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Article

NS-Cross Entropy-Based MAGDM under Single-Valued Neutrosophic Set Environment

1
Department of Mathematics, Nandalal Ghosh B.T. College, Panpur, P.O.-Narayanpur, District–North 24 Parganas, Bhatpara 743126, West Bengal, India
2
Department of Mathematics, Indian Institute of Engineering Science and Technology, Shibpur, P.O.-Botanic Garden, Howrah 711103, West Bengal, India
3
Department of Mathematics & Science, University of New Mexico, 705 Gurley Ave., Gallup, NM 87301, USA
*
Author to whom correspondence should be addressed.
Information 2018, 9(2), 37; https://doi.org/10.3390/info9020037
Submission received: 29 December 2017 / Revised: 3 February 2018 / Accepted: 6 February 2018 / Published: 9 February 2018
(This article belongs to the Special Issue Neutrosophic Information Theory and Applications)

Abstract

:
A single-valued neutrosophic set has king power to express uncertainty characterized by indeterminacy, inconsistency and incompleteness. Most of the existing single-valued neutrosophic cross entropy bears an asymmetrical behavior and produces an undefined phenomenon in some situations. In order to deal with these disadvantages, we propose a new cross entropy measure under a single-valued neutrosophic set (SVNS) environment, namely NS-cross entropy, and prove its basic properties. Also we define weighted NS-cross entropy measure and investigate its basic properties. We develop a novel multi-attribute group decision-making (MAGDM) strategy that is free from the drawback of asymmetrical behavior and undefined phenomena. It is capable of dealing with an unknown weight of attributes and an unknown weight of decision-makers. Finally, a numerical example of multi-attribute group decision-making problem of investment potential is solved to show the feasibility, validity and efficiency of the proposed decision-making strategy.

