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Articles

Exponential and non-Exponential Based Generalized Similarity Measures for Complex Hesitant Fuzzy Sets with Applications

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Pages 38-70 | Received 26 Mar 2020, Accepted 01 Jun 2020, Published online: 07 Jan 2021

Abstract

The purpose of this manuscript is to explore the notion of a complex hesitant fuzzy set (CHFS), as a generalization of the hesitant fuzzy set (HFS) and complex fuzzy set (CFS) to cope with the uncertain and complicated information in the real-world decision. CHFS contains truth grades in the form of a subset of the unit disc in the complex plane. The operational laws of the explored notion are also described. Further, the exponential based generalized similarity measures, without exponential based generalized similarity measures, and their important characteristics are also explored. These similarity measures are applied in the environment of pattern recognition and medical diagnosis to evaluate the proficiency and feasibility of the established measures. We also solved some numerical examples using the established measures. To examine the reliability and validity of the proposed measures by comparing it with existing measures. The advantages, comparative analysis, and graphical representation of the explored measures and existing measures are also discussed in detail.

1. Introduction

The theory of fuzzy set (FS) was firstly explored by Zadeh [Citation1] in 1965 which successfully applied in different fields. FS contains one function, called truth grade, belonging to the unit interval. FS has gained extensive achievement and various researchers have utilized it in the environment of medical diagnosis [Citation2–4], pattern recognition [Citation5], decision making [Citation6], and clustering algorithm. Moreover, the concept of interval-valued FS (IVFS) was established by Zadeh [Citation7], which contains the grade of truth in the form of some closed subinterval of the unit interval. Couso et al. [Citation8] defined a formal relational study of similarity and dissimilarity measures between FSs. The SM between FSs and between elements is described by Lee-Kwang et al. [Citation9]. Pramanik and Mondal [Citation10] presented weighted fuzzy SM based on tangent function and its discussed application to medical diagnosis. Some new SMs on FSs are defined by Wang [Citation11]. Kwon [Citation12] also defined SM based on FSs. A new approach to fuzzy distance measure and SM between generalized fuzzy numbers was described by Guha and Chakraborty [Citation13]. Kakati [Citation14] explored a note on the new similarity measure for FSs. Some SMs based on FSs are presented by Hesamian [Citation15] to find about the closeness between two objects.

Various researchers arise a question, what will happen when the range of FS changes to complex numbers form a unit disc in a complex plan instead of a real number. Ramot et al. [Citation16] introduced the idea of complex FS (CFS), which contains the truth grade in the form of a complex number by a member of a unit disc in the complex plane. CFS deals with two dimensions in a single set. CFS is a powerful procedure to illustrate the belief of a human being in the formation of grades. Bi et al. [Citation17] described complex fuzzy arithmetic aggregation operators. Adaptive image restoration by a novel neuro-fuzzy approach using CFSs is presented by Li [Citation18]. A systematic review of CFSs and logic is described by Yazdanbakhsh and dick [Citation19]. Dai [Citation20] wrote some comments on complex fuzzy logic. Jun and Xin [Citation21] applied CFSs to BCK/BCI-algebra. The orthogonality between CFSs and its application to signal detection is described by Hu et al. [Citation22]. Hu et al. [Citation23] also defined distances of CFSs and continuity of CF operations.

In the real decision making procedure, it is hard to set up the membership degree of FS due to the insufficiency of knowledge or data, hesitation, and many other reasons. To overcome such kind of issues Torra [Citation24] investigated the notion of the hesitant fuzzy set (HFS) which contains the grade of truth in the form of a subset of the unit interval. HFS is the generalization of FS to deal with uncertain and more complicated information in real decision theory. Xu and Xia [Citation25] explored distance and SMs for HFSs. Liao and Xu [Citation26] described subtraction and division operation over HFSs. Decomposition theorems and extension principles for HFSs are explored by Alcantud and Torra [Citation27]. Bishti and Kumar [Citation28] defined fuzzy time series forecasting method based on HFSs. Novel distance and SMs on HFSs with application to clustering analysis presented by Zhang and Xu [Citation29]. Alcantud and Giarlotta [Citation30] proposed an extension of Torra’s concept of HFSs. Farhadinia and Herrera-Viedma [Citation31] defined multiple criteria group decision-making method based on extended HFSs with unknown weight information. Distance and SMs between HFSs and their application in pattern recognition were stated by Zeng et al. [Citation32].

In real-life problems, we come across many situations where we need to quantify the uncertainty existing in the data to make optimal decisions. Exponential based similarity measures and without exponential based similarity measures are important tools for handling uncertain information present in our day-to-day life problems. Different measures, such as similarity, exponential, distance, entropy, and inclusion, process the uncertain information, and enable us to reach some conclusion. Recently, these measures have gained much attention from many authors due to their wide applications in various fields, such as pattern recognition, medical diagnosis, clustering analysis, and image segment. All the existing approaches of decision-makers, based on exponential based similarity measures and without exponential based similarity measures, in FS, CFS, and HFS theories, deal with membership functions belonging to a unit interval in the form of a subset in the concept of HFS. In CHFS theory, membership degrees are complex-valued and are represented in polar coordinates. These all notions worked effectively, but when a decision-maker faced such kinds of information which contains two-dimensional information in a single-set. For instance, 0.9ei2π(0.3),0.7ei2π(0.6),0.3ei2π(0.2),0.1ei2π(0.2), then the existing all notions are failed. For coping with such kind of problems, the CHFS is a proficient technique to resolve realistic decision problems in the environment of fuzzy set theory. CHFS is more powerful and more general than existing notions like HFS, CFS, and FS to cope with awkward and complicated information in real-life decisions. Because these all notions are the special cases of the explored CHFS. The advantages of the presented CHFS are discussed below:

  1. When we choose the imaginary parts of the CHFS as zero, then the CHFS is reduced into HFS which is in the form of 0.9,0.7,0.3,0.1.

  2. When we choose the CHFS as a singleton set, then the CHFS is reduced into CFS which is in the form of 0.9ei2π(0.3).

  3. When we choose the CHFS as a singleton set and the imaginary parts as zero, then the CHFS is reduced into FS which is in the form of 0.9.

Motivated by the above challenges and keeping the advantages of the CHFS, in this manuscript, some key contributions are made:

  1. To explore the novel approach of the complex hesitant fuzzy set (CHFS), which is the generalization of the hesitant fuzzy set (HFS) and complex fuzzy set (CFS) to cope with the uncertain and complicated information in the real-world decision. CHFS contains truth grades in the form of subset of the unit disc in the complex plane. Operational laws of the explored notion are also described and verified with the help of some numerical examples.

  2. To present some similarity measures is called exponential based similarity measures, without exponential based similarity measures, generalized similarity measures and their important characteristics are also explored.

  3. These similarity measures are utilized in the environment of pattern recognition and medical diagnosis to evaluate the proficiency and feasibility of the established measures. We solve some numerical examples using the established measures.

  4. To examine the reliability and validity of the proposed measures by comparing with existing measures. The advantages, comparative analysis, and graphical representation of the explored measures and existing measures are also discussed in detail. The graphical interpretation of the explored works is discussed with the help of .

