we have done for (14) and (16) one can obtain from (21) and (22) the following inequality:
\begin{align}\label{0002} &\left|\Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}}_{v-}f)(z)-f^{(n)}(v)(v-z)^{n-\lambda_{2}}\right|\leq(v-z)^{n-\lambda_{2}+1}\left[\frac{e^{-\beta v}|f^{(n+1)}(v)|+me^{-\beta z}|f^{(n+1)}(z)|}{s+1}\right]. \end{align}
(23)
By combining the inequalities (20) and (23) via triangular inequality we get the required inequality.

It is interesting to see the following inequalities as a special case.

Corollary 2. By setting \(\lambda_{1}=\lambda_{2}\) in (13), we get the following fractional integral inequality: \begin{align*} &\left|\Gamma(n-\lambda_{1}+1)[({^C}D^{\lambda_{1}}_{u+}f)(z)+({^C}D^{\lambda_{1}}_{v-}f)(z)]-\left((z-u)^{n-\lambda_{1}}f^{(n)}(u)+(v-z)^{n-\lambda_{1}}f^{(n)}(v)\right)\right|\\&\leq\frac{(z-u)^{n-\lambda_{1}+1}e^{-\beta u}|f^{(n+1)}(u)|+(v-z)^{n-\lambda_{1}+1}e^{-\beta v}|f^{(n+1)}(v)|}{s+1}\\&+m\frac{e^{-\beta z}|f^{(n+1)}(z)|\left[(z-u)^{n-\lambda_{1}+1}+(v-z)^{n-\lambda_{1}+1}\right]}{s+1}. \end{align*}

Remark 3. By setting \(s=1\) the inequality will be of the form, \begin{align*} &\left|\Gamma(n-\lambda_{1}+1)[({^C}D^{\lambda_{1}}_{u+}f)(z)+({^C}D^{\lambda_{1}}_{v-}f)(z)]-\left((z-u)^{n-\lambda_{1}}f^{(n)}(u)+(v-z)^{n-\lambda_{1}}f^{(n)}(v)\right)\right|\\&\leq\frac{(z-u)^{n-\lambda_{1}+1}e^{-\beta u}|f^{(n+1)}(u)|+(v-z)^{n-\lambda_{1}+1}e^{-\beta v}|f^{(n+1)}(v)|}{2}\\&+m\frac{e^{-\beta z}|f^{(n+1)}(z)|\left[(z-u)^{n-\lambda_{1}+1}+(v-z)^{n-\lambda_{1}+1}\right]}{2}. \end{align*}

Remark 4. By setting \(\lambda_{1}=\lambda_{2}\), \(\beta=0\), \(s=1\) and \(m=1\), we will get Corollary 2.2 of [14].

Before going to the next theorem we observe the following result.

Lemma 1. Let \(f: [u,v] \longrightarrow \mathbb{R}\), be a exponential (s,m)-convex function. If \(f\) is exponentially symmetric about \(\frac{u+v}{2}\), then the following inequality holds

\begin{equation}\label{0110} f\left(\frac{u+v}{2}\right)\leq\frac{1}{2^{s}}\left(e^{-\beta z}f(z)\right)(1+m) \,\,\,\,\,\,\,z\in[u,v]. \end{equation}
(24)

Proof. Since \(f\) is exponential (s,m)-convex we have

\begin{align} &f\left(\frac{u+v}{2}\right)\leq\frac{1}{2^{s}}\left[e^{-\beta (u\tau+(1-\tau)v)}f(u\tau+(1-\tau)v)+me^{-\beta (u(1-\tau)+v\tau)}f(u(1-\tau)+v\tau)\right]. \end{align}
(25)
Since \(f\) is symmetric about \(\frac{a+b}{2}\), therefore we get \(f(u+v-z)=f(v\tau+(1-\tau)u)\).
\begin{align} &f\left(\frac{u+v}{2}\right)\leq\frac{1}{2^{s}}\left[e^{-\beta (u\tau+(1-\tau)v)}f(u\tau+(1-\tau)v)+me^{-\beta (u+v-z)}f(u+v-z)\right]. \end{align}
(26)
By substituting \(z=(u\tau+(1-\tau)v)\) where \(z\in[u,v]\), we get \begin{align} &f\left(\frac{u+v}{2}\right)\leq\frac{1}{2^{s}}\left(e^{-\beta z}f(z)+me^{-\beta (u+v-z)}f(u+v-z)\right).\nonumber \end{align} Also \(f\) is exponentially symmetric about \(\frac{u+v}{2}\), therefore we have \(f(u+v-z)=f(z)\) and inequality in (24) holds.

Theorem 2. Let \(f:I\longrightarrow \mathbb{R}\) be a real valued \(n\)-time differentiable function where \(n\) is a positive integer. If \(f^{(n)}\) is a positive exponential (s,m)- convex and symmetric about \(\frac{u+v}{2}\), then for \(u,v\in I;u< v\) and \(\lambda_{1},\lambda_{2}\geq1\), the following inequality for Caputo fractional derivatives holds

\begin{align}\label{0011} &\notag\frac{ h(\beta)2^{s}}{2(1+m)}\left(\frac{1}{n-\lambda_{1}+1}+\frac{1}{n-\lambda_{2}+1}\right)f^{(n)}\left(\frac{u+v}{2}\right)\\&\leq\frac{\Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}-1}_{v-}f)(u)}{2(v-u)^{n-\lambda_{2}+1}}+\frac{\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}-1}_{u+}f)(v)}{2(v-u)^{n-\lambda_{1}+1}}\nonumber\\&\leq \frac {mf^{(n)}(u)+f^{(n)}(v)}{(s+1)}. \end{align}
(27)
where \(h(\beta)=e^{\beta v}\) for \( \beta< 0\) and \(h(\beta)=e^{\beta u}\) for \( \beta\geq0\).

Proof. For \(z\in[u,v]\), we have

\begin{equation}\label{M} (z-a)^{n-\lambda_{2}}\leq(v-u)^{n-\lambda_{2}}. \end{equation}
(28)
Also \(f\) is exponential \((s,m)\)-convex function, we have
\begin{equation}\label{S} f^{(n)}(z)\leq\left(\frac{z-u}{v-u}\right)^{s}e^{-\beta v}f^{(n)}(v)+\left(\frac{b-x}{v-u}\right)^{s}e^{-\beta u}mf^{(n)}(u). \end{equation}
(29)
Multiplying (28) and (29) and then integrating with respect to \(z\) over \([u,v]\), we have \begin{equation*} \int_{u}^{v}(z-u)^{n-\lambda_{2}}f^{(n)}(z)dz\leq\frac{(v-u)^{n-\lambda_{2}}}{(v-u)^{s}}\left(\int_{u}^{v}e^{-\beta v}(f^{(n)}(v)(z-u)^{s}+e^{-\beta u}mf^{(n)}(u)(v-z)^{s})dz\right). \end{equation*} From which we have
\begin{equation}\label{A} \frac{\Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}-1}_{v-}f)(u)}{(v-u)^{n-\lambda_{2}+1}}\leq\frac{e^{-\beta v}f^{(n)}(v)+e^{-\beta u}mf^{(n)}(u)}{s+1}. \end{equation}
(30)
On the other hand for \(z\in[u,v]\) we have
\begin{equation}\label{B} (v-z)^{n-\lambda_{1}}\leq(v-u)^{n-\lambda_{1}}. \end{equation}
(31)
Multiplying (29) and (31) and then integrating with respect to \(z\) over \([u,v]\), we get \begin{equation*} \int_{u}^{v}(v-z)^{n-\lambda_{1}}f^{(n)}(z)dz\leq(v-u)^{n-\lambda_{1}+1}\frac {e^{-\beta u}mf^{(n)}(u)+e^{-\beta v}f^{(n)}(v)}{s+1}. \end{equation*} From which we have
\begin{equation}\label{C} \frac{\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}-1}_{u+}f)(v)}{(v-u)^{n-\lambda_{1}+1}}\leq \frac {e^{-\beta u}mf^{(n)}(u)+e^{-\beta v}f^{(n)}(v)}{s+1}. \end{equation}
(32)
Adding (30) and (32) we get the second inequality. \begin{equation} \frac{\Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}-1}_{v-}f)(u)}{2(v-u)^{n-\lambda_{2}+1}}+\frac{\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}-1}_{u+}f)(v)}{2(v-u)^{n-\lambda_{1}+1}}\leq\frac {e^{-\beta u}mf^{(n)}(u)+e^{-\beta v}f^{(n)}(v)}{s+1}\nonumber. \end{equation} Since \(f^{(n)}\) is exponential s-convex and symmetric about \(\frac{u+v}{2}\) using Lemma \ref{lemm}, we have
\begin{equation}\label{aqs} f^{(n)}\left(\frac{u+v}{2}\right)\leq \frac{1}{2^{s}}\left(e^{-\beta z}f^{n}(z)(1+m)\right),\,\,\,\,\,\,\,z\in[u,v]. \end{equation}
(33)
Multiplying with \((z-u)^{n-\lambda_{2}}\) on both sides and then integrating over \([u,v]\), we have
\begin{equation} f^{(n)}\left(\frac{u+v}{2}\right)\int_{u}^{v}(z-u)^{n-\lambda_{2}}dz\leq\frac{(1+m)}{h(\beta)2^{s}}\int_{u}^{v}(z-u)^{n-\lambda_{2}}f^{(n)}(z)dz. \end{equation}
(34)
By definition of Caputo fractional derivatives for exponential \((s,m)\)-convex function, one can have
\begin{equation}\label{F} f^{(n)}\left(\frac{u+v}{2}\right)\frac{1}{2(n-\lambda_{2}+1)}\leq\frac{(1+m)}{h(\beta)2^{s}}\frac{\Gamma(n-\lambda_{2}+1)({^C}D^{\lambda_{2}-1}_{v-}f)(u)}{2(v-u)^{n-\lambda_{2}+1}}. \end{equation}
(35)
Multiplying (33) with \((v-z)^{n-\lambda_{1}}\), then integrating over \([u,v]\), one can get
\begin{equation}\label{G} f^{(n)}\left(\frac{u+v}{2}\right)\frac{1}{2(n-\lambda_{1}+1)}\leq\frac{(1+m)}{h(\beta)2^{s}}\frac{\Gamma(n-\lambda_{1}+1)({^C}D^{\lambda_{1}-1}_{u+}f)(v)}{2(v-u)^{n-\lambda_{1}+1}}. \end{equation}
(36)
Adding (35) and (36), we get the first inequality.

Corollary 3. If we put \(\lambda_{1}=\lambda_{2}\) in (27), then we get $$\frac{h(\beta)2^{s}}{(1+m)}f^{(n)}\left(\frac{u+v}{2}\right)\frac{1}{(n-\lambda_{1}+1)}\leq\frac{\Gamma(n-\lambda_{1}+1)}{(2)(v-u)^{\lambda_{1}+1}}\left[({^C}D^{\lambda_{1}+1}_{v-}f)(u)+({^C}D^{\lambda_{1}+1}_{u+}f)(v)\right] \leq\frac{e^{-\beta u}f^{(n)}(u)+e^{-\beta v}f^{(n)}(v)}{s+1}$$ \noindent where \(h(\beta)=e^{\beta v}\) for \( \beta< 0\) and \(h(\beta)=e^{\beta u}\) for \( \beta\geq0\).

Remark By setting \(\gamma=0\), \(s=1\) and \(s=1\) in Theorem 3 we will get Theorem 2.3 of [14].

Autho Contributions

All authors contributed equally to the writing of this paper. All authors read and approved the final manuscript.

Conflict of Interests

The authors declare no conflict of interest.

References

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New perspectives on internet electricity use in 2030 https://old.pisrt.org/psr-press/journals/easl-vol-3-issue-2-2020/new-perspectives-on-internet-electricity-use-in-2030/ Tue, 30 Jun 2020 20:57:30 +0000 https://old.pisrt.org/?p=4209
EASL-Vol. 3 (2020), Issue 2, pp. 19 - 31 Open Access Full-Text PDF
Anders S.G. Andrae
Abstract: The main problems with several existing Information and Communication Technology (ICT) power footprint investigations are: too limited (geographical and temporal) system boundary, overestimation of power saving potential in the next decade, assume that historical power use can predict future global power use in the next decade despite unprecedented data traffic growth, assume that Moore´s law relation to digital circuitry can continue "forever" and that no problems with extra cooling power will occur for several decades. The highly variable outlooks for the future power consumptions depend on "starting values", disruptions, regional differences and perceptual estimations of electricity intensity reductions and data traffic increase. A hugely optimistic scenario - which takes into account 20% annual improvement of the J/bit in data centers and networks until 2030 is presented. However, the electric power consumption of the present ICT scope will be significant unless great efforts are put into power saving features enabling such improvements of J/bit. Despite evident risks, it seems though that planned power saving measures and innovation will be able to keep the electricity consumption of ICT and the World under some kind of control. The major conclusion is based on several simulations in the present study - that future consumer ICT infrastructure cannot slow its overall electricity use until 2030 and it will use more than today. Data traffic may not be the best proxy metric for estimating computing electricity. Operations and J/operation seem more promising for forecasting and scaling of bottom-up models.
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Engineering and Applied Science Letter

New perspectives on internet electricity use in 2030

Anders S.G. Andrae
Huawei Technologies Sweden AB, Kista, Sweden.; anders.andrae@huawei.com

Abstract

The main problems with several existing Information and Communication Technology (ICT) power footprint investigations are: too limited (geographical and temporal) system boundary, overestimation of power saving potential in the next decade, assume that historical power use can predict future global power use in the next decade despite unprecedented data traffic growth, assume that Moore´s law relation to digital circuitry can continue “forever” and that no problems with extra cooling power will occur for several decades. The highly variable outlooks for the future power consumptions depend on “starting values”, disruptions, regional differences and perceptual estimations of electricity intensity reductions and data traffic increase. A hugely optimistic scenario – which takes into account 20% annual improvement of the J/bit in data centers and networks until 2030 is presented. However, the electric power consumption of the present ICT scope will be significant unless great efforts are put into power saving features enabling such improvements of J/bit. Despite evident risks, it seems though that planned power saving measures and innovation will be able to keep the electricity consumption of ICT and the World under some kind of control. The major conclusion is based on several simulations in the present study – that future consumer ICT infrastructure cannot slow its overall electricity use until 2030 and it will use more than today. Data traffic may not be the best proxy metric for estimating computing electricity. Operations and J/operation seem more promising for forecasting and scaling of bottom-up models.