Graphical Abstract

1. Introduction

To tackle the uncertainty and modeling of real and scientific problems, Zadeh [1] first introduced the fuzzy set by defining membership measure in 1965. Bellman and Zadeh [2] contributed important research on fuzzy decision-making using max and min operators. Atanassov [3] established the intuitionistic fuzzy set (IFS) in 1986 by adding non-membership measure as an independent component to the fuzzy set. Theoretical and practical applications of IFSs in multi-criteria decision-making (MCDM) have been reported in the literature [4,5,6,7,8,9,10,11,12]. Zadeh [13] introduced entropy measure in the fuzzy environment. Burillo and Bustince [14] proposed distance measure between IFSs and offered an axiomatic definition of entropy measure. In the IFS environment, Szmidt and Kacprzyk [15] proposed a new entropy measure based on geometric interpretation of IFS. Wei et al. [16] developed an entropy measure for interval-valued intuitionistic fuzzy set (IVIFS) and presented its applications in pattern recognition and MCDM. Li [17] presented a new multi-attribute decision-making (MADM) strategy combining entropy and Technique for Order Preference by Similarity to Ideal Solution (TOPSIS) in an IVIFS environment. Shang and Jiang [18] introduced the cross entropy in the fuzzy environment. Vlachos and Sergiadis [19] presented intuitionistic fuzzy cross entropy by extending fuzzy cross entropy [18]. Ye [20] defined a new cross entropy under an IVIFS environment and presented an optimal decision-making strategy. Xia and Xu [21] put forward a new entropy and a cross entropy and employed them for multi-attribute criteria group decision-making (MAGDM) strategy under an IFS environment. Tong and Yu [22] defined cross entropy under an IVIFS environment and applied it to MADM problems.
The study of uncertainty took a new direction after the publication of the neutrosophic set (NS) [23] and single-valued neutrosophic set (SVNS) [24]. SVNS appeals more to researchers for its applicability in decision-making [25,26,27,28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54], conflict resolution [55], educational problems [56,57], image processing [58,59,60], cluster analysis [61,62], social problems [63,64], etc. The research on SVNS gained momentum after the inception of the international journal “Neutrosophic Sets and Systems”. Combining with the neutrosophic set, a number of hybrid neutrosophic sets such as the neutrosophic soft set [65,66,67,68,69,70,71,72], the neutrosophic soft expert set [73,74,75], the neutrosophic complex set [76], the rough neutrosophic set [77,78,79,80,81,82,83,84,85,86], the rough neutrosophic tri complex set [87], the neutrosophic rough hyper complex set [88], the neutrosophic hesitant fuzzy sets/multi-valued neutrosophic set [89,90,91,92,93,94,95,96,97], the bipolar neutrosophic set [98,99,100,101,102,103], the rough bipolar neutrosophic set [104], the neutrosophic cubic set [105,106,107,108,109,110,111,112,113], and the neutrosophic cubic soft set [114,115] has been reported in the literature. Wang et al. [116] defined the interval neutrosophic set (INS). Different interval neutrosophic hybrid sets and their theoretical development and applications have been reported in the literature, such as the interval-valued neutrosophic soft set [117], the interval neutrosophic complex set [118], the interval neutrosophic rough set [119,120,121], and the interval neutrosophic hesitant fuzzy set [122]. Other extensions of neutrosophic sets, such as trapezoidal neutrosophic sets [123,124], normal neutrosophic sets [125], single-valued neutrosophic linguistic sets [126], interval neutrosophic linguistic sets [127,128], simplified neutrosophic linguistic sets [129], single-valued neutrosophic trapezoid linguistic sets [130], interval neutrosophic uncertain linguistic sets [131,132,133], neutrosophic refined sets [134,135,136,137,138,139], linguistic refined neutrosophic sets [140] bipolar neutrosophic refined sets [141], and dynamic single-valued neutrosophic multi-sets [142] have been proposed to enrich the study of neutrosophics. So the field of neutrosophic study has been steadily developing.
Majumdar and Samanta [143] defined an entropy measure and presented an MCDM strategy under SVNS environment. Ye [144] proposed cross entropy measure under the single-valued neutrosophic set environment, which is not symmetric straight forward and bears undefined phenomena. To overcome the asymmetrical behavior of the cross entropy measure, Ye [144] used a symmetric discrimination information measure for single-valued neutrosophic sets. Ye [145] defined cross entropy measures for SVNSs to overcome the drawback of undefined phenomena of the cross entropy measure [144] and proposed a MCDM strategy.
The aforementioned applications of cross entropy [144,145] can be effective in dealing with neutrosophic MADM problems. However, they also bear some limitations, which are outlined below:
i.
The strategies [144,145] are capable of solving neutrosophic MADM problems that require the criterion weights to be completely known. However, it can be difficult and subjective to offer exact criterion weight information due to neutrosophic nature of decision-making situations.
ii.
The strategies [144,145] have a single decision-making structure, and not enough attention is paid to improving robustness when processing the assessment information.
iii.
The strategies [144,145] cannot deal with the unknown weight of the decision-makers.
Research gap:
MAGDM strategy based on cross entropy measure with unknown weight of attributes and unknown weight of decision-makers.
This study answers the following research questions:
i.
Is it possible to define a new cross entropy measure that is free from asymmetrical phenomena and undefined behavior?
ii.
Is it possible to define a new weighted cross entropy measure that is free from the asymmetrical phenomena and undefined behavior?
iii.
Is it possible to develop a new MAGDM strategy based on the proposed cross entropy measure in single-valued neutrosophic set environment, which is free from the asymmetrical phenomena and undefined behavior?
iv.
Is it possible to develop a new MAGDM strategy based on the proposed weighted cross entropy measure in the single-valued neutrosophic set environment that is free from the asymmetrical phenomena and undefined behavior?
v.
How do we assign unknown weight of attributes?
vi.
How do we assign unknown weight of decision-makers?
Motivation:
The above-mentioned analysis describes the motivation behind proposing a comprehensive NS-cross entropy-based strategy for tackling MAGDM under the neutrosophic environment. This study develops a novel NS-cross entropy-based MAGDM strategy that can deal with multiple decision-makers and unknown weight of attributes and unknown weight of decision-makers and free from the drawbacks that exist in [144,145].
The objectives of the paper are:
  • To define a new cross entropy measure and prove its basic properties, which are free from asymmetrical phenomena and undefined behavior.
  • To define a new weighted cross measure and prove its basic properties, which are free from asymmetrical phenomena and undefined behavior.
  • To develop a new MAGDM strategy based on weighted cross entropy measure under single-valued neutrosophic set environment.
  • To develop a technique to incorporate unknown weight of attributes and unknown weight of decision-makers in the proposed NS-cross entropy-based MAGDM under single-valued neutrosophic environment.
To fill the research gap, we propose NS-cross entropy-based MAGDM, which is capable of dealing with multiple decision-makers with unknown weight of the decision-makers and unknown weight of the attributes.
The main contributions of this paper are summarized below:
  • We define a new NS-cross entropy measure and prove its basic properties. It is straightforward symmetric and it has no undefined behavior.
  • We define a new weighted NS-cross entropy measure in the single-valued neutrosophic set environment and prove its basic properties. It is straightforward symmetric and it has no undefined behavior.
  • In this paper, we develop a new MAGDM strategy based on weighted NS cross entropy to solve MAGDM problems with unknown weight of the attributes and unknown weight of decision-makers.
  • Techniques to determine unknown weight of attributes and unknown weight of decisions makers are proposed in the study.
The rest of the paper is presented as follows: Section 2 describes some concepts of SVNS. In Section 3 we propose a new cross entropy measure between two SVNS and investigate its properties. In Section 4, we develop a novel MAGDM strategy based on the proposed NS-cross entropy with SVNS information. In Section 5 an illustrative example is solved to demonstrate the applicability and efficiency of the developed MAGDM strategy under SVNS environment. In Section 6 we present comparative study and discussion. Section 7 offers conclusions and the future scope of research.