Figure 1. The geometrical representation of the explored approach.

Figure 1. The geometrical representation of the explored approach.

The remainder of this manuscript is organized as follows: In Section 2, the notion of FSs, CFSs, HFSs are review. In Section 3, the purpose of this manuscript is to explore the notion of the complex hesitant fuzzy set (CHFS), as a mixture of the hesitant fuzzy set (HFS) and complex fuzzy set (CFS) to cope with the uncertain and complicated information in the real-world decision. CHFS contains truth grades in the form of a subset of the unit disc in a complex plane. The operational laws of the explored notion are also described. In Section 4, the exponential based similarity measures, without exponential based similarity measures, generalized similarity measures, and their important characteristics are also explored. In Section 5, these similarity measures are applied in the environment of pattern recognition and medical diagnosis to evaluate the proficiency and feasibility of the established measures. We solve some numerical examples using the established measures. To examine the reliability and validity of the proposed measures by comparing it with existing measures. The advantages, comparative analysis, and graphical representation of the explored measures and existing measures are also discussed in detail. The conclusion of this manuscript is discussed in Section 6.

2. Preliminaries

In this part of the article, we review basic definitions like FS, CFS, and HFS. Throughout this article X represents a fix set.

Definition 1

[Citation1]: A FS E is of the form: E=(x,μE(x))|xX with a condition 0μE(x)1, where μE(x) represents the grade of truth. Throughout this article, the collection of all FSs on X are denoted by FS(X). The pair E=(x,μE(x)) is called fuzzy number (FN).

Definition 2

[Citation16]: A CFS E is of the form: E=(x,μE(x)|xX where μE(x)=γE(x).ei2π(ωγE(x)) represents the complex-valued truth grade in the form of polar coordinate, where γE(x),ωγE(x)[0,1]. Further, the pair E=(x,γE(x).ei2π(ωγE(x))) is called complex fuzzy number (CFN).

Definition 3

[Citation24]: A HFS E is of the form: E=(x,μE(x))|xX where μE(x)is the set of different finite values in [0,1] representing the grade of truth for each element xX. Further, the pair E=(x,μE(x)) is called hesitant fuzzy number (HFN).

Definition 4

[Citation25]: For any two HFSs E and F, the similarity measure S(E,F) satisfies the following conditions:

  1. 0S(E,F)1;

  2. S(E,F)=1E=F;

  3. S(E,F)=S(F,E).

Definition 5

[Citation25]: For any two HFSs E and F, the distance measure d(E,F) satisfies the following conditions:

  1. 0d(E,F)1;

  2. d(E,F)=1E=F;

  3. d(E,F)=d(F,E).

From the above analysis, we obtain that the S(E,F)=1d(E,F).

3. Complex Hesitant Fuzzy Sets

In this portion, we presented the idea of complex hesitant fuzzy sets (CHFSs) and its some properties.

Definition 6:

A CHFS E is of the form: E=\{ (x,μE(x))|xX} where μE(x)=γEj(x).ei2π(ωγEj(x)),j=1,2,3,,n=γE1(x).ei2π(ωγE1(x)),γE2(x).ei2π(ωγE2(x)),,γEn(x).ei2π(ωγEn(x)) represented the complex-valued truth grade which is subset of unit disc in complex plane with a condition γEj(x),ωγEj(x)[0,1]. Further, E=(x,γEj(x).ei2π(ωγEj(x))) is called complex hesitant fuzzy number (CHFN).

Definition 7:

Let E=(x,γEj(x).ei2π(ωγEj(x))) and F=(x,γFj(x).ei2π(ωγFj(x))) be two CHFNs. Then

  1. c(γE(x))=(x,1γEj(x).ei2π(1ωγEj(x)));

  2. EF=(x,max(γEj(x),γFj(x)).ei2π(max(ωγEj(x),ωγFj(x))));

  3. EF=(x,min(γEj(x),γFj(x)).ei2π(min(ωγEj(x),ωγFj(x)))).

The notion of CHFS is an extensive powerful technique to cope with uncertain and awkward information in realistic decision theory. The CHFS contains the grade of supporting in the form of a subset of the unit disc in the complex plane, whose entities in the form of polar coordinates. Basically, the CHFS contains two-dimension information in a single set. The presented CHFS is more general than existing drawbacks, whose detailed and justifications are discussed are below:

In Definitions (6) and (7), if we choose the imaginary parts as zero, then the explored notion is converted for HFS, which is presented by Torra [Citation24]. Similarly, if we choose the CHFS as a singleton set, then the CHFS is converted for CFS, which is presented by Ramot et al. [Citation16]. Further, if we choose the CHFs as a singleton set and the imaginary part is zero, then the CHFS is converted for FS, which is explored by Zadeh [Citation1]. Due to its structure, it makes powerful and proficient to cope with uncertain and unreliable information in real decision theory.

Example 1:

Let E=(x1,0.9ei2π(0.3),0.7ei2π(0.6)),(x2,0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6)),(x3,0.6ei2π(0.8)),(x4,0.7ei2π(0.5),0.9ei2π(0.1),0.3ei2π(0.6)) and F=(x1,0.8ei2π(0.6),0.1ei2π(1)),(x2,0.2ei2π(0.3)),(x3,0.6ei2π(0.5),0.7ei2π(0.8)),(x4,1ei2π(0.5),0.7ei2π(0.6),0.9ei2π(0.2)), be two CHFSs. Then the operational laws are defined as

  1. Ec=0.1ei2π(0.7),0.3ei2π(0.4),0.7ei2π(0.6),0.2ei2π(0.5),0.5ei2π(0.4),0.4ei2π(0.2),0.3ei2π(0.5),0.1ei2π(0.9),0.7ei2π(0.4);

  2. EF=0.9ei2π(0.6),0.7ei2π(1),0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6),0.6ei2π(0.8),0.7ei2π(0.8),1ei2π(0.5),0.9ei2π(0.6),0.9ei2π(0.6); EF=0.8ei2π(0.3),0.1ei2π(0.6),0.2ei2π(0.3),0.6ei2π(0.5),0.7ei2π(0.5),0.7ei2π(0.1),0.3ei2π(0.2).

Theorem 1:

Let E,F and GCHFS(X) then the following holds

  1. c(c(E))=E

  2. i. EF=FEii. EF=FE

  3. i. (EF)G=E(FG)

    ii. (EF)G=E(FG)

  4. E(FG)=(EF)(EG)

  5. E(FG)=(EF)(EG)

Proof:

In this theorem we have E=(x,γEj(x).ei2π(ωγEj(x))), F=(x,γFj(x).ei2π(ωγFj(x))) and G=(x,γGj(x).ei2π(ωγGj(x)))

  1. By Definition 7 we have c(E)=c(x,γEj(x).ei2π(ωγEj(x)))=(x,1γEj(x).ei2π(1ωγEj(x))),thenc(c(E))=(x,1(1γEj(x)).ei2π(1(1ωγEj(x))))=(x,γEj(x).ei2π(ωγEj(x)))=E.