Keywords:

Communication, computing, data center, data traffic, devices, electricity use, electricity intensity, 5G, forecast, information, instructions, networks, operations, video streaming.

1. Introduction

In recent years some controversy has emerged concerning the potential electric power use of Information and Communication Technology (ICT) technology going forward in the present decade. The electricity consumption is important as there are more or less sustainable ways of producing electricity. Most schools of thought agree that with the current moderate data traffic the power consumption of ICT has - so far - been kept more or less under control. There are conflicting messages regarding the path to a power consumption under control. Depending on scope, in 2020 ICT stands for up to 7% of the total global electricity use. Researchers have used different ways to measure, different ways to model and have also used different kind of statistics. The rise of ICT electric power use is far from a "phantom" problem. A recent review [1] confirmed that ICT systems - despite a large number of energy saving technologies at hand are at a critical point regarding current and future energy consumption of telecommunication networks, data centers and user-related devices. Most evidence speaks against flattening or reducing ICT power. For example, Weldon estimated that the electricity use of all connected devices - including all consumer devices with network connections - would rise from 200 TWh in 2011 to 1100 TWh in 2019 and 1400 TWh in 2025 [2]. Hintemann argued credibly against too pessimistic (e.g. expected and worst case in [3]) and optimistic scenarios for global data center power by listing indisputable global trends such as cryptocurrency mining, relentless speed of data center construction and cloud to hybrid cloud [4]. Moreover, for 2018 Hintemann estimated as much as 400 TWh for global data center electricity use [4]. Then it has been argued that the efficiency gains will continue unhindered between 2022 and 2030 thanks to Artificial Intelligence (AI) [5]. Nevertheless, on computing level Khokhriakov et al. found that multicore processor computing is not energy proportional as the optimization for performance alone results in increase in dynamic energy consumption by up to 89% and optimization for dynamic energy alone results in performance degradation by up to 49% [6]. Actual electricity measurements from Leibniz Supercomputing Centre in Germany showed that between 2000 and 2018 - despite higher power efficiency - the increase in system density and overall performance lead to increase in electricity consumption [7]. The electricity generated by renewable energy is increasing. In 2015 the share of hydro, wind, solar and biomass power was 25% on average in China [8] which is of importance as the growth of ICT construction will be of huge significance there compared to more developed nations.

Truthfully it is challenging to make accurate predictions of global ICT electric power use as it is problematic to account for unknown unknowns. Most researchers agree that the data traffic - no matter how it is defined - will increase exponentially for several years as it has been doing the last decade. The disagreement concerns how fast and how large the ICT related power use will become in around 2030. Probably there is a parallel to linear or exponential thinking of how fast some entity will increase. Further discussions concern whether the anticipated extra electricity use by ICT really is a concern if the additional power can drive the corresponding share of sustainable electric power in specific grids used by the ICT infrastructure. The cost of electricity has to date been rather small for ICT Service providers compared to other expenditures [9], but this could change if the electricity prices and electricity use increase. There is not much expectation that future consumer ICT infrastructure can actually slow its overall electricity use until 2030. With the current knowledge, there are more circumstances pointing towards rising - 1-2 PWh - power consumption of ICT than slowing or flattening.

2030 is rather far away and unprecedented changes in economic activity is hard to predict as the first quarters of 2020 has showed. Here it is assumed that the trend of more ICT and data will not be affected dramatically until 2030 as a result of the slow-down Q1-2 2020. Therefore trends are more important than "exact" use patterns and numbers, as we do not exactly know how and which devices will be used in the future. Blockchain, artificial intelligence (AI), virtual reality (VR), and augmented reality (AR) might be the biggest trends for ICT power use. Anyway, a proper power analysis of the ICT Sector should include production of hardware including embedded chips, use of data centers, use of networks, and use of consumer communication devices.

Production is today around 20% of ICTs footprint but there is room for improving the precision. The digital revolution may possibly in itself help optimize the power use of production. However the total emission of ICT production - and thereby the power use - may well be heavily underestimated [10]. Use stage power of data centers is now around 15%, but is expected to become one of the most important drivers for ICT electricity use. Use stage power of Networks (wireless and core) is now at around 15% of ICT, but its share is expected to increase. There is however considerable uncertainty about 5G's power use depending on point of introduction, learning curve and regional differences.

Use stage power of consumer devices (including Wi-Fi modems) is now at some 50% of ICT total power use but is ideally expected to decrease thanks to advanced power saving features. Current downward trend is expected to continue if no "dramatic processing power saving problems related to Moores law" happen around 2022. The speed of electricity intensity reduction vs. the speed of data traffic increase is the determinant of ICT power. As hypothesized in Section 5, other more fundamental determinants are possible.

1.1. Objectives

The objective of this prediction study is to estimate the global electric power use in 2030 associated with computing and communication - the Information and Communication Technology (ICT) infrastructure - consisting of the use stage of end-user consumer devices, network infrastructure and data centers as well as the production of hardware for all. The specific purpose is to update previous predictions [3] and understand if the power consumption is still likely to develop as previously understood.

1.2. Hypothesis

The hypothesis is that the electric power consumption of the ICT Sector will increase along something in between the best and expected scenario as outlined by Andrae and Edler in 2015 [3] when adding new assumptions of data traffic and electricity intensity improvements.

2. Materials and methods

The approach follows the one outlined in [3] however with several new assumptions for parameters such as electricity intensity improvements and data traffic growth. The expected case scenario in [3] constitute the baseline for the present research, however, the best case scenario is also shown occasionally for entities of the ICT Sector. The baseline year is 2020 and only one trend curve - for ICT total - will be proposed toward 2030. All assumptions made are available in the Supplementary Information.

2.1. Alternate assumptions for data centers use stage

Compared to the expected case scenario in [3] the following assumptions have been made
  • The annual electricity intensity improvement taking place from - 2010 to 2022 - has been increased to 20% instead of 10%. This implies a lower starting point in 2020 than in [3].
  • A much higher amount of data will be processed in the data centers (see Table 1).
Table 1. Differences between [3] expected case and the present prediction for data centers.
Global Data Center IP Traffic   (ZettaBytes/year) Electricity use (TWh)
\textbackslash{}cite\{10\} Present \textbackslash{}cite{10} present
2020 13 19 660 299
2021 16 25 731 311
2022 20 33 854 328
2023 25 43 998 320
2024 30 56 1166 377
2025 37 72 1362 412
2026 46 94 1592 471
2027 56 122 1860 551
2028 69 159 2173 652
2029 85 206 2539 788
2030 105 268 2967
Data traffic is a crude proxy for power use but the numbers are reported frequently [10]. Operations/s [11] may be a better proxy as will be discussed in Section 5.

3. Alternate assumptions for Networks

3.1. Wireless access

Compared to expected case scenario in [3] the following assumptions have been made
  • The factor of historical improvement of the TWh/EB factor between 2010 and 2020 as assumed in [3] has been corrected.
Andrae and Edler [3] arrived at an accumulated improvement factor of 0.083 in 2030 for 5G by assuming 22% improvement between 2010 and 2022 and 5% improvement from 2022 to 2030. However, it is wrong to assume an improvement for 5G from 2010 to 2020 as 5G did not (more or less) exist then. Due to gradually introduced Moore's law problems, the accumulated improvement factor is assumed to be 0.229 in 2030. On top of this, a gradually waning Moore's law is introduced for all mobile technology Gs from 2022 so that the improvement factors run from 19% in 2022 to 5% in 2030, instead of 5% from 2022 to 2030. This leads to more than 4 times more TWh from 5G in the latest understanding mentioned in [12] than in [3]. Tables 2 and 3 show some of the new assumptions.
Table 2. Differences between [3] and the present prediction for 5G mobile networks.
2021 2022 2023 2024 2025 2026 2027 2028 2029 2030
Best Case 5G Traffic EB 41 164 324 677 1248 2656 4316 6685 9928 14403
TWh 0 0 0 1 1 3 4 7 9 13
Expected case 5G Traffic EB 44 189 399 892 1762 3881 6996 11609 18473 28714
TWh 0 1 2 4 7 15 26 41 61 91
Best case 5G Traffic EB 41 164 324 677 1248 2565 4316 6685 9928 14403
TWh 0 5 8 15 23 41 62 87 120 166
Expected case 5G Traffic EB 44 189 399 892 1762 3881 6996 11609 18473 28714
TWh 2 7 12 23 38 74 120 181 268 396
According to [13], in 2020 4G networks deliver 20 kbit/J while [3] predicted (better) 40 kbit/J in 2020. For 5G [13] predicted 10 Mbit/J while [3] predicted (worse) 0.8-2.8 Mbit/J for 2030. The starting point in 2020 for 5G in [3] is 0.05 Mbit/J. As shown in Table 2, the energy efficiency prediction for 5G has decreased - compared to [3] - to 0.18-0.22 Mbit/J [12].
Table 3. Differences between [3] expected case and the present prediction for mobile networks.
Electricity use TWh
\textbackslash{}cite\{10\} Present
2020 98 98
2021 92 94
2022 100 92
2023 114 95
2024 127 102
2025 144 116
2026 145 142
2027 149 181
2028 157 237
2029 172 320
2030 196 446

3.2. Fixed access wired

One of the major weaknesses of the predictions done in [3] is likely the overestimation of fixed wired (core) networks. To improve this, a faster improvement of the TWh/EB is assumed between 2010 and 2022, 20% per year is used instead of 10%. However, a gradually waning Moore's law is introduced from 2022 so that the improvement factors run from 19% in 2022 to 5% in 2030, instead of 5% from 2022 to 2030. Overall however, this results in a dramatically lower electricity use of these networks in 2030 compared to [3] (Table 4).
Table 4. Differences between [3] expected case and the present prediction for fixed access wired networks.
Electricity use (TWh)
\textbackslash{}cite\{10\} Present best case Present expected case
2020 439 134 171
2021 494 129 171
2022 588 126 174
2023 703 125 179
2024 843 126 188
2025 1014 129 200
2026 1222 138 223
2027 1477 152 255
2028 1789 169 296
2029 2171 192 352
2030 2641 224 428

3.3. Alternate assumptions for Devices power use including Wi-Fi modems

From 2020 the improvement of kWh/unit/year for devices is assumed 3% as in [10]. The difference is that Wi-Fi is added to the consumer devices section. Wi-Fi is overestimated in [3] as the Wi-Fi modems electric power use is actually rather independent of handled traffic. The action taken is to increase the electricity intensity improvement from 10% to 20% per year from 2010 to 2022 for the expected case scenario. The resulting electricity use is shown in Table 5. As a sensitivity check, 2 billion homes globally - each with one 3 Watt Wi-Fi modem - would use on average around 52 TWh per year. This shows that the new assumption is more reasonable than previous [3]. Table 5 shows that adding Wi-Fi (moving Wi-Fi from the Networks) to consumer devices, both in [3] and here, suggest increasing and flattening TWh, respectively.
Table 5. Differences between [3] expected case and the present prediction for devices use stage electric power use.
Electricity use (TWh)
\textbackslash{}cite\{10\}Consumer devices Present Consumer devices Wi-Fi modems
+ Wi-Fi modems + Wi-Fi modems
2020 1132 1039 72
2021 1153 1051 75
2022 1171 1054 79
2023 1186 1049 84
2024 1200 1037 91
2025 1217 1017 99
2026 1250 1008 113
2027 1298 1008 133
2028 1365 1017 157
2029 1451 1038 190
2030 1559 1073 234
This prediction is to be considered highly uncertain as the devices will of course also be affected by the power issues related to the slow-down of Moore´s law. This slow-down is included for Wi-Fi devices. Anyway, the order of magnitude for the TWh is most likely correct. Still, a reduction of consumer devices power use seems quite optimistic. It can happen though, thanks to a firm focus on power saving and updated energy labeling requirements for end-user devices.
In the future the use stage electric power of USB dongles, smart home devices, wearables, AR & VR devices, and Wi-Fi modems should be added systematically. Moreover, due to a strong push for longer lifetimes for consumer devices, lifetimes may increase compared to [3].