  2. By Definition 7 we have EF=(x,max(γEj(x),γFj(x)).ei2π(max(ωγEj(x),ωγFj(x))))=(x,max(γFj(x),γEj(x)).ei2π(max(ωγFj(x),ωγEj(x))))=FE. EF=(x,min(γEj(x),γFj(x)).ei2π(min(ωγEj(x),ωγFj(x))))=(x,min(γFj(x),γEj(x)).ei2π(min(ωγFj(x),ωγEj(x))))=FE

  3. i. By Definition 7 we have EF=(x,max(γEj(x),γFj(x)).ei2π(max(ωγEj(x),ωγFj(x))))

To prove that (EF)G=E(FG). As EF=(x,max(γEj(x),γFj(x)).ei2π(max(ωγEj(x),ωγFj(x)))) then(EF)G=(x,max(max(γEj(x),γFj(x)),γGj(x)).ei2π(max(max(ωγEj(x),ωγFj(x)),ωγGj(x))))=(x,max(γEj(x),max(γFj(x),γGj(x))).ei2π(max(ωγEj(x),max(ωγFj(x),ωγGj(x)))))=E(FG).   ii. By Definition 7 we have EF=(x,min(γEj(x),γFj(x)).ei2π(min(ωγEj(x),ωγFj(x)))) To prove that (EF)G=E(FG). As EF=(x,min(γEj(x),γFj(x)).ei2π(min(ωγEj(x),ωγFj(x)))) then(EF)G=(x,min(min(γEj(x),γFj(x)),γGj(x)).ei2π(min(min(ωγEj(x),ωγFj(x)),ωγGj(x))))=(x,min(γEj(x),min(γFj(x),γGj(x))).ei2π(min(ωγEj(x),min(ωγFj(x),ωγGj(x)))))=E(FG).

(4)

By definition 7 we have FG=(x,min(γFj(x),γGj(x)).ei2π(min(ωγFj(x),ωγGj(x))))

Then E(FG)=(x,max(γEj(x),min(γFj(x),γGj(x))).ei2π(max(ωγEj(x),min(ωγFj(x),ωγGj(x))))) Next we have EF=(x,max(γEj(x),γFj(x)).ei2π(max(ωγEj(x),ωγFj(x)))) and EG=(x,max(γEj(x),γGj(x)).ei2π(max(ωγEj(x),ωγGj(x)))) then (EF)(EG)=x,minmax(γEj(x),γFj(x)),max(γEj(x),γGj(x)).ei2πminmax(ωγEj(x),ωγFj(x)),max(ωγEj(x),ωγGj(x))=(x,max(γEj(x),min(γFj(x),γGj(x))).ei2π(max(ωγEj(x),min(ωγFj(x),ωγGj(x))))) Finally we obtain E(FG)=(EF)(EG).
(5)

By Definition 7 we have FG=(x,max(γFj(x),γGj(x)).ei2π(max(ωγFj(x),ωγGj(x))))

Then E(FG)=(x,min(γEj(x),max(γFj(x),γGj(x))).ei2π(min(ωγEj(x),max(ωγFj(x),ωγGj(x))))) Next we have EF=(x,min(γEj(x),γFj(x)).ei2π(min(ωγEj(x),ωγFj(x)))). and EG=(x,min(γEj(x),γGj(x)).ei2π(min(ωγej(x),ωγGj(x)))) then (EF)(EG)=x,maxmin(γEj(x),γFj(x)),min(γEj(x),γGj(x)).ei2πmaxmin(ωγEj(x),ωγFj(x)),min(ωγEj(x),ωγGj(x))=(x,min(γEj(x),max(γFj(x),γGj(x))).ei2π(min(ωγEj(x),max(ωγFj(x),ωγGj(x))))) Finally we obtain E(FG)=(EF)(EG).

Example 2:

Let E=(x1,0.9ei2π(0.3),0.7ei2π(0.6)),(x2,0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6)),(x3,0.6ei2π(0.8)),(x4,0.7ei2π(0.5),0.9ei2π(0.1),0.3ei2π(0.6)) F=(x1,0.8ei2π(0.6),0.1ei2π(1)),(x2,0.2ei2π(0.3)),(x3,0.6ei2π(0.5),0.7ei2π(0.8)),(x4,1ei2π(0.5),0.7ei2π(0.6),0.9ei2π(0.2)),and G=(x1,0.2ei2π(0.1),0.7ei2π(0.1)),(x2,0.3ei2π(0.9),1ei2π(0.4)),(x3,0.9ei2π(0.8),0.4ei2π(0.2)),(x4,0.7ei2π(0.6),0.8ei2π(0.3),0.9ei2π(1)) be CHFSs. Then

  1. c(E)=0.1ei2π(0.7),0.3ei2π(0.4),0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6),0.4ei2π(0.2),0.3ei2π(0.5),0.1ei2π(0.9),0.7ei2π(0.4);

  2. c(c(E))=0.9ei2π(0.3),0.7ei2π(0.6),0.7ei2π(0.6),0.2ei2π(0.5),0.5ei2π(0.4),0.6ei2π(0.8),0.7ei2π(0.5),0.9ei2π(0.1),0.3ei2π(0.6);

  3. i. EF=0.9ei2π(0.6),0.7ei2π(1),0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6),0.6ei2π(0.8),0.7ei2π(0.8),1ei2π(0.5),0.9ei2π(0.6),0.9ei2π(0.6)

and EF=0.9ei2π(0.6),0.7ei2π(1),0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6),0.6ei2π(0.8),0.7ei2π(0.8),1ei2π(0.5),0.9ei2π(0.6),0.9ei2π(0.6) this implies that EF=FE.

   ii. EF=0.8ei2π(0.3),0.1ei2π(0.6),0.2ei2π(0.3),0.6ei2π(0.5),0.7ei2π(0.5),0.7ei2π(0.1),0.3ei2π(0.2)

and FE=0.8ei2π(0.3),0.1ei2π(0.6),0.2ei2π(0.3),0.6ei2π(0.5),0.7ei2π(0.5),0.7ei2π(0.1),0.3ei2π(0.2) this implies that EF=FE.

(4)

i. We have (EF)G=0.9ei2π(0.6),0.7ei2π(1),0.3ei2π(0.9),1ei2π(0.5),0.5ei2π(0.6),0.9ei2π(0.8),0.7ei2π(0.8),1ei2π(0.6),0.9ei2π(0.6),0.9ei2π(1)

And FG=0.8ei2π(0.6),0.7ei2π(1),0.3ei2π(0.9),1ei2π(0.4),0.9ei2π(0.8),0.7ei2π(0.8),1ei2π(0.6),0.8ei2π(0.6),0.9ei2π(1) This implies that E(FG)=0.9ei2π(0.6),0.7ei2π(1),0.3ei2π(0.9),1ei2π(0.5),0.5ei2π(0.6),0.9ei2π(0.8),0.7ei2π(0.8),1ei2π(0.6),0.9ei2π(0.6),0.9ei2π(1) Finally we obtain (EF)G=E(FG).    ii. Next we have (EF)G=0.2ei2π(0.1),0.1ei2π(0.1),0.2ei2π(0.3),0.6ei2π(0.5),0.7ei2π(0.5),0.7ei2π(0.1),0.3ei2π(0.2) And FG=0.2ei2π(0.1),0.1ei2π(0.1),0.2ei2π(0.3),0.6ei2π(0.5),0.4ei2π(0.2),0.7ei2π(0.5),0.7ei2π(0.3),0.9ei2π(0.2) This implies that E(FG)=0.2ei2π(0.1),0.1ei2π(0.1),0.2ei2π(0.3),0.6ei2π(0.5),0.7ei2π(0.5),0.7ei2π(0.1),0.3ei2π(0.2) Finally we obtain (EF)G=E(FG).
(5)

We have FG=0.2ei2π(0.1),0.1ei2π(0.1),0.2ei2π(0.3),0.6ei2π(0.5),0.4ei2π(0.2),0.7ei2π(0.5),0.7ei2π(0.3),0.9ei2π(0.2)

Then E(FG)=(x1,0.9ei2π(0.3),0.7ei2π(0.6)),(x2,0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6)),(x3,0.6ei2π(0.8),0.4ei2π(0.2)),(x4,0.7ei2π(0.5),0.9ei2π(0.3),0.9ei2π(0.6)) Next we have EF=0.9ei2π(0.6),0.7ei2π(1),0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6),0.6ei2π(0.8),0.7ei2π(0.8),1ei2π(0.5),0.9ei2π(0.6),0.9ei2π(0.6) and EG=(x1,0.9ei2π(0.3),0.7ei2π(0.6)),(x2,0.3ei2π(0.9),1ei2π(0.5),0.5ei2π(0.6)),(x3,0.9ei2π(0.8),0.4ei2π(0.2)),(x4,0.7ei2π(0.6),0.9ei2π(0.3),0.9ei2π(1)) then (EF)(EG)=0.9ei2π(0.3),0.7ei2π(0.6),0.3ei2π(0.4),0.8ei2π(0.5),0.5ei2π(0.6),0.6ei2π(0.8),0.4ei2π(0.2),0.7ei2π(0.5),0.9ei2π(0.3),0.9ei2π(0.6) Finally we obtain E(FG)=(EF)(EG).
(6)

We have FG=0.8ei2π(0.6),0.7ei2π(1),0.3ei2π(0.9),1ei2π(0.4),0.9ei2π(0.8),0.7ei2π(0.8),1ei2π(0.6),0.8ei2π(0.6),0.9ei2π(1)

Then E(FG)=0.8ei2π(0.6),0.7ei2π(1),0.3ei2π(0.4),0.8ei2π(0.4),0.6ei2π(0.8),0.7ei2π(0.5),0.8ei2π(0.1),0.3ei2π(0.6) Next we have EF=0.8ei2π(0.3),0.1ei2π(0.6),0.2ei2π(0.3),0.6ei2π(0.5),0.7ei2π(0.5),0.7ei2π(0.1),0.3ei2π(0.2) and E then (EF)(EG)=0.8ei2π(0.6),0.7ei2π(1),0.3ei2π(0.4),0.8ei2π(0.4),0.6ei2π(0.8),0.7ei2π(0.5),0.8ei2π(0.1),0.3ei2π(0.6) Finally we obtain E(FG)=(EF)(EG).

4. The Generalized Similarity Measures Based on CHFSs

In the part of the paper, we proposed SMs established on the exponential function. We also proposed SMs without exponential function.

Definition 8:

Let E and F be two CHFSs on X. Then similarity measure (SM) between E and Fis identified by Sc(E,F), which satisfies the following properties

  1. 0Sc(E,F)1;

  2. Sc(E,F)=1if and only if E=F;

  3. Sc(E,F)=Sc(F,E).

Definition 9:

Let E and F be two CHFS on X. Then the exponential based generalized SM is calculated as Sc1(E,F)=1nk=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ11λ where λ>0, and described the maximum operation.

In Definitions (8) and (9), if we choose the imaginary parts will be zero, then the explored notion is converted for HFS. Similarly, if we choose the CHFS is a singleton set, then the CHFS is converted for CFS. Further, if we choose the CHFs is a singleton set and the imaginary part will be zero, then the CHFS is converted for FS. Due to its structure, it make powerful and proficient to cope with uncertain and unreliable information in real decision theory.

Theorem 2:

The SM Sc1(E,F) satisfy the following properties

  1. 0Sc1(E,F)1;

  2. Sc1(E,F)=1 if and only if E=F;

  3. Sc1(E,F)=Sc1(F,E).

Proof:

1. Since 1j=1|γEj(xk)γFj(xk)|λ[0,1] and 1j=1|ωγEj(xk)ωγFj(xk)|λ[0,1] then 1j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ[0,1] this implies that for k=1 we have 211j=1|γEj(x1)γFj(x1)|λ1j=1|ωγEj(x1)ωγFj(x1)|λ1[0,1] For k=2 211j=1|γEj(x2)γFj(x2)|λ1j=1|ωγEj(x2)ωγFj(x2)|λ1[0,1] By doing this process we obtain k=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1n[0,1]0k=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1n01nk=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1101nk=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ11λ10Sc1(E,F)1. 2. By Definition 7 we have Sc1(E,F)=1nk=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ11λSc1(E,F)=1nk=1n211((|γE1(xk)γF1(xk)|λ+|γE2(xk)γF2(xk)|λ++|γE(xk)γF(xk)|λ))1(|ωγE1(xk)ωγF1(xk)|λ+|ωγE2(xk)ωγF2(xk)|λ++|ωγE(xk)ωγF(xk)|λ)11λSc1(E,F)=1n211((|γE1(x1)γF1(x1)|λ+|γE2(x1)γF2(x1)|λ++|γE(x1)γF(x1)|λ))1(|ωγE1(x1)ωγF1(x1)|λ+|ωγE2(x1)ωγF2(x1)|λ++|ωγE(x1)ωγF(x1)|λ)1+211((|γE1(x2)γF1(x2)|λ+|γE2(x2)γF2(x2)|λ++|γE(x2)γF(x2)|λ))1(|ωγE1(x2)ωγF1(x2)|λ+|ωγE2(x2)ωγF2(x2)|λ++|ωγE(x2)ωγF(x2)|λ)1++211((|γE1(xn)γF1(xn)|λ+|γE2(xn)γF2(xn)|λ++|γE(xn)γF(xn)|λ))1(|ωγE1(xn)ωγF1(xn)|λ+|ωγE2(xn)ωγF2(xn)|λ++|ωγE(xn)ωγF(xn)|λ)11λ Now as E=F μE(xk)=μF(xk) for k=1,2,,n γEj(xk)ei2π(ωEj(xk))=γFj(xk)ei2π(ωFj(xk))for k=1,2,,nγEj(xk)=γFj(xk) and ei2π(ωEj(xk))=ei2π(ωFj(xk)) for k=1,2,,n. Then Sc1(E,F)=1n[2101+2101++2101]1λSc1(E,F)=1. 3. We have Sc1(E,F)=1nk=1n211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ11λ=1nk=1n211j=1|γF(xk)+γEj(xk)|λ1j=1|ωγFj(xk)+ωγEj(xk)|λ11λ=1nk=1n211j=1|(γF(xk)γEj(xk))|λ1j=1|(ωγFj(xk)ωγEj(xk))|λ11λ=1nk=1n211j=1|γF(xk)+γEj(xk)|λ1j=1|ωγFj(xk)+ωγEj(xk)|λ11λ=Sc1(F,E).