3.4. Alternate assumptions for Production of ICT hardware

Andrae and Edler [3] overestimated the electric power used to produce ICT goods used in Networks and Data Centers. This is improved in the present prediction by setting the so called life cycle ratio for Networks and Data Center production to 0.02 instead of 0.15. This assumption brings down the production TWh significantly. Assuming that 2 million base stations with ?3 MWh/unit [14] - used in wireless access networks - and 60 million servers with 1 MWh/unit [15] - used in data centers - will be produced in 2030, the electric power needed would be around 66 TWh. The present study predicts 38 TWh in 2030 - of 289 TWh - for all network and data center equipment. This suggests that a 0.02 life cycle ratio for production is reasonable for traffic dependent calculations of data centers and networks. Table 6 shows that the production estimates are much lower in the present study than in [3].
Table 6. Differences between [3] expected case and the present prediction for production of ICT hardware.
Electricity use (TWh)
\textbackslash{}cite\{10\} Present
2020 549 381
2021 540 358
2022 547 339
2023 562 324
2024 584 311
2025 614 302
2026 650 295
2027 696 291
2028 752 290
2029 821 292
2030 903 298
With the current twists and turns in the global economy it is almost undoable to predict parameters for production of ICT. Still, the latest understanding [10]is that production of ICT is underestimated.

4. Results

The stability of Andrae and Edler [3] trend analysis - of how much electric power the ICT Sector might use in 2030 - is remarkable considering the number of changed (improved) assumptions made in the present update and others [10, 11, 12]. In summary in 2030, all entities are predicted to use much less electricity - except wireless access networks - than the expected scenario in [10]. The total TWhrs - for the current studied Internet scope - are very close to best case scenario in [3].

4.1. Data centers power use

Figure 1 shows some trends for data centers 2020 to 2030.

Figure 1. Trends for data centers 2020 to 2030. 

Although the electricity intensity improvements are assumed higher than in [3] the consequences caused by data traffic increase compensate, and the electricity use might still rise. 366 TWh in 2030 - for the best case - are due to a very moderate data traffic growth.

4.2. Networks power use

Figures 2 and 3 show some trends for Networks 2020 to 2030.

Figure 2. Trends for wireless access networks 2020 to 2030.

Figure 3. Trends for fixed access wired networks 2020 to 2030.

4.3. Devices power use

Figure 4 shows some trends for end-user consumer ICT goods use stage 2020 to 2030.

Figure 4. Trends for consumer ICT goods use stage 2020 to 2030.

5. Summary

Figures 5 and 6 show some trends for the synthesis per contributing category in 2020 and 2030, separately. Andrae and Edler [3] is compared to the present update.

Figure 5. Trends for ICT electric power overall 2020.

Figure 6. Trends for ICT electric power overall 2030.

Generally the values for 2020 are lower for most entities. For 2030 too except for wireless access networks which will use more electricity. In total the electric power predictions for the ICT Sector have been reduced by 31% in 2020 and 61% 2030 in the present study compared to expected case scenario in [3]. Potential further reductions are discussed in Section 8.1.

6. Discussion

The ideal framework for ICT electric power footprint would be based on annual shipments of each ICT good, each lifetime and each measured annual and lifetime electric power consumption. However, it may not be practicable to make that journey yet. Connectivity and smart metering is probably the road ahead for collecting power data. Still, the electricity predictions need to be checked against bottom-up and national top-down assessments too. It is crucial to find out how such national assessments are done and to which degree ICT electric power consumption estimates are included. The implications for researchers regarding the path to sustainable computing practices are at least four:
  1. Produce research results which help reduce the electricity use and environmental impact of computing
  2. Sourcing of the power
  3. Power saving strategies
  4. Recycling strategies for the used computers, screens etc
Knowing the high degree of variability, here follows some suggestions for future research approach of this topic. Nissen et al. [16] suggested that process flow modelling would be the best for improving the precision of wireless access networks energy use modeling. As for the future forecasting of ICTs electricity use, Artificial Neural Networks seems a very useful modeling tool [17].

7. Bottom-up considerations for research

The electricity cost of individual computing in particular might be difficult to isolate. Still, there are ways with which we can implement green computing. For example, somehow mimicking the green software coding idea "Proof of stake" - by which the cryptocurrency ethereum plan to slash its power use [18] seems like a good idea. Nevertheless it does not seem useful for individuals to calculate their personal ICT electricity consumption, but some measures probably can be taken. One easy measure is to turn off the video image in communication when voice+video is possible but visual communication is not really required. Still, in Section 4.3 the overall individual and global electricity cost of video streaming is estimated.

8. Testing of the order of magnitude of worldwide ICT and data center electric power use

8.1. What if the 20% per year electricity intensity improvements continue after 2022

Figure 7 shows the summary of the present predictions. At the moment Wi-Fi based - or fixed optic fibre broadband - computing is preferable to wireless 4G based computing from an overall electricity consumption point of view.

Figure 7. Trends for ICT electric power use 2020 to 2030.

The "extreme positive" scenario assumes that no slowdown of electricity intensity improvements happen after 2022 i.e. no gradually waning annual improvements from 2022 to 2030 as in the present baseline (expected case scenario) - and that 20% improvements still happen in Networks and Data Centers until 2030. In that case ICT power will more or less stay flat while the total data traffic grows 14 times between 2020 and 2030. The electricity use of networks and data centers will be 54% less in such an "extreme positive" scenario than in the present study.

8.2. Blockchain and cryptocurrencies

The blockchain is established on databases that are not consolidated in one server, but in a global network of computers. The information is eternally registered, in sequential order, and in all parts of the computer network. The computing power allocated to the specific blockchain application bitcoin is likely very high [19]. The reason is that with bitcoin every new piece of information added to the chain requires that someone uses computer power to solve an advanced cryptographic problem via Proof of Work. The sooner this cryptographic problem gets resolved, the greater the likelihood that the person who is in charge of the mining of bitcoin cryptocurrencies will be paid in bitcoin cryptocurrency. The demand for bitcoins - as long as it lasts - will therefore increase the demand for electric power. Mora et al., [19] pointed out that any further development of cryptocurrencies should critically aim to reduce electricity demand. Reducing the power use of cryptocurrencies might have a solution in the form of Proof of Stake instead of Proof of Work [18].

8.3. Renewable electric power and ICT

There are discussions ongoing about the possibility that ICT infrastructure can be run entirely on renewable power. One of many challenges is that the renewable power should be located in the vicinity of the ICT infrastructure.
Using renewable energy to power data centers and networks can reduce the environmental impacts. However, the uneven geospatial distribution of renewable energy resources and regions with high ICT use might create uncertainty of supply [20, 21]. The relation between renewable energy resources and associated environmental impacts - of data centers and networks driven by renewable energy at a global scale should be investigated thoroughly [10].
Overall the present predictions suggest a trajectory in between the Best and Expected Case Scenarios in [3], \(\approx\)1990 TWh in 2020 and 3200 TWh in 2030 (Figure 6). The ICT Sector has and will have a considerable share of the global electricity footprint.

8.4. Bottom-up calculation of the electricity use associated with video streaming

It is relevant to estimate how much data is generated - and associated electric power used - by normal behavior like video streaming several hours every day. For the present estimations the following key indicators are used (Table 7).
Table 7. 2020 and 2030 key electricity intensity indicators relevant for video streaming.
Entity used in video streaming 2020 2030 units Assumed share of total Global access traffic (internet traffic) 2020 Assumed share of total Global access traffic (internet traffic) 2030
Wireless access network 0.18 (98 TWh/549 ExaByte) 0.0144 (446/30899) kWh/GB 15% 85%
Fixed access wired networks 0.07 (171/2444) 0.017 (428/25901) kWh/GB 85% 15%
Data center 0.015 (299/19919) 0.004 (974/274599) kWh/GB
The electricity intensities are set to decrease massively, especially for wireless access networks. However, those networks are perhaps used much less extensively for video streaming in 2020 than optic fixed access. Table 7 suggests that the electric power use of video streaming is strongly correlated to the way in which the video streaming is obtained. Streaming via a 4G router directly or with Wi-Fi is less efficient at the moment than optical broadband via a mobile phone/tablet using Wi-Fi.
Typically standard definition video use 1 GB per hour and high definition (HD) video use 3 GB per hour. Other video formats with higher resolution (e.g. 8K 3D) might use even higher amounts. It is assumed 20 GB per hour for the most typical video technology used in 2030.
By this information it is possible to predict the current and future data generation and electricity consumption associated with video streaming and relate it to the total for ICT.

8.5. Data amounts and TWh from global video streaming

For 2020 it is assumed that one person watches video streaming in HD 2 hours/day in weekdays and 4 hour/day on weekends, i.e. 18 hours per week and 936 hours per year.
To provide these hours, 2808 GB per person is generated in 2020. If all entities are used in Table 7 to deliver the stream, 285 kWh per year per person is required. Assuming that 2 billion persons have this behavior, 570 TWh is needed for 5230 ExaBytes. This suggests that video streaming is a noticeable driver for ICT electric power use in 2020. For 2030 it is assumed that one person watches video streaming in HD 2 hours/day in weekdays and 4 hour/day on weekends, i.e. 18 hours per week and 936 hours per year.
However, due to higher GB/hour, 18720 GB per person is generated in 2030. If all entities are used in Table 7 to deliver the stream, 352 kWh per year per person is needed. Assuming that 7 billion persons will have this behavior, 2464 TWh is required for 122040 ExaBytes. These simple hypotheses shows that increasing electricity use of the ICT Sector is unquestionably in the cards.

9. Conclusions

It is very difficult to fathom the circumstances under which the electric power use of communication and computing (the ICT infrastructure) cannot rise considerably until 2030. The total TWh will develop along an average of the best and expected scenario in [3] with a strong leaning to the best case.

10. Next steps

New advances in large-scale fiber-optic communication systems [22, 23, 24, 25] should be translated to J/bit and used for predictions of the fixed core network. Advances in heat recovery and lowering temperature of microchips [26] may have big implications for the global ICT power use. The reason is that the energy consumption per transistor is strongly correlated to the temperature at which the transistor is working [11]. The overall effect of solving the Internet of Things, edge devices high computation, memory requirements and power dilemma is not well understood [27]. Moreover, it is plausible that ICT infrastructure can help save electric power in society as a whole, and Ono et al. suggested 1300 TWh in 2030 [28]. These assumptions should be further explored. Also these areas are next steps:
  • Find out best way to define an operation or instruction in computing
  • Forecast the number of different operations and instructions
  • Measure different J/operation or J/instruction.
Andrae [9] put forward these hypotheses for 2015: (i) the "traffic" (instructions/s) was around 1 Zettainstructions/s in total and (ii) the energy efficiency was overall around 7 Gigainstructions/J.
Falsifying in detail the above hypotheses would enable reliable forecasting of the power consumption of computing which involve new technologies. Equation (1) may be the way forward if the data could be collected:
\begin{equation} ICT_{t}=\sum _{j,i} 8760 \times \left(\frac{(\frac{Ins}{s})_{j,i,t}}{(\frac{Ins}{j})_{j,i,t}}\right) \end{equation}
(1)
where, \(ICT_{t}=\) ICT sector total global average electricity use in Wh related to processing and computing. \(j=\)computing type; special purpose, general purpose, machine learning, dark calculations etc. \(i=\)ICT good type. \(t=\) year. \(Ins=\)computing instructions. Has data traffic reached the end of the line as proxy for ICT power forecasting? Machine learning training done in a data center may send only a few bits of data to the data center, presumably creating a relatively small amount of IP traffic. That is, on one hand the training process may imply many calculations without necessarily generating a lot of IP traffic. On the other hand the training may use more energy due to the required operations and J/operation [12]. Deep learning may use enormous amounts of electricity [29], however unclear how many Joules per instruction. Then research [30] showed that this electricity use may be reduced 1000 times. These frameworks and speculations need more analysis and put into a global perspective and Equation 1. Another angle to be analyzed further is that as web page sizes increase, the metrics Page Load Time and Page Render Time have larger impact on energy usage on the client side [31].

Autho Contributions

All authors contributed equally to the writing of this paper. All authors read and approved the final manuscript.

Conflict of Interests

The authors declare no conflict of interest.