Remark 1:

If λ=1 then the exponential based generalized SM becomes Sc1(E,F)=1nk=1n211j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1

Definition 10:

Let E and F be two CHFS on X. Then we can also calculate exponential based generalized SM as follows Sc2(E,F)=1nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ11λ where λ>0.

Theorem 3:

The SM Sc2(E,F) satisfy the following properties

  1. 0Sc2(E,F)1;

  2. Sc2(E,F)=1 if and only if E=F;

  3. Sc2(E,F)=Sc2(F,E).

Proof:

1. Since 12j=1|γEj(xk)γFj(xk)|λ[0,1] and 12j=1|ωγEj(xk)ωγFj(xk)|λ[0,1] then 12j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ[0,1] this implies that for k=1 we have 2112j=1|γEj(x1)γFj(x1)|λ+12j=1|ωγEj(x1)ωγFj(x1)|λ1[0,1] For k=2 2112j=1|γEj(x2)γFj(x2)|λ+12j=1|ωγEj(x2)ωγFj(x2)|λ1[0,1] By doing this process we obtain k=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ1n[0,1]0k=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ1n01nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ1101nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ11λ101nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ11λ101nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ11λ10Sc2(E,F)1. 2. By definition 7 we have Sc2(E,F)=1nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ11λSc2(E,F)=1nk=1n2112((|γE1(xk)γF1(xk)|λ+|γE2(xk)γF2(xk)|λ++|γE(xk)γF(xk)|λ)+)12(|ωγE1(xk)ωγF1(xk)|λ+|ωγE2(xk)ωγF2(xk)|λ++|ωγE(xk)ωγF(xk)|λ)11λSc2(E,F)=1n2112((|γE1(x1)γF1(x1)|λ+|γE2(x1)γF2(x1)|λ++|γE2(x1)γF2(x1)|λ)+)12(|ωγE1(x1)ωγF1(x1)|λ+|ωγE2(x1)ωγF2(x1)|λ++|ωγE(x1)ωγF(x1)|λ)1+2112((|γE1(x2)γF1(x2)|λ+|γE2(x2)γF2(x2)|λ++|γE(x2)γF(x2)|λ)+)12(|ωγE1(x2)ωγF1(x2)|λ+|ωγE2(x2)ωγF2(x2)|λ++|ωγE(x2)ωγF(x2)|λ)1++2112((|γE1(xn)γF1(xn)|λ+|γE2(xn)γF2(xn)|λ++|γE(xn)γF(xn)|λ)+)12(|ωγE1(xn)ωγF1(xn)|λ+|ωγE2(xn)ωγF2(xn)|λ++|ωγE(xn)ωγF(xn)|λ)11λ Now as E=F μE(xk)=μF(xk) for k=1,2,,n γEj(xk)ei2π(ωEj(xk))=γFj(xk)ei2π(ωFj(xk))for k=1,2,,nγEj(xk)=γFj(xk) and ei2π(ωEj(xk))=ei2π(ωFj(xk)) for k=1,2,,n. Then Sc2(E,F)=1n[2101+2101++2101]1λSc1(E,F)=1. 3. We have Sc2(E,F)=1nk=1n2112j=1|γEj(xk)γFj(xk)|λ+12j=1|ωγEj(xk)ωγFj(xk)|λ11λ=1nk=1n2112j=1|γF(xk)+γEj(xk)|λ+12j=1|ωγFj(xk)+ωγEj(xk)|λ11λ=1nk=1n2112j=1|(γF(xk)γEj(xk))|λ+12j=1|(ωγFj(xk)ωγEj(xk))|λ11λ=1nk=1n2112j=1|γF(xk)+γEj(xk)|λ+12j=1|ωγFj(xk)+ωγEj(xk)|λ11λ=Sc2(F,E).

Remark 2:

If λ=1 then the exponential based generalized SM becomes Sc2(E,F)=1nk=1n2112j=1|γEj(xk)γFj(xk)|+12j=1|ωγEj(xk)ωγFj(xk)|1

Definition 11:

Let E and F be two CHFSs on X. Then without exponential based generalized SMs are calculated as follows Sc3(E,F)=1nk=1n11j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1+1j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1λSc4(E,F)=1nk=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1λSc5(E,F)=1nk=1n1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λ1/λ where λ>0 and αcc,βcc[0,1] such that αcc+βcc=1.

Theorem 4:

The SM Sc3(E,F) satisfies the following properties

  1. 0Sc3(E,F)1;

  2. Sc3(E,F)=1if and only if E=F;

  3. Sc3(E,F)=Sc3(F,E).

Proof:

1. Since 1j=1|γEj(xk)γFj(xk)|λ[0,1] and 1j=1|ωγEj(xk)ωγFj(xk)|λ[0,1] then 1j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ[0,1] and denominator will always greater than numerator, then for k=1 we have 11j=1|γEj(x1)γFj(x1)|1j=1|ωγEj(x1)ωγFj(x1)|1+1j=1|γEj(x1)γFj(x1)|1j=1|ωγEj(x1)ωγFj(x1)|[0,1] For k=2 11j=1|γEj(x2)γFj(x2)|1j=1|ωγEj(x2)ωγFj(x2)|1+1j=1|γEj(x2)γFj(x2)|1j=1|ωγEj(x2)ωγFj(x2)|[0,1] By doing this process we obtain k=1n11j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1+1j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|n[0,1]0k=1n11j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1+1j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|n01nk=1n11j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1+1j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|101nk=1n11j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1+1j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1λ1Sc3(E,F). 2. By definition 7 we have

Now as E=F μE(xk)=μF(xk) for k=1,2,,n γEj(xk)ei2π(ωEj(xk))=γFj(xk)ei2π(ωFj(xk))for k=1,2,,nγEj(xk)=γFj(xk) and ei2π(ωEj(xk))=ei2π(ωFj(xk)) for k=1,2,,n. Then Sc3(E,F)=1n[1+1++1]1λ Sc3(E,F)=1. 3. We have Sc3(E,F)=1nk=1n11j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1+1j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1λ =1nk=1n11j=1|(γFj(xk)γEj(xk))|λ1j=1|(ωγFj(xk)ωγEj(xk))|λ1+1j=1|(γFj(xk)γEj(xk))|λ1j=1|(ωγFj(xk)ωγEj(xk))|λ1λ =1nk=1n11j=1|(γFj(xk)γEj(xk))|λ1j=1|(ωγFj(xk)ωγEj(xk))|λ1+1j=1|(γFj(xk)γEj(xk))|λ1j=1|(ωγFj(xk)ωγEj(xk))|λ1λ=Sc3(F,E).

Theorem 5:

The SM Sc4(E,F) satisfy the following properties

  1. 0Sc4(E,F)1;

  2. Sc4(E,F)=1 if and only if E=F;

  3. Sc4(E,F)=Sc4(F,E).

Proof:

1. Since 1j=1(γEj(xk)γFj(xk))λ[0,1], 1j=1(ωγEj(xk)ωγFj(xk))λ[0,1], 1j=1(γEj(xk)γFj(xk))λ[0,1], 1j=1(ωγEj(xk)ωγFj(xk))λ[0,1] and denominator is always greater then nominator. Thus for k=1 we have 1j=1(γEj(x1)γFj(x1))λ+1j=1(ωγEj(x1)ωγFj(x1))λ1j=1(γEj(x1)γFj(x1))λ+1j=1(ωγEj(x1)ωγFj(x1))λ[0,1] For k=2 1j=1(γEj(x2)γFj(x2))λ+1j=1(ωγEj(x2)ωγFj(x2))λ1j=1(γEj(x2)γFj(x2))λ+1j=1(ωγEj(x2)ωγFj(x2))λ[0,1] By doing this process we obtain k=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λn[0,1]0k=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λn01nk=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ101nk=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1λ10Sc4(E,F)1. 2. By definition 7 we have

Now as E=F μE(xk)=μF(xk) for k=1,2,,n γEj(xk)ei2π(ωEj(xk))=γFj(xk)ei2π(ωFj(xk))for k=1,2,,nγEj(xk)=γFj(xk) and ei2π(ωEj(xk))=ei2π(ωFj(xk)) for k=1,2,,n. Then Sc4(E,F)=1n[1+1++1]1λSc4(E,F)=1.

3. We have Sc4(E,F)=1nk=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1λ=1nk=1n1j=1(γFj(xk)γEj(xk))λ+1j=1(ωγFj(xk)ωγEj(xk))λ1j=1(γFj(xk)γEj(xk))λ+1j=1(ωγFj(xk)ωγEj(xk))λ1λ=Sc4(F,E).

Theorem 6:

The SM Sc5(E,F) satisfy the following properties

  1. 0Sc5(E,F)1;

  2. Sc5(E,F)=1if and only if E=F;

  3. Sc5(E,F)=Sc5(F,E).

Proof:

1. Since (γEj(xk)γFj(xk))λ[0,1], (ωγEj(xk)ωγFj(xk))λ[0,1], (γEj(xk)γFj(xk))λ[0,1], (ωγEj(xk)ωγFj(xk))λ[0,1] this implies that αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ[0,1] and βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λ[0,1]. Thus for k=1 we have 1j=1αcc(γEj(x1)γFj(x1))λ(γEj(x1)γFj(x1))λ+βcc(ωγEj(x1)ωγFj(x1))λ(ωγEj(x1)ωγFj(x1))λ[0,1] For k=2 1j=1αcc(γEj(x2)γFj(x2))λ(γEj(x2)γFj(x2))λ+βcc(ωγEj(x2)ωγFj(x2))λ(ωγEj(x2)ωγFj(x2))λ[0,1] By doing this process we obtain k=1n1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λn[0,1]0k=1n1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λn01nk=1n1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λ101nk=1n1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λ1λ10Sc5(E,F)1.

2. By definition 7 we have

Now as E=F μE(xk)=μF(xk) for k=1,2,,n γEj(xk)ei2π(ωEj(xk))=γFj(xk)ei2π(ωFj(xk))for k=1,2,,nγEj(xk)=γFj(xk) and ei2π(ωEj(xk))=ei2π(ωFj(xk))for k=1,2,,n. and αcc,βcc[0,1] such that αcc+βcc=1. Then Sc5(E,F)=1. 3. We have Sc5(E,F)=1nk=1n1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λ1λ=1nk=1n1j=1αcc(γFj(xk)γEj(xk))λ(γFj(xk)γEj(xk))λ+βcc(ωγFj(xk)ωγEj(xk))λ(ωγFj(xk)ωγEj(xk))λ1λ=Sc5(F,E).

Remark 3:

If λ=1 then without exponential based generalized SMs become Sc3(E,F)=1nk=1n11j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1+1j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|Sc4(E,F)=1nk=1n1j=1(γEj(xk)γFj(xk))+1j=1(ωγEj(xk)ωγFj(xk))1j=1(γEj(xk)γFj(xk))+1j=1(ωγEj(xk)ωγFj(xk))Sc5(E,F)=1nk=1n1j=1αcc(γEj(xk)γFj(xk))(γEj(xk)γFj(xk))+βcc(ωγEj(xk)ωγFj(xk))(ωγEj(xk)ωγFj(xk)) Now we defined exponential based weighted generalized SMs and without exponential based weighted generalized SMs.

Definition 12:

Let E and F be two CHFS on X. Then the exponential based weighted generalized SM is calculated as Scw1(E,F)=k=1nwk211j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ11λ where λ>0, and described the maximum operation and wk[0,1] be the weight of each element xk for k=1,2,3,..,n such that k=1nwk=1.

Remark 4:

If λ=1 then the exponential based weighted generalized SM becomes Scw1(E,F)=k=1nwk211j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1

Definition 13:

Let E and F be two CHFS on X. Then we can also calculate the exponential based weighted generalized SM as follows Scw2(E,F)=k=1nwk211j=1|γEj(xk)γFj(xk)|λ+1j=1|ωγEj(xk)ωγFj(xk)|λ11λ where λ>0.

Remark 5:

If λ=1 then the exponential based weighted generalized SM becomes Scw2(E,F)=k=1nwk211j=1|γEj(xk)γFj(xk)|+1j=1|ωγEj(xk)ωγFj(xk)|1

Definition 14:

Let E and F be two CHFSs on X. Then without exponential based weighted generalized SMs are calculated as follows Scw3(E,F)=k=1nwk11j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1+1j=1|γEj(xk)γFj(xk)|λ1j=1|ωγEj(xk)ωγFj(xk)|λ1λScw4(E,F)=wkk=1n1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1j=1(γEj(xk)γFj(xk))λ+1j=1(ωγEj(xk)ωγFj(xk))λ1λScw5(E,F)=k=1nwk1j=1αcc(γEj(xk)γFj(xk))λ(γEj(xk)γFj(xk))λ+βcc(ωγEj(xk)ωγFj(xk))λ(ωγEj(xk)ωγFj(xk))λ1λ where λ>0 and αcc,βcc[0,1] such that αcc+βcc=1.

Remark 6:

If λ=1 then without exponential based weighted generalized SMs become Scw3(E,F)=k=1nwk11j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)|1+1j=1|γEj(xk)γFj(xk)|1j=1|ωγEj(xk)ωγFj(xk)| Scw4(E,F)=k=1nwk1j=1(γEj(xk)γFj(xk))+1j=1(ωγEj(xk)ωγFj(xk))1j=1(γEj(xk)γFj(xk))+1j=1(ωγEj(xk)ωγFj(xk)) Scw5(E,F)=k=1nwk1j=1αcc(γEj(xk)γFj(xk))(γEj(xk)γFj(xk))+βcc(ωγEj(xk)ωγFj(xk))(ωγEj(xk)ωγFj(xk))

5. Application

In this portion, the SMs and WSMs are applied to two cases which are pattern recognition and medical diagnosis. We evaluate the performance of the SMs in dealing with different practical world problems.