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New fractional Hadamard and Fejér-Hadamard inequalities associated with exponentially \((h,m)\)-convex functions https://old.pisrt.org/psr-press/journals/easl-vol-3-issue-2-2020/new-fractional-hadamard-and-fejer-hadamard-inequalities-associated-with-exponentially-hm-convex-functions/ Thu, 09 Apr 2020 13:53:11 +0000 https://old.pisrt.org/?p=4005
EASL-Vol. 3 (2020), Issue 2, pp. 9 - 18 Open Access Full-Text PDF
Sajid Mehmood, Ghulam Farid,, Khuram Ali Khan, Muhammad Yussouf
Abstract: The aim of this paper is to establish some new fractional Hadamard and Fejér-Hadamard inequalities for exponentially \((h,m)\)-convex functions. These inequalities are produced by using the generalized fractional integral operators containing Mittag-Leffler function via a monotonically increasing function. The presented results hold for various kinds of convexities and well known fractional integral operators.
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Engineering and Applied Science Letter

New fractional Hadamard and Fejér-Hadamard inequalities associated with exponentially \((h,m)\)-convex functions

Sajid Mehmood, Ghulam Farid\(^1\), Khuram Ali Khan, Muhammad Yussouf
Department of Mathematics, COMSATS University Islamabad, Attock Campus, Pakistan.; (S.M & G.F)
Department of Mathematics, University of Sargodha, Sargodha, Pakistan.; (K.A.K & M.Y)

\(^{1}\)Corresponding Author: ghlmfarid@cuiatk.edu.pk

Abstract

The aim of this paper is to establish some new fractional Hadamard and Fejér-Hadamard inequalities for exponentially \((h,m)\)-convex functions. These inequalities are produced by using the generalized fractional integral operators containing Mittag-Leffler function via a monotonically increasing function. The presented results hold for various kinds of convexities and well known fractional integral operators.

Keywords:

Convex functions, exponentially \((h,m)\)-convex functions, Hadamard inequality, Fejér-Hadamard inequality, generalized fractional integral operators, Mittag-Leffler function.

1. Introduction

Convex functions are very important in the field of mathematical inequalities. Nobody can deny the importance of convex functions. A large number of mathematical inequalities exist in literature due to convex functions. For more information related to convex functions and it's properties (see, [1, 2, 3]).

Definition 1. A function \(\mu:I\rightarrow \mathbb{R}\) on an interval of real line is said to be convex, if for all \(\alpha,\beta\in I\) and \(\kappa\in[0,1]\), the following inequality holds:

\begin{equation}\label{34} \mu(\kappa \alpha+(1-\kappa)\beta)\leq \kappa\mu(\alpha)+(1-\kappa)\mu(\beta). \end{equation}
(1)
The function \(\mu\) is said to be concave if \(-\mu\) is convex.

A convex function is interpreted very nicely in the coordinate plane by the well known Hadamard inequality stated as follows:

Theorem 2. Let \(\mu:[\alpha,\beta]\rightarrow \mathbb{R}\) be a convex function such that \(\alpha< \beta\). The following inequalities holds: \begin{equation*} \mu\left(\frac{\alpha+\beta}{2}\right)\leq \frac{1}{\beta-\alpha}\int^{\beta}_{\alpha}\mu(\kappa)d\kappa\leq \frac{\mu(\alpha)+\mu(\beta)}{2}. \end{equation*}

In [4], Fejér gave the generalization of Hadamard inequality known as the Fejér-Hadamard inequality stated as follows:

Theorem 3. Let \(\mu:[\alpha,\beta]\rightarrow \mathbb{R}\) be a convex function such that \(\alpha< \beta\). Also let \(\nu:[\alpha,\beta]\rightarrow \mathbb{R}\) be a positive, integrable and symmetric to \(\frac{\alpha+\beta}{2}\). The following inequalities hold:

\begin{equation}\label{r} \mu\left(\frac{\alpha+\beta}{2}\right)\int_{\alpha}^{\beta}\nu(\kappa)d\kappa\leq \int_{\alpha}^{\beta}\mu(\kappa)\nu(\kappa)d\kappa\leq \frac{\mu(\alpha)+\mu(\beta)}{2}\int_{\alpha}^{\beta}\nu(\kappa)d\kappa. \end{equation}
(2)
The Hadamard and the Fejér-Hadamard inequalities are further generalized in various ways by using different fractional integral operators such as Riemann-Liouville, Katugampola, conformable and generalized fractional integral operators containing Mittag-Leffler function etc. For more results and details (see, [5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21]). Next we give the definition of exponentially convex functions.

Definition 4.[9, 22] A function \(\mu: I\rightarrow\mathbb{R}\) on an interval of real line is said to be exponentially convex, if for all \(\alpha,\beta \in I\) and \(\kappa\in[0,1]\), the following inequality holds:

\begin{equation}\label{11} e^{ \mu(\kappa \alpha+(1-\kappa)\beta)}\leq \kappa e^{\mu(\alpha)}+(1-\kappa)e^{\mu(\beta)}. \end{equation}
(3)
In [23], Rashid et al., gave the definition of exponentially \(s\)-convex functions.

Definition 5. Let \(s\in[0,1]\). A function \(\mu: I\rightarrow\mathbb{R}\) on an interval of real line is said to be exponentially \(s\)-convex, if for all \(\alpha,\beta \in I\) and \(\kappa\in[0,1]\), the following inequality holds:

\begin{equation}\label{12} e^{ \mu(\kappa \alpha+(1-\kappa)\beta)}\leq \kappa^s e^{\mu(\alpha)}+(1-\kappa)^se^{\mu(\beta)}. \end{equation}
(4)
In [24], Rashid et al., gave the definition of exponentially \(h\)-convex functions.

Definition 6. Let \(J\subseteq\mathbb{R}\) be an interval containing \((0,1)\) and let \(h: J\rightarrow\mathbb{R}\) be a non-negative function. Then a function \(\mu: I\rightarrow\mathbb{R}\) on an interval of real line is said to be exponentially \(h\)-convex, if for all \(\alpha,\beta \in I\) and \(\kappa\in[0,1]\), the following inequality holds:

\begin{equation}\label{13} e^{ \mu(\kappa \alpha+(1-\kappa)\beta)}\leq h(\kappa) e^{\mu(\alpha)}+h(1-\kappa)e^{\mu(\beta)}. \end{equation}
(5)
In [25], Rashid et al., gave the definition of exponentially \(m\)-convex functions.

Definition 7. A function \(\mu: I\rightarrow\mathbb{R}\) on an interval of real line is said to be exponentially \(m\)-convex, if for all \(\alpha,\beta \in I\), \(m\in(0,1]\) and \(\kappa\in[0,1]\), the following inequality holds:

\begin{equation}\label{14} e^{ \mu(\kappa \alpha+m(1-\kappa)\beta)}\leq \kappa e^{\mu(\alpha)}+m(1-\kappa)e^{\mu(\beta)}. \end{equation}
(6)
In [26], Rashid et al., gave the definition of exponentially \((h,m)\)-convex functions.

Definition 8. Let \(J\subseteq\mathbb{R}\) be an interval containing \((0,1)\) and let \(h: J\rightarrow\mathbb{R}\) be a non-negative function. Then a function \(\mu: I\rightarrow\mathbb{R}\) on an interval of real line is said to be exponentially \((h,m)\)-convex, if for all \(\alpha,\beta \in I\), \(m\in(0,1]\) and \(\kappa\in[0,1]\), the following inequality holds:

\begin{equation}\label{15} e^{ \mu(\kappa \alpha+m(1-\kappa)\beta)}\leq h(\kappa) e^{\mu(\alpha)}+mh(1-\kappa)e^{\mu(\beta)}. \end{equation}
(7)

Remark 1.

  1. If we set \(h(\kappa)=\kappa\) and \(m=1\) in (7), then exponentially convex function (3) is obtained.
  2. If we set \(h(\kappa)=\kappa^s\) and \(m=1\) in (7), then exponentially \(s\)-convex function (4) is obtained.
  3. If we set \(m=1\) in (7), then exponentially \(h\)-convex function (5) is obtained.
  4. If we set \(h(\kappa)=\kappa\) in (7), then exponentially \(m\)-convex function (6) is obtained.

Fractional integral operators also play important role in the subject of mathematical analysis. Recently in [27], Andrić et al., defined the generalized fractional integral operators containing generalized Mittag-Leffler function in their kernels as follows:

Definition 9. Let \(\psi,\sigma,\phi,l,\varsigma,c\in \mathbb{C}\), \(\Re(\sigma),\Re(\phi),\Re(l)>0\), \(\Re(c)>\Re(\varsigma)>0\) with \(p\geq0\), \(r>0\) and \(0< q\leq r+\Re(\sigma)\). Let \(\mu\in L_{1}[\alpha,\beta]\) and \(u\in[\alpha,\beta].\) Then the generalized fractional integral operators \(\Upsilon_{\sigma,\phi,l,\psi,\alpha^{+}}^{\varsigma,r,q,c}\mu \) and \(\Upsilon_{\sigma,\phi,l,\psi,\beta^{-}}^{\varsigma,r,q,c}\mu\) are defined by:

\begin{equation}\label{a} \left(\Upsilon_{\sigma,\phi,l,\psi,\alpha^{+}}^{\varsigma,r,q,c}\mu \right)(u;p)=\int_{\alpha}^{u}(u-\kappa)^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi(u-\kappa)^{\sigma};p)\mu(\kappa)d\kappa, \end{equation}
(8)
\begin{equation} \left(\Upsilon_{\sigma,\phi,l,\psi,\beta^{-}}^{\varsigma,r,q,c}\mu \right)(u;p)=\int_{u}^{\beta}(\kappa-u)^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi(\kappa-u)^{\sigma};p)\mu(\kappa)d\kappa, \end{equation}
(9)
where \(E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\kappa;p)\) is the generalized Mittag-Leffler function defined as follows: \begin{equation*} E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\kappa;p)= \sum_{n=0}^{\infty}\frac{\beta_{p}(\varsigma+nq,c-\varsigma)}{\beta(\varsigma,c-\varsigma)} \frac{(c)_{nq}}{\Gamma(\sigma n +\phi)} \frac{\kappa^{n}}{(l)_{n r}}. \end{equation*}

In [28], Farid defined the following unified integral operators:

Definition 10. Let \(\mu, \nu: [\alpha,\beta]\rightarrow \mathbb{R}\), \(0< \alpha< \beta\) be the functions such that \(\mu\) be a positive and integrable and \(\nu\) be a differentiable and strictly increasing. Also, let \(\frac{\gamma}{u}\) be an increasing function on \([\alpha,\infty)\) and \(\psi,\phi,l,\varsigma,c\in \mathbb{C}\), \(\Re(\phi),\Re(l)>0\), \(\Re(c)>\Re(\varsigma)>0\) with \(p\geq0\), \(\sigma,r>0\) and \(0< q\leq r+\sigma\). Then for \(u\in[\alpha,\beta]\) the integral operators \(_{\nu}\Upsilon_{\sigma, \phi,l, \alpha^{+}}^{\gamma, \varsigma,r,q,c}\mu\) and \(_{\nu}\Upsilon_{\sigma, \phi,l, \beta^{-}}^{\gamma, \varsigma,r,q,c}\mu\) are defined by:

\begin{align}\label{sd} \left(_{\nu}\Upsilon_{\sigma, \phi,l, \alpha^{+}}^{\gamma, \varsigma,r,q,c}\mu\right)(u;p)=\int_{\alpha}^{u}\frac{\gamma(\nu(u)-\nu(\kappa))}{\nu(u)-\nu(\kappa)} E_{\sigma, \phi, l}^{\varsigma,r,q,c} (\psi(\nu(u)-\nu(\kappa))^{\sigma};p)\mu(\kappa)d(\nu(\kappa)), \end{align}
(10)
\begin{align}\label{sb} \left(_{\nu}\Upsilon_{\sigma, \phi,l, \beta^{-}}^{\gamma, \varsigma,r,q,c}\mu\right)(u;p)=\int_{u}^{\beta}\frac{\gamma(\nu(\kappa)-\nu(u))}{\nu(\kappa)-\nu(u)} E_{\sigma, \phi, l}^{\varsigma,r,q,c} (\psi(\nu(\kappa)-\nu(u))^{\sigma};p)\mu(\kappa)d(\nu(\kappa)). \end{align}
(11)
If we set \(\gamma(u)=u^\phi\) in (10) and (11), then we get the following generalized fractional integral operators containing Mittag-Leffler function:

Definition 11. Let \(\mu, \nu: [\alpha,\beta]\rightarrow \mathbb{R}\), \(0< \alpha< \beta\) be the functions such that \(\mu\) be a positive and integrable and \(\nu\) be a differentiable and strictly increasing. Also let \(\psi,\phi,l,\varsigma,c\in \mathbb{C}\), \(\Re(\phi),\Re(l)>0\), \(\Re(c)>\Re(\varsigma)>0\) with \(p\geq0\), \(\sigma,r>0\) and \(0< q\leq r+\sigma\). Then for \(u\in[\alpha,\beta]\) the integral operators \(_{\nu}\Upsilon_{\sigma, \phi,l,\psi, \alpha^{+}}^{\varsigma,r,q,c}\mu\) and \(_{\nu}\Upsilon_{\sigma, \phi,l,\psi, \beta^{-}}^{ \varsigma,r,q,c}\mu\) are defined by:

\begin{equation}\label{1} \left(_{\nu}\Upsilon_{\sigma, \phi,l, \psi, \alpha^{+}}^{ \varsigma,r,q,c}\mu\right)(u;p)=\int_{\alpha}^{u}(\nu(u)-\nu(\kappa))^{\phi-1} E_{\sigma, \phi, l}^{\varsigma,r,q,c} (\psi(\nu(u)-\nu(\kappa))^{\sigma};p)\mu(\kappa)d(\nu(\kappa)), \end{equation}
(12)
\begin{equation}\label{7} \left(_{\nu}\Upsilon_{\sigma, \phi,l,\psi, \beta^{-}}^{ \varsigma,r,q,c}\mu\right)(u;p)=\int_{u}^{\beta}(\nu(\kappa)-\nu(u))^{\phi-1} E_{\sigma, \phi, l}^{\varsigma,r,q,c} (\psi(\nu(\kappa)-\nu(u))^{\sigma};p)\mu(\kappa)d(\nu(\kappa)). \end{equation}
(13)

Remark 2. (12) and (13) are the generalization of the following fractional integral operators:

  1. Setting \(\nu(u)=u\), the fractional integral operators (8) and (9), can be obtained.
  2. Setting \(\nu(u)=u\) and \(p=0\), the fractional integral operators defined by Salim-Faraj in [29]TOS}, can be obtained.
  3. Setting \(\nu(u)=u\) and \(l=r=1\), the fractional integral operators defined by Rahman et al., in [30], can be obtained.
  4. Setting \(\nu(u)=u\), \(p=0\) and \(l=r=1\), the fractional integral operators defined by Srivastava-Tomovski in [31], can be obtained.
  5. Setting \(\nu(u)=u\), \(p=0\) and \(l=r=q=1\), the fractional integral operators defined by Prabhakar in [32], can be obtained.
  6. Setting \(\nu(u)=u\) and \(\psi=p=0\), the Riemann-Liouville fractional integral operators can be obtained.

In [33], Mehmood et al., proved the following formulas for constant function:
\begin{equation}\label{1*} \left(_{\nu}\Upsilon_{\sigma, \phi,l, \psi, \alpha^{+}}^{ \varsigma,r,q,c}1\right)(u;p)=(\nu(u)-\nu(\alpha))^{\phi}E_{\sigma, \phi+1, l}^{\varsigma,r,q,c} (\psi(\nu(u)-\nu(\alpha))^{\sigma};p):=_{\nu}\xi_{\psi, \alpha^{+}}^{\phi}(u;p), \end{equation}
(14)
\begin{equation}\label{7*} \left(_{\nu}\Upsilon_{\sigma, \phi,l, \psi, \beta^{-}}^{ \varsigma,r,q,c}1\right)(u;p)=(\nu(\beta)-\nu(u))^{\phi}E_{\sigma, \phi+1, l}^{\varsigma,r,q,c} (\psi(\nu(\beta)-\nu(u))^{\sigma};p):=_{\nu}\xi_{\psi, \beta^{-}}^{ \phi}(u;p). \end{equation}
(15)
The objective of this paper is to establish the Hadamard and the Fejér-Hadamard inequalities for generalized fractional integral operators (12) and (13) containing Mittag-Leffler function via a monotone function by using the exponentially \((h,m)\)-convex functions. These inequalities lead to produce the Hadamard and the Fejér-Hadamard inequalities for various kinds of exponentially convexity and well known fractional integral operators given in Remark 1 and Remark 2. In Section 2, we prove the Hadamard inequalities for generalized fractional integral operators (12) and (13) via exponentially \((h,m)\)-convex functions. In Section 3, we prove the Fejér-Hadamard inequalities for these generalized fractional integral operators via exponentially \((h,m)\)-convex functions. Moreover, some of the results published in [26, 33, 34] have been obtained in particular.

2.Fractional Hadamard inequalities for exponentially \((h,m)\)-convex functions

In this section, we will give two versions of the generalized fractional Hadamard inequality. To establish these inequalities exponentially \((h,m)\)-convexity and generalized fractional integrals operators have been used.

Theorem 12. Let \(\mu,\nu: [\alpha,m\beta]\subset[0,\infty)\to\mathbb{R}\), \(0< \alpha< m\beta\) be two functions such that \(\mu\) be integrable and \(\nu\) be differentiable. If \(\mu\) be exponentially \((h,m)\)-convex, \(\nu\) be strictly increasing and \(h\in[0,1]\). Then for generalized fractional integral operators, the following inequalities hold:

\begin{align}\label{yty} &{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}} _{\nu}\xi^{\phi}_{\bar{\psi},\alpha^{+}}(\nu^{-1}(m\nu(\beta));p)\nonumber\\\nonumber &\leq\! h\!\left(\!\frac{1}{2}\!\right)\!\!\left[\!\left(\!_{\nu}\Upsilon_{\sigma,\phi,l,\bar{\psi},\alpha^{+}}^{\varsigma,r,q,c}e^{\mu\circ\nu}\!\right)\!\!(\!\nu^{-1}(\!m\nu(\beta));p)\!+\!\nonumber m^{\phi+1}\!\!\left(\!_{\nu}\Upsilon_{\sigma,\phi,l,\bar{\psi}m^\sigma,\beta^{-}}^{\varsigma,r,q,c}e^{\mu\circ\nu}\!\!\right)\!\!\left(\!\!\nu^{-1}\!\left(\!\frac{\nu(\alpha)}{m}\!\right)\!;p\!\right)\!\right]\\\nonumber &\leq h\left(\frac{1}{2}\right){(m\nu(\beta)-\nu(\alpha))}^\phi\left[\left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right) \left(\Upsilon_{\sigma,\phi,l,{\psi},1^{-}}^{\varsigma,r,q,c}h\right)(0;p)\right.\nonumber\\ &\;\;\;\left.+m\left(e^{\mu(\nu(\beta))}+me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\right)\left(\Upsilon_{\sigma,\phi,l,{\psi},0^{+}}^{\varsigma,r,q,c}h\right)(1;p)\right],\;\;\text{where}\;\; \bar{\psi}=\frac{\psi}{(m\nu(\beta)-\nu(\alpha))^{\sigma}}. \end{align}
(16)

Proof. By the exponentially \((h,m)\)-convexity of \(\mu\), we have

\begin{equation}\label{b} {e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}}\leq h\left(\frac{1}{2}\right) \left[{e^{{\mu(\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta))}}}+m{e^{{\mu((1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}}}\right]. \end{equation}
(17)
Multiplying (17) with \(\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)\) and integrating over \([0,1]\), we have
\begin{align}\label{ad} &{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}}\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)d\kappa\notag \\&\leq h\left(\frac{1}{2}\right) \left[ \int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p){e^{{\mu(\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta))}}}d\kappa\right.\left.+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p){e^{{\mu((1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}}}d\kappa\right]. \end{align}
(18)
Setting \(\nu(u)=\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta)\) and \(\nu(v)=(1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta)\) in (18), then again from exponentially \((h,m)\)-convexity of \(\mu\), we have
\begin{align}\label{c} &e^{{\mu(\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta))}}+me^{{\mu((1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}}\notag\\ &\leq h(\kappa)\left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right)+mh(1-\kappa)\left(e^{\mu(\nu(\beta))}+me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\right). \end{align}
(19)
Multiplying (19) with \(h\left(\frac{1}{2}\right)\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)\) and integrating over \([0,1]\), we have
\begin{align}\label{ab} &\notag h\left(\frac{1}{2}\right)\bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{{\mu(\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta))}}d\kappa+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{{\mu((1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}}d\kappa\bigg]\\&\leq h\left(\frac{1}{2}\right) \bigg[\left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right)\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h(\kappa)d\kappa+m\left(e^{\mu(\nu(\beta))}+me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\right) \nonumber\\&\;\;\;\times \int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h(1-\kappa)d\kappa\bigg]. \end{align}
(20)
Setting \(\nu(u)=\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta)\) and \(\nu(v)=(1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta)\) in (20), then by using (8), (9), (12)and (13), the second inequality of (16) is obtained.

Corollary 1. Setting \(m=1\) in (16), the following inequalities for exponentially \(h\)-convex function can be obtained:

\begin{align}\label{yty*} & {e^{\mu\left( \frac{\nu(\alpha)+\nu(\beta)}{2}\right)}} _{\nu}\xi^{\phi}_{\bar{\psi},\alpha^{+}}(\beta;p)\leq h\left(\frac{1}{2}\right)\bigg[\left(_{\nu}\Upsilon_{\sigma,\phi,l,\bar{\psi},\alpha^{+}}^{\varsigma,r,q,c}e^{\mu\circ\nu}\right)(\beta;p)+ \left(_{\nu}\Upsilon_{\sigma,\phi,l,\bar{\psi},\beta^{-}}^{\varsigma,r,q,c}e^{\mu\circ\nu}\right)\left(\alpha;p \right)\bigg]\nonumber\\ &\leq h\left(\frac{1}{2}\right){(\nu(\beta)-\nu(\alpha))}^\phi\left(e^{\mu(\nu(\alpha))}+e^{\mu(\nu(\beta))}\right)\left[ \left(\Upsilon_{\sigma,\phi,l,{\psi},1^{-}}^{\varsigma,r,q,c}h\right)(0;p)+\left(\Upsilon_{\sigma,\phi,l,{\psi},0^{+}}^{\varsigma,r,q,c}h\right)(1;p)\right], \end{align}
(21)
where \(\bar{\psi}=\frac{\psi}{(\nu(\beta)-\nu(\alpha))^{\sigma}}. \)

Remark 3.

  1. If we set \(h(\kappa)=\kappa\) in (16), then [33, Theorem 8] is obtained.
  2. If we set \(h(\kappa)=\kappa\) and \(m=1\) in (16), then [33, Corollary 1] is obtained.
  3. If we set \(\nu(u)=u\) and \(h(\kappa)=\kappa\) in (16), then [34, Theorem 2.1] is obtained.
  4. If we set \(\nu(u)=u\), \(h(\kappa)=\kappa\) and \(m=1\) in (16), then [34, Corollary 2.2] is obtained.
  5. If we set \(\nu(u)=u\) in (16), then [26, Theorem 2.1] is obtained.

In the following we give another version of the Hadamard inequality for generalized fractional integral operators via exponentially \((h,m)\)-convex functions.

Theorem 13. Let \(\mu,\nu: [\alpha,m\beta]\subset[0,\infty)\to\mathbb{R}\), \(0< \alpha< m\beta\) be two functions such that \(\mu\) be integrable and \(\nu\) be differentiable. If \(\mu\) be exponentially \((h,m)\)-convex and \(\nu\) be strictly increasing. Then for generalized fractional integral operators, the following inequalities hold:

\begin{align}\label{lmo} &\notag{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}}_{\nu}\xi^{\phi}_{\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+m\nu(\beta)}{2}\right)\right) ^{+}}(\nu^{-1}(m\nu(\beta));p)\\\nonumber &\leq h\!\left(\frac{1}{2}\right)\! \left[\left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+m\nu(\beta)}{2}\right)\right) ^{+}}e^{\mu\circ\nu}\right)(\nu^{-1}(m\nu(\beta));p)\right.\\&\nonumber\;\;\;\left.+m^{\phi+1} \left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}(2m)^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+m\nu(\beta)}{2m}\right)\right) ^{-}}e^{\mu\circ\nu}\right)\left(\nu^{-1}\left(\frac{\nu(\alpha)}{m}\right);p \right)\right] \\&\nonumber\leq\!h\!\left(\!\frac{1}{2}\!\right)\!\! \frac{(m\nu(\beta)-\nu(\alpha))^\phi}{2^{\phi}}\!\!\left[\!\left(\!e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\!\right)\!\!\int_{0}^{1}\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h\left(\frac{\kappa}{2}\right)\!d\kappa\right.\\&\;\;\;\left.+m\!\left(\!e^{\mu(\nu(\beta))}+me^{\mu\left(\frac{\nu(\alpha)}{m^2}\!\right)}\right)\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h\left(\frac{2-\kappa}{2}\right)d\kappa\right], \end{align}
(22)
where \(\bar{\psi}\) is same as in (16).

Proof. By the exponentially \((h,m)\)-convexity of \(\mu\), we have

\begin{align}\label{d} {e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}} \leq h\left(\frac{1}{2}\right)\left[{e^{\mu\left( \frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\right)}}+m {e^{\mu\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}\right]. \end{align}
(23)
Multiplying (23) with \(\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)\) and integrating over \([0,1]\), we have
\begin{align}\label{w} &{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}}\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)d\kappa \nonumber\\ &\leq h\left(\frac{1}{2}\right) \bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p){e^{\mu\left( \frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\right)}}d\kappa+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\mu\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}d\kappa\bigg]. \end{align}
(24)
Setting \(\nu(u)=\frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\) and \(\nu(v)=\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\) in (24), then by using (12), (13) and (14), the first inequality of (22) is obtained. Again from exponentially \((h,m)\)-convexity of \(\mu\), we have
\begin{align}\label{e} &e^{\mu\left( \frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\right)} +me^{\mu\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)} \\\nonumber &\leq h\left(\frac{\kappa}{2}\right)\left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right)+mh\left(\frac{2-\kappa}{2}\right)\left(e^{\mu(\nu(\beta))}+me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\right)\nonumber. \end{align}
(25)
Multiplying (25) with \(h\left(\frac{1}{2}\right) \kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)\) and integrating over \([0,1]\), we have
\begin{align}\label{x} &h\left(\frac{1}{2}\right)\bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\mu\left( \frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\right)}d\kappa+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\mu\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}d\kappa\nonumber\bigg]\\&\nonumber\leq h\left(\frac{1}{2}\right) \bigg[ \left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right)\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h\left(\frac{\kappa}{2}\right)d\kappa\nonumber\\&\;\;\;+m\left(e^{\mu(\nu(\beta))}+me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\right) \int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h\left(\frac{2-\kappa}{2}\right)d\kappa\bigg]. \end{align}
(26)
Putting \(\nu(u)=\frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\) and \(\nu(v)=\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\) in (26), then by using (12) and (13), the second inequality of (22) is obtained.