5.1. Pattern Recognition

Example 3:

Let X=x1,x2,x3,x4 be a set and four know patterns Ej(j=1,2,3,4) which are given in the form of CHFSs as follows E1=(x1,0.9ei2π(1),0.1ei2π(0.1)),(x2,0.4ei2π(0.6),0.7ei2π(0.3),0.5ei2π(0.2)),(x3,0.2ei2π(0.6)),(x4,0.3ei2π(0.8),0.2ei2π(0.7)) E2=(x1,0.3ei2π(0.5)),(x2,0.6ei2π(0.4),1ei2π(0.5)),(x3,0.2ei2π(0.8),0.2ei2π(0.7)),(x4,0.9ei2π(0.6),0.7ei2π(0.1)) E3=(x1,0.6ei2π(0.3)),(x2,0.2ei2π(0.1),0.4ei2π(0.2),0.3.ei2π(0.6)),(x3,0.8ei2π(0.1),1ei2π(0.2)),(x4,0.5ei2π(0.8),0.8ei2π(0.4),) E4=(x1,0.3ei2π(0.9),1ei2π(1),0.9ei2π(0.5)),(x2,0.4.ei2π(0.2),0.7ei2π(0.4)),(x3,0.1ei2π(1)),(x4,0.2ei2π(0.2),0.9ei2π(0.6))

Next let an unknown pattern which need to be identify E=(x1,0.3ei2π(0.1),0.9ei2π(0.5)),(x2,0.5ei2π(0.6),0.6ei2π(0.5)),(x3,0.4ei2π(0.9)),(x4,0.8ei2π(0.7),0.2ei2π(0.4),1ei2π(1)),

In we calculated the proposed SMs from E to Ej(j=1,2,3,4). The motive of this issue is to find that the unknown pattern E belong to which of the Pattern Ej(j=1,2,3,4). From the calculation stated in , we obtained the following consequences

  1. The similarity degree between E and E2 is a massive one as got by SMs, SMc1, SMc2, and SMc3. So by the principle of the maximum degree of similarity the SMs SMc1, SMc2 and SMc3 allot the unknown pattern E to the pattern E2.

  2. The similarity degree between E and E4 is a massive one as got by SMs, SMc4, and SMc5. So by the principle of the maximum degree of similarity the SMs SMc4 and SMc5 allot the unknown pattern E to the pattern E4.

Table 1. Calculation of proposed SMs for λ=1 and (αcc,βcc)=(0.5,0.5).

If we let the weight of each element xk(k=1,2,3,4) are 0.1,0.2,0.3 and 0.4 respectively. Then the calculation of proposed SMs are stated in . From the calculation stated in , we obtained the following consequences

  1. The similarity degree between E and E1 is a massive one as got by SMs, SMcw1, SMcw2, SMcw3 and SMcw5. So by the principle of the maximum degree of similarity the SMs SMcw1, SMcw2, SMcw3, and SMcw5 allot the unknown pattern E to the pattern E1.

  2. The similarity degree between E and E4 is a massive one as got by SM, SMcw5. So by the principle of the maximum degree of similarity the SM SMcw4 allot the unknown pattern E to the pattern E4.

Table 2. Calculation of proposed WSMs for Example (3) based on λ=1 and (αcc,βcc)=(0.5,0.5).

The ranking of the proposed SMs and WSMs are also stated in Tables 1 and 2 respectively. The graphical representation of the proposed SMs is shown in and proposed WSMs are shown in .

Figure 2. Graphical representation of established SMs for Example 3.

Figure 2. Graphical representation of established SMs for Example 3.

5.2. Medical Diagnosis

The symptoms of different diseases are different. The medical diagnosis depends on the victim’s symptoms which show what type of disease a victim has. The multiple symptoms of a victim represent a symptom set and a set of diseases can represent by different diseases.

Example 4:

Let a set of diagnoses D=D1(Coronovirous),D2(Pneumonia),D3(Flu),D4(Chestproblem) and a set of symptoms X={x1(shortofbreath),x2(Fever),x3(cough),x4(chestpain)}. The victim’s symptoms can be showed in the form of CHFSs as below P=(x1,0.9ei2π(1),0.5ei2π(1),0.5ei2π(0.5)),(x2,0.5ei2π(0.8),0.7ei2π(0.3),0.4ei2π(0.4)),(x3,0.2ei2π(0.6),0.8ei2π(0.9)),(x4,0.1ei2π(0.3)) The symptoms of each disease Dj(j=1,2,3,4) can be showed in CHFSs as below D1(coronovirous)=(x1,1ei2π(0.5),0.8ei2π(0.8)),(x2,0.5ei2π(0.7),0.6ei2π(0.9)),(x3,0.8ei2π(0.7),0.6ei2π(1),0.9ei2π(0.7)),(x4,0.1ei2π(0.1)), D2(Pneumonia)=(x1,0.1ei2π(0.2)),(x2,0.6ei2π(0.7),0.4ei2π(0.9)),(x3,0.4ei2π(0.6),0.5ei2π(0.6)),(x4,0.3ei2π(0.4),0.4ei2π(0.2)) D3(Flu)=(x1,0.1ei2π(0.0)),(x2,0.3ei2π(0.2),0.2ei2π(0.5)),(x3,1ei2π(0.8),0.6ei2π(0.7),0.9ei2π(0.6)),(x4,0.1ei2π(0.2),0.2ei2π(0.4)) D4(Chestpain)=(x1,0.2ei2π(0.1),0.3ei2π(0.2)),(x2,0.1.ei2π(0.2),0.0ei2π(0.2)),(x3,0.1ei2π(0.3)),(x4,1ei2π(0.9),0.9ei2π(0.7),0.5ei2π(0.6))

In we calculated the proposed SMs from P to Dj(j=1,2,3,4). The motive of this issue is to know about the disease of the victim that what disease a victim has in the above four diseases Dj(j=1,2,3,4). From the calculation stated in , we obtained that the similarity degree between P and D1 is a massive one as got by all SMs. So by the principle of the maximum degree of similarity, we can say that a victim has coronavirus.

Table 3. Calculation of proposed SMs for λ=1 and (αcc,βcc)=(0.5,0.5).

If we let the weight of each element xk(k=1,2,3,4) are 0.1,0.2,0.3 and 0.4 respectively. Then the calculation of proposed SMs are stated in . From the calculation stated in , we obtained the following consequences

  1. The similarity degree between P and D1 is a massive one as got by SMs, SMcw2, SMcw4, and SMcw5. So by the principle of the maximum degree of similarity the SMs SMcw2, SMcw4 and SMcw5 give us that a victim has coronavirus.

  2. The similarity degree between P and D2 is a massive one as got by SMs, SMcw1, and SMcw3. So by the principle of the maximum degree of similarity the SMs SMcw1, and SMcw3 provide that a victim has pneumonia.