Corollary 2. Setting \(m=1\) in (22), the following inequalities for exponentially \(h\)-convex function can be obtained:

\begin{align}\label{lmo*} &\nonumber2{e^{\mu\left( \frac{\nu(\alpha)+\nu(\beta)}{2}\right)}}_{\nu}\xi^{\phi}_{\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+\nu(\beta)}{2}\right)\right) ^{+}}(\beta;p)\\\nonumber &\leq h\left(\frac{1}{2}\right) \left[\left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+\nu(\beta)}{2}\right)\right) ^{+}}e^{\mu\circ\nu}\right)(\beta;p)\right.\left.+ \left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+\nu(\beta)}{2}\right)\right) ^{-}}e^{\mu\circ\nu}\right)(\alpha;p)\right]\\ &\leq h\left(\frac{1}{2}\right) \frac{(\nu(\beta)-\nu(\alpha))^\phi}{2^{\phi}}\left(\!e^{\mu(\nu(\alpha))}+e^{\mu(\nu(\beta))}\right)\!\left[\!\int_{0}^{1}\!\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h\left(\frac{\kappa}{2}\right)\!d\kappa\!+\!\!\!\int_{0}^{1}\!\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)h\left(\!\frac{2-\kappa}{2}\!\right)\!d\kappa\right] \end{align}
(27)
where \(\bar{\psi}\) is same as in (21).

Remark 4.

  1. If we set \(h(\kappa)=\kappa\) in (22), then [33, Theorem 9] is obtained.
  2. If we set \(h(\kappa)=\kappa\) and \(m=1\) in (22), then [33, Corollary 2] is obtained.
  3. If we set \(\nu(u)=u\) and \(h(\kappa)=\kappa\) in (22), then [34, Theorem 2.4] is obtained.
  4. If we set \(\nu(u)=u\), \(h(\kappa)=\kappa\) and \(m=1\) in (22), then [34, Corollary 2.5] is obtained.
  5. If we set \(\nu(u)=u\) in (22), then [26, Theorem 2.2] is obtained.

3.Fractional Fejér-Hadamard Inequalities for exponentially \((h,m)\)-convex functions

In this section, we will give two versions of the generalized fractional Fejér-Hadamard inequality. To establish these inequalities exponentially \((h,m)\)-convexity and generalized fractional integrals operators have been used.

Theorem 14. Let \(\mu,\nu: [\alpha,m\beta]\subset[0,\infty)\to\mathbb{R}\), \(0< \alpha< m\beta\) be two functions such that \(\mu\) be integrable and \(\nu\) be differentiable. If \(\mu\) be exponentially \((h,m)\)-convex and \(\mu(\nu(v))=\mu(\nu(\alpha)+m\nu(\beta)-m\nu(v))\) and \(\nu\) be strictly increasing. Also, let \(\gamma : [\alpha,m\beta]\to\mathbb{R}\) be a function which is non-negative and integrable. Then for generalized fractional integral operators, the following inequalities hold:

\begin{align}\label{yy} &\notag {e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}} \left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}m^\sigma,\beta^{-}}e^{\gamma\circ\nu}\right)\left(\nu^{-1}\left(\frac{\nu(\alpha)}{m}\right);p\right) \leq {h\left(\frac{1}{2}\right)(1+m)\left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}m^\sigma,\beta^{-}}e^{\mu\circ\nu}e^{\gamma\circ\nu}\right)\left(\nu^{-1}\left(\frac{\nu(\alpha)}{m}\right);p\right)}\\\nonumber &\leq h\left(\frac{1}{2}\right) \frac{(m\nu(\beta)-\nu(\alpha))^\phi}{m^\phi}\bigg[\left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right)\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}h\left(\kappa\right)d\kappa\\ &\;\;\;+\!m\!\left(\!e^{\mu(\nu(\beta))}\!+\!me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\!\right) \!\!\int_{0}^{1}\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}h\left(1-\kappa\right)\!d\kappa\bigg],\, \end{align}
(28)
where \(\bar{\psi}\) is same as in (16).

Proof. Multiplying (17) with \(\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}\) and integrating over \([0,1]\), we have

\begin{align}\label{z} &\notag{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}}\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))} d\kappa\\\nonumber & \leq h\left(\frac{1}{2}\right) \bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p){e^{{\mu(\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta))}}}e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))} d\kappa\\ &\;\;\;+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p){e^{{\mu((1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}}}e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}d\kappa\bigg]. \end{align}
(29)
Setting \(\nu(v)=(1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta)\) in (29), then by using (13) and assumption \(\mu(\nu(v))=\mu(\nu(\alpha)+m\nu(\beta)-m\nu(v))\), the first inequality of (28) is obtained. Now multiplying (19) with \(h\left(\frac{1}{2}\right)\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}\) and integrating over \([0,1]\), we have
\begin{align}\label{23} &\notag h\left(\frac{1}{2}\right)\bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{{\mu(\kappa\nu(\alpha)+m(1-\kappa)\nu(\beta))}}e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))} d\kappa\\ \nonumber&\;\;\;+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{{\mu((1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}}e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}d\kappa\bigg]\\&\nonumber\leq\! h\!\left(\!\frac{1}{2}\!\right) \!\!\bigg[\!\!\left(\!e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\!\right)\!\!\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}h\left(\kappa\right)d\kappa\\ &\;\;\;+\!m\!\left(\!e^{\mu(\nu(\beta))}\!+\!me^{\mu\left(\frac{\nu(\alpha)}{m^2}\right)}\!\right) \!\!\int_{0}^{1}\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta))}h\left(1-\kappa\right)\!d\kappa\bigg]. \end{align}
(30)
Setting \(\nu(v)=(1-\kappa)\frac{\nu(\alpha)}{m}+\kappa\nu(\beta)\) in (30), then by using (13) and assumption \(\mu(\nu(v))=\mu(\nu(\alpha)+m\nu(\beta)-m\nu(v))\), the second inequality of (28) is obtained.

Corollary 3. Setting \(m=1\) in (28), the following inequalities for exponentially \(h\)-convex function can be obtained:

\begin{align}\label{yy**} &\notag{e^{\mu\left( \frac{\nu(\alpha)+\nu(\beta)}{2}\right)}} \left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi},\beta^{-}}e^{\gamma\circ\nu}\right)\left(\alpha;p\right) \leq {2 h\left(\frac{1}{2}\right)\left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi},\beta^{-}}e^{\mu\circ\nu}e^{\gamma\circ\nu}\right)\left(\alpha;p\right)}\\\nonumber &\leq h\left(\frac{1}{2}\right) {(\nu(\beta)-\nu(\alpha))^\phi}\left(e^{\mu(\nu(\alpha))}+e^{\mu(\nu(\beta))}\right)\bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa){\nu(\alpha)}+\kappa\nu(\beta))}h\left(\kappa\right)d\kappa\\ &\;\;\;+ \int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\gamma( (1-\kappa){\nu(\alpha)}+\kappa\nu(\beta))}h\left(1-\kappa\right)d\kappa\bigg], \end{align}
(31)
where \(\bar{\psi}\) is same as in (21).

Remark 5.

  1. If we set \(h(\kappa)=\kappa\) in (28), then [33, Theorem 10] is obtained.
  2. If we set \(h(\kappa)=\kappa\) and \(m=1\) in (28), then [33, Corollary 3] is obtained.
  3. If we set \(\nu(u)=u\) and \(h(\kappa)=\kappa\) in (28), then [34, Theorem 2.7] is obtained.
  4. If we set \(\nu(u)=u\), \(h(\kappa)=\kappa\) and \(m=1\) in (28), then [34, Corollary 2.8] is obtained.
  5. If we set \(\nu(u)=u\) in (28), then [26, Theorem 2.3] is obtained.

In the following we give another generalized fractional version of the Fejér-Hadamard inequality.

Theorem 15. Let \(\mu,\nu: [\alpha,m\beta]\subset[0,\infty)\to\mathbb{R}\), \(0< \alpha< m\beta\) be two functions such that \(\mu\) be integrable and \(\nu\) be differentiable. If \(\mu\) be exponentially \((h,m)\)-convex and \(\mu(\nu(v))=\mu(\nu(\alpha)+m\nu(\beta)-m\nu(v))\) and \(\nu\) be strictly increasing. Also, let \(\gamma : [\alpha,m\beta]\to\mathbb{R}\) be a function which is non-negative and integrable. Then for generalized fractional integral operators, the following inequalities hold:

\begin{align}\label{yy*} &\notag{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}} \!\!\left(\!_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}(2m)^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+m\nu(\beta)}{2m}\right)\right) ^{-}}e^{\gamma\circ\nu}\!\right)\!\left(\!\nu^{-1}\!\left(\frac{\nu(\alpha)}{m}\!\right);p\!\right) \\&\nonumber\leq \!h\!\left(\!\frac{1}{2}\!\right) {\!(1\!+\!m)\!\!\left(\!\!_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}(2m)^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+m\nu(\beta)}{2m}\right)\right) ^{-}}e^{\mu\circ\nu}e^{\gamma\circ\nu}\!\!\right)\!\!\left(\!\!\nu^{-1}\!\left(\!\frac{\nu(\alpha)}{m}\right);p\!\right)}\\\nonumber &\leq h\left(\frac{1}{2}\right) \frac{(m\nu(\beta)-\nu(\alpha))^\phi}{(2m)^\phi}\bigg[\left(e^{\mu(\nu(\alpha))}+me^{\mu(\nu(\beta))}\right)\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}h\left(\frac{\kappa}{2}\right)d\kappa\\ &\;\;\;+\!m\!\!\left(\!e^{\mu(\nu(\beta))}\!+\!me^{\mu\left(\frac{\nu(\alpha)}{m^2}\!\right)}\right)\!\!\!\int_{0}^{1}\!\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\!\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\!\right)}}h\!\left(\!\frac{2\!-\!\kappa}{2}\!\right)\!d\kappa\bigg], \end{align}
(32)
where \(\bar{\psi}\) is same as in (16).

Proof. Multiplying (23) with \(\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}\) and integrating over \([0,1]\), we have

\begin{align}\label{z*} &\notag{e^{\mu\left( \frac{\nu(\alpha)+m\nu(\beta)}{2}\right)}}\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}} d\kappa\\\nonumber & \leq h\left(\frac{1}{2}\right) \bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p){e^{\mu\left( \frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\right)}} {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}} d\kappa\\ &\;\;\;+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\mu\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}} {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}d\kappa\bigg]. \end{align}
(33)
Setting \(\nu(v)=\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\) in 33), then by using (13) and assumption \(\mu(\nu(v))=\mu(\nu(\alpha)+m\nu(\beta)-m\nu(v))\), the first inequality of (32) is obtained. Now multiplying (25) with \(h\left(\frac{1}{2}\right)\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}\) and integrating over \([0,1]\), we have
\begin{align}\label{24} &\notag h\left(\frac{1}{2}\right)\bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\mu\left( \frac{\kappa}{2}\nu(\alpha)+m\frac{(2-\kappa)}{2}\nu(\beta)\right)} {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}} d\kappa\\ \nonumber&+m\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p)e^{\mu\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)} {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}d\kappa\bigg]\\&\nonumber\leq\! h\!\left(\!\frac{1}{2}\!\right)\!\! \bigg[\!\!\left(\!e^{\mu(\nu(\alpha))}\!+\!me^{\mu(\nu(\beta))}\!\right)\!\!\int_{0}^{1}\!\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\right)}}h\left(\frac{\kappa}{2}\right)\!d\kappa\\ &\;\;\;+\!m\!\!\left(\!e^{\mu(\nu(\beta))}\!+\!me^{\mu\left(\frac{\nu(\alpha)}{m^2}\!\right)}\right)\!\!\!\int_{0}^{1}\!\!\!\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\!\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\!\right)}}h\!\left(\!\frac{2\!-\!\kappa}{2}\!\right)\!d\kappa\bigg]. \end{align}
(34)
Setting \(\nu(v)=\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}\frac{\nu(\alpha)}{m}\) in (34), then by using (13) and assumption \(\mu(\nu(v))=\mu(\nu(\alpha)+m\nu(\beta)-m\nu(v))\), the second inequality of (32) is obtained.