Table 4. Calculation of proposed WSMs for Example (4) based on λ=1 and (αcc,βcc)=(0.5,0.5).

The ranking of the proposed SMs and WSMs are also stated in Tables and respectively. The graphical representation of the proposed SMs is shown in and proposed WSMs are shown in .

Figure 3. Graphical representation of established WSMs for Example 3.

Figure 3. Graphical representation of established WSMs for Example 3.

6. Comparison

Our goal to expand the new SMs is to deal with new kinds of data such as CHFSs and existing data CFSs, HFSs, and FSs. In this portion, we expressed the benefits of proposed SMs by comparing with existing SMs. The geometrical representations of the information's of example 4 and example 5, are discussed in Figures .

Figure 4. Graphical representation of established WSMs for Example 4.

Figure 4. Graphical representation of established WSMs for Example 4.

Figure 5. Graphical representation of established WSMs for Example 4.

Figure 5. Graphical representation of established WSMs for Example 4.

Figure 6. Graphical representation of the comparison of the establish SMs with existing SMs for Example 5.

Figure 6. Graphical representation of the comparison of the establish SMs with existing SMs for Example 5.

Figure 7. Graphical representation of the comparison of the establish SMs with existing SMs for Example 3.

Figure 7. Graphical representation of the comparison of the establish SMs with existing SMs for Example 3.

Example 5:

Let X=x1,x2,x3,x4 be a set and four know patterns Ej(j=1,2,3,4) which are given in the form of HFSs as follows E1=(x1,0.1,0.4,0.6),(x2,0.4,1),(x3,0.7,0.8),(x4,0.2), E2=(x1,0.3,0.5,0.8),(x2,0.4.,0.6),(x3,0.1,0.3),(x4,0.2,0.4,0.7) E3=(x1,0.6,0.8),(x2,0.1,0.2,0.6),(x3,0.7),(x4,0.4,0.5) E4=(x1,0.1,0.3),(x2,0.4,0.8),(x3,0.4,0.7,0.8),(x4,0.4),

Next let an unknown pattern which need to be identify E=(x1,0.2,0.3,0.6),(x2,0.8,1),(x3,0.5,0.8),(x4,1)

Now we have that e0=1 then the data given in the HFSs converted into the CHFSs as follows E1=(x1,0.1ei2π(0.0),0.4ei2π(0.0),0.6ei2π(0.0)),(x2,0.4ei2π(0.0),0.1ei2π(0.0)),(x3,0.7ei2π(0.0),0.8ei2π(0.0)),(x4,0.2.ei2π(0.0)) E2=(x1,0.3ei2π(0.0),0.5ei2π(0.0),0.8ei2π(0.0)),(x2,0.4ei2π(0.0),0.6.ei2π(0.0)),(x3,0.1ei2π(0.0),0.3ei2π(0.0)),(x4,0.2ei2π(0.0),0.4ei2π(0.0),0.7ei2π(0.0)) E3=(x1,0.6ei2π(0.0),0.8ei2π(0.0)),(x2,0.1ei2π(0.0),0.2ei2π(0.0),0.6ei2π(0.0)),(x3,0.7ei2π(0.0)),(x4,0.4ei2π(0.0),0.5ei2π(0.0)) E4=(x1,0.9.ei2π(0.0),1.ei2π(0.0),1.ei2π(0.0)),(x2,0.1.ei2π(0.0),0.3.ei2π(0.0)),(x3,0.4eiπ(0.0),0.7ei2π(0.0),0.8ei2π(0.0)),(x4,0.4ei2π(0.0))

And E=(x1,0.2ei2π(0.0),0.3ei2π(0.0),0.6ei2π(0.0)),(x2,0.8ei2π(0.0),1ei2π(0.0)),(x3,0.5ei2π(0.0),0.8ei2π(0.0)),(x4,1ei2π(0.0))

From we can observe that the data in the form of FSs and HFSs are solvable through existing SMs in the literature. The data in Example 5 is in the form HFSs which we can convert to CHFSs by taking 1=e0 and through proposed SMs we get the similarity between E and Ej(j=1,2,3,4) as shown in . But what about the data in the form of CFSs and CHFSs, these type of data are unsolvable through the existing SMs as shown in . The data in Example 3 are in the form of CHFSs so we can find the similarity between E and Ej(j=1,2,3,4) through proposed SMs. This means that our proposed SMs are the extension of the existing SMs. Through the proposed SMs we can find the similarity between FS, HFS, CFS, and CHFSs. The ranking of Example 5 is given in . The similarity degree between E and E1 is a massive one as got by all SMs in Example 5. The ranking of Example 3 given in is slightly different than ranking given in . The similarity degree between E and E2 is a massive one as got by SMs, SMc1, SMc2, and SMc3 and the similarity degree between E and E4 is a massive one as got by SMs, SMc4 and SMc5.

Table 5. Comparison between Proposed SMs and Existing SMs for Example (5) and λ=1, (αcc,βcc)=(1,0).

Table 6. Comparison between proposed SMs with existing SMs for Example (3) and λ=1.

7. Conclusion

SMs are utilized to inspect the variation between the two objects. The purpose of this article is to define the fundamental notion of CHFSs which is the combination of HFS and CFS and also defined their fundamental properties. We explored SMs for CHFSs. We presented exponential based generalized SMs and without exponential based generalized SMs for CHFSs. We obtained some valuable remarks. Further, the established SMs are used in Pattern recognition and medical diagnosis to inspect the practicability and credibility of the established SMs. Furthermore, we solved numerical examples for established SMs to show the supremacy and integrity of the proposed SMs. At last, to assess the trustworthiness of the established SMs we represented the comparison of the established SMs with some existing SMs. Our future work is to explore the application of CHFNs in many other type of researches [Citation34–48].

Disclosure statement

No potential conflict of interest was reported by the authors.

Additional information

Notes on contributors

Tahir Mahmood

Tahir Mahmood is Assistant Professor of Mathematics at Department of Mathematics and Statistics, International Islamic University Islamabad, Pakistan. He received his Ph.D. degree in Mathematics from Quaid-i-Azam University Islamabad, Pakistan in 2012 under the supervision of Professor Dr. Muhammad Shabir. His areas of interest are Algebraic structures, Fuzzy Algebraic structures and Soft sets. He has more than 65 international publications to his credit and he has also produced 38 MS students.

Ubaid ur Rehman

Ubaid ur Rehman, received the M.Sc. degrees in Mathematics from International Islamic University Islamabad, in 2018. Currently, He is a Student of MS in mathematics from International Islamic University Islamabad, Pakistan. His research interests include similarity measures, distance measures, fuzzy logic, fuzzy decision making, and their applications.

Zeeshan Ali

Zeeshan Ali, received the B.S. degrees in Mathematics from Abdul Wali Khan University Mardan, Pakistan, in 2016. He received has M.S. degrees in Mathematics from International Islamic University Islamabad, Pakistan, in 2018. Currently, He is a Student of Ph.D. in mathematics from International Islamic University Islamabad, Pakistan. His research interests include aggregation operators, fuzzy logic, fuzzy decision making, and their applications. He has published more than Thirteen articles.

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