Corollary 4. Setting \(m=1\) in (32), the following inequalities for exponentially \(h\)-convex function can be obtained:

\begin{align}\label{yy***} &\notag{e^{\mu\left( \frac{\nu(\alpha)+\nu(\beta)}{2}\right)}} \left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+\nu(\beta)}{2}\right)\right) ^{-}}e^{\gamma\circ\nu}\right)\left(\alpha;p\right)\leq 2h\left(\frac{1}{2}\right) {\left(_{\nu}\Upsilon^{\varsigma,r,q,c}_{\sigma,\phi,l,\bar{\psi}2^\sigma,\left(\nu^{-1}\left(\frac{\nu(\alpha)+\nu(\beta)}{2}\right)\right) ^{-}}e^{\mu\circ\nu}e^{\gamma\circ\nu}\right)\left(\alpha;p\right)}\\\nonumber &\leq h\left(\frac{1}{2}\right) \frac{(\nu(\beta)-\nu(\alpha))^\phi}{2^\phi}\left(e^{\mu(\nu(\alpha))}+e^{\mu(\nu(\beta))}\right)\bigg[\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}{\nu(\alpha)}\right)}}h\left(\frac{\kappa}{2}\right)d\kappa\\ &\;\;\;+\int_{0}^{1}\kappa^{\phi-1}E_{\sigma,\phi,l}^{\varsigma,r,q,c}(\psi \kappa^{\sigma};p) {e^{\gamma\left(\frac{\kappa}{2}\nu(\beta)+\frac{(2-\kappa)}{2}{\nu(\alpha)}\right)}}h\left(\frac{2-\kappa}{2}\right)d\kappa\bigg], \end{align}
(35)
where \(\bar{\psi}\) is same as in (21).

Remark 6.

  1. If we set \(h(\kappa)=\kappa\) in (32), then [33, Theorem 11] is obtained.
  2. If we set \(h(\kappa)=\kappa\) and \(m=1\) in (32), then [33, Corollary 4] is obtained.

Remark 7. By setting \(h(\kappa)=\kappa^s\) and \(m=1\) in Theorems 12, 13, 14 and 15, the Hadamard and the Fejér-Hadamard inequalities for exponentially \(s\)-convex functions can be obtained. We leave it for interested reader.

4.Concluding remarks

In this article, we established the Hadamard and the Fejér-Hadamard inequalities. To established these inequalities generalized fractional integral operators and exponentially \((h,m)\)-convexity have been used. The presented results hold for various kind of exponentially convexity and well known fractional integral operators given in Remarks 1 and 2. Moreover, the established results have connection with already published results.

Acknowledgments

The research work of the Ghulam Farid is supported by Higher Education Commission of Pakistan under NRPU 2016, Project No. 5421.

Autho Contributions

All authors contributed equally to the writing of this paper. All authors read and approved the final manuscript.

Conflict of Interests

The authors declare no conflict of interest.

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Leap Zagreb and leap hyper-Zagreb indices of Jahangir and Jahangir derived graphs https://old.pisrt.org/psr-press/journals/easl-vol-3-issue-2-2020/leap-zagreb-and-leap-hyper-zagreb-indices-of-jahangir-and-jahangir-derived-graphs/ Thu, 09 Apr 2020 13:41:22 +0000 https://old.pisrt.org/?p=4003
EASL-Vol. 3 (2020), Issue 2, pp. 1 - 8 Open Access Full-Text PDF
Fatima Asif, Zohaib Zahid, Sohail Zafar
Abstract: Topological indices are numerical parameters of a graph which characterize its topology. The second degree of a vertex in a graph is equal to the number of its second neighbors. In this paper, we will compute leap Zagreb indices and leap hyper-Zagreb indices of Jahangir graph and its line graph based on the 2-distance degree of the vertices. Moreover we will compute the same indices for the subdivision graph and the line graph of the subdivision of Jahangir graph.
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Engineering and Applied Science Letter

Leap Zagreb and leap hyper-Zagreb indices of Jahangir and Jahangir derived graphs

Fatima Asif, Zohaib Zahid\(^1\), Sohail Zafar
Department of Mathematics, University of Management and Technology, Lahore Pakistan.; (F.A & Z.Z & S.Z)

\(^{1}\)Corresponding Author: zohaib_zahid@hotmail.com

Abstract

Topological indices are numerical parameters of a graph which characterize its topology. The second degree of a vertex in a graph is equal to the number of its second neighbors. In this paper, we will compute leap Zagreb indices and leap hyper-Zagreb indices of Jahangir graph and its line graph based on the 2-distance degree of the vertices. Moreover we will compute the same indices for the subdivision graph and the line graph of the subdivision of Jahangir graph.

Keywords:

Leap Zagreb indices, leap hyper-Zagreb indices, F-leap indices, Jahangir graph, second degree.

1. Introduction

Chemical graph theory, a branch of mathematical chemistry, applies graph theory to mathematical modeling of chemical phenomena. Topological indices are real numbers that are presented as graph parameters (e.g. the degree of vertices, distances, etc.) introduced during studies conducted on the molecular graphs in chemistry and can describe some physical and chemical properties of molecules.

Let \(G\) be a simple and connected graph with order \(V(G)\) and size \(E(G)\subseteq V(G) \times V(G)\). The degree \(d_u\) of any vertex \(u\) is defined as the number of vertices joined to that vertex \(u\). The distance between two vertices \(u\) and \(v\) of a graph \(G\) is the number of edges in a shortest path connecting them and is denoted by \(d(u, v)\). The subdivision graph \(S(G)\) is a graph resulting from the subdivision of all the edges of \(G\). The line graph \(L(G)\) of a graph \(G\) whose vertices are the edges of \(G\), with \(uv\in E(L(G))\) when \(u\) and \(v\) have a common end point in \(G\). In structural chemistry, line graph of a graph \(G\) is very useful. The first topological indices on the basis of line graph was introduced by Bertz in 1981 (see [1]). The topological indices of Jahangir graph and its line graph are computed by many researchers (see [2, 3, 4, 5]).

For a vertex \(v\) in \(G\), the open \(k-\)neighborhood of \(v\) is defined as \(N_{k}(v/G) = \{u \in V(G): d(u, v) = k\}\), where \(k\) is a positive integer. The \(k-\)distance degree, denoted by \(d_{k}(v/G)\), of a vertex \(v \in V(G)\) is the number of \(k-\)neighbors of \(v\) in \(G\), \(i.e.,\) \(d_k(v/G) = |N_k(v/G)|\). It is clear that \(d_1(v/G) = d_v\) for every \(v \in V(G)\). The \(2-\)distance degree of a vertex \(v\) consists of all vertices at distance two to \(v\).

Recently, leap Zagreb indices of a graph have been introduced by Naji et al., (see [6]), depending on \(2-\)distance degree of the vertices. The leap Zagreb indices have several chemical applications. The first leap Zagreb index has very good correlation with physical properties of chemical compounds like boiling point, entropy, \(DHVAP\), \(HVAP\) and accentric factor (see [7]). Shiladhar et al., computed leap Zagreb indices of some wheel related graphs (see [8]). For more details about leap indices, see [9, 10, 11, 12].

For a graph \(G\), the first, second, and third leap Zagreb indices are defined as:
\begin{equation} LM_1(G) =\sum_{v \in V(G)} (d_{2}(v/G))^2, \end{equation}
(1)
\begin{equation} LM_2(G) =\sum_{uv \in E(G)} d_{2}(u/G)(d_{2}(v/G), \end{equation}
(2)
\begin{equation} LM_3(G) =\sum_{v \in V(G)} d_{1}(v/G)d_{2}(v/G). \end{equation}
(3)
The first and second leap-hyper Zagreb indices were introduced by Kulli [13] as:
\begin{equation} HLM_1(G)=\sum_{uv \in E(G)} [d_{2}(u/G)+d_{2}(v/G)]^2,\label{4} \end{equation}
(4)
\begin{equation} HLM_2(G)=\sum_{uv \in E(G)} [d_{2}(u/G)d_{2}(v/G)]^2. \label{5} \end{equation}
(5)
Later on, Basavanagoud and Chitra computed leap hyper-Zagreb indices of some nanostructures [14]. In 2019, Kulli et al., computed leap hyper-Zagreb indices of certain windmill graphs [15].

2. Leap Zagreb and leap hyper-Zagreb indices of Jahangir graph \(J_{n,m}\)

In this section, we will compute leap Zagreb indices and hyper-leap Zagreb indices of Jahangir graph \(J_{n,m}\). The Jahangir graph \(J_{n,m}\) consists of a cycle \(C_{nm}\) with one additional vertex which is adjacent to \(m\) vertices of \(C_{nm}\) at distance to each other [16].

Figure 1. The Jahangir graph \(J_{n,m}\).

Theorem 1. Let \(J_{n,m}\) be the Jahangir graph, then

  1. \(LM_1(J_{n,m})=m^3+6m^2+4mn+7m\).
  2. \(LM_2(J_{n,m})=2m^3+8m^2+4mn+2m\).
  3. \(LM_3(J_{n,m})=5m^2+4mn+3m.\)
  4. \(HLM_1(J_{n,m})=11m^3+22m^2+16mn+19m.\)
  5. \(HLM_2(J_{n,m})=4m^5+8m^4+22m^3+36m^2+16mn+26m.\)

Proof. Let \(J_{n,m}\) be a Jahangir graph with \(m(n+1)\) edges and \(mn+1\) vertices as shown in Figure 1. For an edge \(uv \in E(J_{n,m})\), the \(2-\)distance degree of a vertex \(u\) and vertex \(v\) is denoted by \(d_2(u/J_{n,m})\) and \(d_2(v/J_{n,m})\) respectively. The edge partition of \(J_{n,m}\) with respect to \(2-\)distance degree of vertices of \(J_{n,m}\) is shown in Table 1. The vertex partition of graph \(J_{n,m}\) based on the \(1-\)distance degree of a vertex \(u\) and \(2-\)distance degree of a vertex \(u\) is shown in Table 2.

Table 1. The edge partition of \(J_{n,m}\), where \(d_2(u/J_{n,m})d_2(v/J_{n,m})\) \(\in E(J_{n,m})\).
No. of edges \(d_2(u/J_{n,m})\) \(d_2(v/J_{n,m})\)
\(m(n-4)\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(2m\) \(3\) \(m+1\)
\(m\) \(2m\) \(m+1\)
Table 2. The vertex partition of \(J_{n,m}\) where \(d_1(v/J_{n,m})\), \(d_2(v/J_{n,m})\) \(\in V(J_{n,m})\).
No. of vertices \(d_1(v/J_{n,m})\) \(d_2(v/J_{n,m})\)
\(1\) \(m\) \(2m\)
\(m(n-3)\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(m\) \(3\) \(m+1\)
  1. Using Formula (1) and Table 2, we have \begin{eqnarray*} LM_1(J_{n,m})&=&1.(2m)^2+m(n-3)(2)^2+2m(3)^2+m(m+1)^2\\ &=&m^3+6m^2+4mn+7m. \end{eqnarray*}
  2. Using Formula (2) and Table 1, we have \begin{eqnarray*} LM_2(J_{n,m})&=&m(n-4)(2.2)+2m(2.3)+2m(3.(m+1))+m(2m.(m+1))\\ &=&2m^3+8m^2+4mn+2m. \end{eqnarray*}
  3. Using Formula (3) and Table 2, we have \begin{eqnarray*} LM_3(J_{n,m})&=&1.(2m.m)+m(n-3)(2.2)+m(3.(m+1))+2m(3.2)\\ &=&5m^2+4mn+3m. \end{eqnarray*}
  4. Using Formula (4) and Table 1, we have \begin{eqnarray*} HLM_1(J_{n,m})&=&m(n-4)(2+2)^2+2m(2+3)^2+2m(3+(m+1))^2+m(2m+(m+1))^2\\ &=&11m^3+22m^2+16mn+19m. \end{eqnarray*}
  5. Using Formula (5) and Table 1, we have \begin{eqnarray*} HLM_2(J_{n,m})&=&m(n-4)(2.2)^2+2m(2.3)^2+2m(3.(m+1))^2+m(2m.(m+1))^2\\ &=&4m^5+8m^4+22m^3+36m^2+16mn+26m. \end{eqnarray*}

3. Leap Zagreb and leap hyper-Zagreb indices of the line graph of Jahangir graph \(J_{n,m}\)

In this section, we will compute leap Zagreb indices and hyper-leap Zagreb indices of the line graph of Jahangir graph \(J_{n,m}\).

Figure 2. The line graph of Jahangir graph \(J_{n,m}\)

Theorem 2. Let \(L(J_{n,m})\) be the line graph of the Jahangir graph \(J_{n,m}\), then

  1. \(LM_1(L(J_{n,m}))=m^3+2m^2+4mn+11m\).
  2. \(LM_2(L(J_{n,m}))=2m^4+3m^3+12m^2+4mn-m\).
  3. \(LM_3(L(J_{n,m}))=2m^3+8m^2+4mn+2m\).
  4. \(HLM_1(L(J_{n,m}))=8m^4+13m^3+30m^2+16mn+5m\).
  5. \(HLM_2(L(J_{n,m}))=8m^6+16m^4+27m^3+38m^2+16mn+11m\).

Proof. Let \(L(J_{n,m})\) be a line graph of Jahangir graph \(J_{n,m}\) with \(\frac{m^2+2mn+3m}{2}\) edges and \(m(n+1)\) vertices is shown in Figure 2. For an edge \(uv \in E(L(J_{n,m}))\), the \(2\)-distance degree of a vertex \(u\) and vertex \(v\) is denoted by \(d_2(u/L(J_{n,m}))\) and \(d_2(v/L(J_{n,m}))\) respectively. The edge partition of \(L(J_{n,m})\) with respect to \(2\)-distance degree of vertices of \(L(J_{n,m})\) is shown in Table 3. The vertex partition of graph \(L(J_{n,m})\) based on the \(1\)-distance degree of a vertex \(u\) and \(2\)-distance degree of a vertex \(u\) is shown in Table 4.

Table 3. The edge partition of \(L(J_{n,m})\), where \(d_2(u/L(J_{n,m}))d_2(v/L(J_{n,m}))\) \(\in\) \(E(L(J_{n,m}))\).
Number of edges \(d_2(u/L(J_{n,m}))\) \(d_2(v/L(J_{n,m}))\)
\(m(n-5)\) \(2\) \(2\)
\(2m\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(m\) \(3\) \(3\)
\(2m\) \(3\) \(m+1\)
\(\frac{m(m-1)}{2}\) \(m+1\) \(m+1\)
Table 4. The vertex partition of \(L(J_{n,m})\) where \(d_1(v/L(J_{n,m}))\), \(d_2(v/L(J_{n,m}))\) \(\in V(L(J_{n,m}))\).
No. of \(1-\)distance degree vertices \(d_1(u/L(J_{n,m}))\) No. of \(2-\)distance degree vertices \(d_2(u/L(J_{n,m}))\)
\(m(n-4)\) \(2\) \(m(n-4)\) \(2\)
\(2m\) \(2\) \(2m\) \(3\)
\(2m\) \(3\) \(m\) \(2m\)
\(m\) \(m+1\) \(2m\) \(m+1\)
  1. Using Formula (1) and Table 4, we have \begin{eqnarray*} LM_1(L(J_{n,m}))&=&m(n-4)(2)^2+2m(2)^2+2m(3)^2+m(m+1)^2\\ &=&m^3+2m^2+4mn+11m. \end{eqnarray*}
  2. Using Formula (2) and Table 3, we have \begin{eqnarray*} LM_2(L(J_{n,m}))&=&m(n-5)(2.2)+2m(2.3)+2m(3.(m+1))+m(m+1)^2+2m(2m.(m+1))\\&&+\frac{m(m-1)}{2}(2m.2m)\\ &=&2m^4+3m^3+12m^2+4mn-m. \end{eqnarray*}
  3. Using Formula (3) and Table 4, we have \begin{eqnarray*} LM_3(L(J_{n,m}))&=&m(n-4)(2.2)+m.(2m.(m+1))+2m(3.(m+1))+2m(3.2)\\ &=&2m^3+8m^2+4mn+2m. \end{eqnarray*}
  4. Using Formula (4) and Table 3, we have \begin{eqnarray*} HLM_1(L(J_{n,m}))&=&m(n-5)(2+2)^2+2m(2+3)^2+2m(3+(m+1))^2+m(m+1)^2\\&&+2m(2m+(m+1))^2+\frac{m(m-1)}{2}(2m+2m)^2\\ &=&8m^4+13m^3+30m^2+16mn+5m. \end{eqnarray*}
  5. Using Formula (5) and Table 3, we have \begin{eqnarray*} HLM_2(L(J_{n,m}))&=&m(n-5)(2.2)^2+2m(2.3)^2+2m(3.(m+1))^2+m(m+1)^2\\&&+2m(2m.(m+1))^2+\frac{m(m-1)}{2}(2m.2m)^2\\ &=&8m^6+16m^4+27m^3+38m^2+16mn+11m. \end{eqnarray*}

4. Leap Zagreb and leap-hyper Zagreb indices of the subdivision of Jahangir Graph \(J_{n,m}\)

In this section, we will compute leap Zagreb indices and hyper-leap Zagreb indices of the subdivision of Jahangir graph \(J_{n,m}\).

Figure 3. The subdivision of Jahangir graph \(J_{n,m}\)

Theorem 3. Let \(S(J_{m,n})\) be the subdivision graph of the Jahangir graph \(J_{m,n}\), then

  1. \(LM_1(S(J_{n,m}))=m^3+3m^2+8mn+16m\).
  2. \(LM_2(S(J_{n,m}))=m^3+4m^2+8mn+17m \).
  3. \(LM_3(S(J_{n,m}))=3m^2+4mn+11m\).
  4. \(HLM_1(S(J_{n,m}))=5m^3+12m^2+32mn+75m\).
  5. \(HLM_2(S(J_{n,m}))=m^5+2m^4+10m^3+18m^2+32mn+179m\).

Proof. Let \(S(J_{n,m})\) be a subdivision of Jahangir graph with \(2m(n+1)\) edges and \(m(2n+1)+1\) vertices is shown in Figure 3. For an edge \(uv \in E(S(J_{n,m}))\), the \(2-\)distance degree of a vertex \(u\) and vertex \(v\) is denoted by \(d_2(u/S(J_{n,m}))\) and \(d_2(v/S(J_{n,m}))\) respectively. The edge partition of \(E(S(J_{n,m}))\) with respect to \(2-\)distance degree of a vertex \(u\) in \(S(J_{n,m})\) is shown in Table 5. The vertex partition of graph \(S(J_{n,m})\) based on the \(1-\)distance degree of a vertex \(u\) and \(2-\)distance degree of a vertex \(u\) is shown in Table 6. \begin{table}[H] \centering

Table 5. The edge partition of \(S(J_{n,m})\), where \(d_2(u/S(J_{n,m}))d_2(v/S(J_{n,m}))\) \(\in E(S(J_{n,m}))\).
No. of edges \(d_2(u/S(J_{n,m}))\) \(d_2(v/S(J_{n,m}))\)
\(2m(n-2)\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(2m\) \(3\) \(3\)
\(m\) \(3\) \(m+1\)
\(m\) \(m\) \(m+1\)
Table 6. The vertex partition of \(S(J_{n,m})\), where \(d_1(v/S(J_{n,m}))\), \(d_2(v/S(J_{n,m}))\) \(\in V(S(J_{n,m}))\).
No. of vertices \(d_1(v/S(J_{n,m}))\) \(d_2(v/S(J_{n,m}))\)
\(1\) \(m\) \(m\)
\(m(2n-3)\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(m\) \(2\) \(3\)
\(m\) \(3\) \(m+1\)
  1. Using Formula (1) and Table 6, we have \begin{eqnarray*} LM_1[S(J_{n,m})]&=&1.(m)^2+m(2n-3)(2)^2+2m(3)^2+m(3)^2+m(m+1)^2\\ &=&m^3+3m^2+8mn+16m. \end{eqnarray*}
  2. Using Formula (2) and Table 5, we have \begin{eqnarray*} LM_2[S(J_{n,m})]&=&2m(n-2)(2.2)+2m(2.3)+2m(3.3)+m(3.(m+1))+m(m.(m+1))\\ &=&m^3+4m^2+8mn+17m. \end{eqnarray*}
  3. Using Formula (3) and Table 6, we have \begin{eqnarray*} LM_3[S(J_{n,m})]&=&1.(m.m)+m(n-3)(2.2)+2m(2.3)+m(3.3)+m(2.(m+1))\\ &=&3m^2+4mn+11m. \end{eqnarray*}
  4. Using Formula (4) and Table 5, we have \begin{eqnarray*} HLM_1[S(J_{n,m})]&=&2m(n-2)(2+2)^2+2m(2+3)^2+2m(3+3)^2+m(3+(m+1))^2+m(m+(m+1))^2\\ &=&5m^3+12m^2+32mn+75m. \end{eqnarray*}
  5. Using Formula (5) and Table 5, we have \begin{eqnarray*} HLM_2[S(J_{n,m})]&=&2m(n-2)(2.2)^2+2m(2.3)^2+2m(3.3)^2+m(3.(m+1))^2+m(m.(m+1))^2\\ &=&m^5+2m^4+10m^3+18m^2+32mn+179m. \end{eqnarray*}

5. Leap Zagreb and leap-hyper Zagreb indices of line graph of the subdivision of Jahangir graph \(J_{n,m}\)

In this section, we will compute leap Zagreb indices and hyper-leap Zagreb indices of the line graph of the subdivision of Jahangir graph \(J_{n,m}\).

Figure 4. The line graph of the subdivision of Jahangir graph \(J_{n,m}\).

Theorem 4. Let \(L[(S(J_{n,m}))]\) be the line graph of the subdivision of Jahangir graph \(J_{n,m}\), then

  1. \(LM_1[L(S(J_{n,m}))]=2m^3+4m^2+8mn+22m\).
  2. \(LM_2[L(S(J_{n,m}))]=\frac{1}{2}[m^4+3m^3+15m^2+8mn+51m]\).
  3. \(LM_3[L(S(J_{n,m}))]=m^3+4m^2+8mn+17m\).
  4. \(HLM_1[L(S(J_{n,m}))]=\frac{1}{2}[4m^4+16m^3+44m^2+64mn+224m]\).
  5. \(HLM_2[L(S(J_{n,m}))]=\frac{1}{2}[m^6+5m^5+10m^4+46m^3+77m^2+64mn+507m]\).

Proof. Let \(L(S(J_{n,m}))\) be the line graph of the subdivision of Jahangir graph \(J_{n,m}\) with \(\frac{m^2+4mn+5m}{2}\) edges and \(2m(n+1)\) vertices is shown in Figure 4. For an edge \(uv \in E[L(S(J_{n,m}))]\), the \(2-distance\) degree of a vertex \(u\) and vertex \(v\) is denoted by \(d_2(u/L(S(J_{n,m})))\) and \(d_2(v/L(S(J_{n,m})))\) respectively. The edge partition of \(E[L(S(J_{n,m}))]\) with respect to \(2-\)distance degree of a vertex \(u\) in \(L(S(J_{n,m}))\) is shown in Table 7. The vertex partition of graph \(L(S(J_{n,m}))\) based on the \(1-\)distance degree of a vertex \(u\) and \(2-\)distance degree of a vertex \(u\) is shown in Table 8.

Table 7. The edge partition of \(L(S(J_{n,m}))\), where \(d_2(u/L(S(J_{n,m})))d_2(v/L(S(J_{n,m})))\) \(\in E(L(S(J_{n,m})))\).
No. of edges \(d_2(u/L(S(J_{n,m})))\) \(d_2(v/L(S(J_{n,m})])\)
\(m(2n-5)\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(3m\) \(3\) \(3\)
\(2m\) \(3\) \(m+1\)
\(\frac{m(m+1)}{2}\) \(m+1\) \(m+1\)
Table 8. The vertex partition of \(L[S(J_{n,m})]\), where \(d_1(u/L(S(J_{n,m})))\), \(d_2(u/L(S(J_{n,m})))\) \(\in V(L(S(J_{n,m})))\).
No. of vertices \(d_1(u/L(S(J_{n,m})))\) \(d_2(u/L(S(J_{n,m})))\)
\(2m(n-2)\) \(2\) \(2\)
\(2m\) \(2\) \(3\)
\(2m\) \(3\) \(3\)
\(m\) \(3\) \(m+1\)
\(m\) \(m\) \(m+1\)
  1. Using Formula (1) and Table 8, we have \begin{eqnarray*} LM_1[L(S(J_{n,m}))]&=&4m(3)^2+2m(n-2)(2)^2+2m(m+1)^2\\ &=&2m^3+4m^2+8mn+22m. \end{eqnarray*}
  2. Using Formula (2) and Table 7, we have \begin{eqnarray*} LM_2[L(S(J_{n,m}))] &=&m(2n-5)(2)^2+2m(2.3)+3m(3)^2+2m(3.(m+1))+\frac{m(m+1)^3}{2}\\ &=&\frac{1}{2}[m^4+3m^3+15m^2+8mn+51m]. \end{eqnarray*}
  3. Using Formula (3) and Table 8, we have \begin{eqnarray*} LM_3[L(S(J_{n,m}))]&=&2m(n-2)(2.2)+2m(2.3)+2m(3.3)+m(3.(m+1))+m(m.(m+1))\\ &=&m^3+4m^2+8mn+17m. \end{eqnarray*}
  4. Using Formula (4) and Table 7, we have \begin{eqnarray*} HLM_1[L(S(J_{n,m}))]&=&m(2n-5)(2+2)^2+2m(2+3)^2+3m(3+3)^2+2m(3+(m+1))^2\\ &&+\frac{m(m+1)}{2}[(m+1)+(m+1)]^2\\ &=&\frac{1}{2}[4m^4+16m^3+44m^2+64mn+224m]. \end{eqnarray*}
  5. Using Formula (5) and Table 7, we have \begin{eqnarray*} HLM_2[L(S(J_{n,m}))] &=&m(2n-5)(2.2)^2+2m(2.3)^2+3m(3.3)^2+2m(3.(m+1))^2\\ &&+\frac{m(m+1)}{2}[(m+1).(m+1)]^2\\ &=&\frac{1}{2}[m^6+5m^5+10m^4+46m^3+77m^2+64mn+507m]. \end{eqnarray*}

Autho Contributions

All authors contributed equally to the writing of this paper. All authors read and approved the final manuscript.

Conflict of Interests

The authors declare no conflict of interest.

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