2. Preliminaries

This section presents a short list of mostly known definitions pertaining to this paper.
Definition 1 [23] NS.
Let U be a space of points (objects) with a generic element in U denoted by u, i.e., u U. A neutrosophic set A in U is characterized by truth-membership measure T A ( u ) , indeterminacy-membership measure I A ( u ) and falsity-membership measure F A ( u ) , where T A ( u ) , I A ( u ) , F A ( u ) are the measures from U to ] 0, 1+ [i.e., T A ( u ) , I A ( u ) , F A ( u ) :U ] 0, 1+[ NS can be expressed as A = {<u; ( T A ( u ) , I A ( u ) , F A ( u ) )>: u U}. Since T A ( u ) , I A ( u ) , F A ( u ) are the subsets of ]0, 1+ [there the sum ( T A ( u ) + I A ( u ) + F A ( u ) ) lies between 0 and 3+.
Example 1.
Suppose that U = { u 1 ,   u 2 ,   u 3 ,   } be the universal set. Let R 1 be any neutrosophic set in U. Then R 1 expressed as R 1 = {< u 1 ; (0.6, 0.3, 0.4)>: u 1 U}.
Definition 2 [24] SVNS.
Assume that U be a space of points (objects) with generic elements u ∈ U. A SVNS H in U is characterized by a truth-membership measure TH(u), an indeterminacy-membership measure IH(u), and a falsity-membership measure FH(u), where TH(u), IH(u), FH(u) ∈ [0, 1] for each point u in U. Therefore, a SVNS A can be expressed as H = {u, (TH (u), I H (u), FH (u)) | u ∈ U}, whereas, the sum of TH(u), IH(u) and FH(u) satisfy the condition 0 ≤ TH(u) + IH(u) + FH(u) ≤ 3 and H(u) = <(TH (u), IH (u), FH (u)> call a single-valued neutrosophic number (SVNN).
Example 2.
Suppose that U = { u 1 ,   u 2 ,   u 3 ,   } be the universal set. A SVNS H in U can be expressed as: H = { u 1 , (0.7, 0.3, 0.5)| u 1 ∈ U} and SVNN presented H = <0.7, 0.3, 0.5>.
Definition 3 [24] Inclusion of SVNSs.
The inclusion of any two SVNS sets H1 and H2 in U is denoted by H1 ⊆ H2 and defined as follows:
H 1 H 2 ,   T H 1 ( u )     T H 2 ( u ) ,   I H 1 ( u ) I H 2 ( u ) ,   F H 1 ( u ) F H 2 ( u )   i f f   f o r   a l l   u U .
Example 3.
Let H1 and H2 be any two SVNNs in U presented as follows: H1 = <(0.7, 0.3, 0.5)> and H2 = <(0.8, 0.2, 0.4)> for all u ∈ U. Using the property of inclusion of two SVNNs, we conclude that H1 ⊆ H2.
Definition 4 [24] Equality of two SVNSs.
The equality of any two SVNS H1 and H2 in U denoted by H1 = H2 and defined as follows:
T H 1 ( u ) = T H 2 ( u ) ,   I H 1 ( u ) = I H 2 ( u )   a n d   F H 1 ( u ) = F H 2 ( u )   f o r   a l l   u U .
Definition 5 Complement of any SVNSs.
The complement of any SVNS H in U denoted by H c and defined as follows:
H c   =   { u ,   1 T H , 1 I H ,   1 F H   |   u U } .
Example 4.
Let H be any SVNN in U presented as follows: H = < (0.7, 0.3, 0.5) >. Then compliment of H is obtained as H c = <(0.3, 0.7, 0.5)>.
Definition 6 [24] Union.
The union of two single-valued neutrosophic sets H1 and H2 is a neutrosophic set H3 (say) written as
H3 = H1 H2.
T H 3 ( u ) = max { T H 1 ( u ) , T H 2 ( u ) }, I H J 3 ( u ) = min { I H 1 ( u ) , I H 2 ( u ) }, F H 3 (u) = min { F H 1 ( u ) , F H 2 ( u ) }, u U.
Example 5.
Let H1 and H2 be two SVNSs in U presented as follows:
H1 = <(0.6, 0.3, 0.4)> and H2 = <(0.7, 0.3, 0.6)>. Then union of them is presented as:
H 1 H 2 = < ( 0.7 , 0.3 , 0.4 ) > .
Definition 7 [24] Intersection.
The intersection of two single-valued neutrosophic sets H1 and H2 denoted by H4 and defined as
H4 = H1 H2
T H 4 (u) = min { T H 1 ( u ) , T H 2 ( u ) }, I H 4 ( u ) = max{ I H 1 ( u ) , I H 2 ( u ) }
F H 4 ( u ) = max { F H 1 ( u ) , F H 2 ( u ) }, u U.
Example 6.
Let H1 and H2 be two SVNSs in U presented as follows:
H1 = <(0.6, 0.3, 0.4)> and H2 = <(0.7, 0.3, 0.6)>.
Then intersection of H1 and H2 is presented as follows:
H1H2 = <(0.6, 0.3, 0.6)>

3. NS-Cross Entropy Measure

In this section, we define a new single-valued neutrosophic cross-entropy measure for measuring the deviation of single-valued neutrosophic variables from an a priori one.
Definition 8 NS-cross entropy measure.
Let H1 and H2 be any two SVNSs in U = { u 1 ,   u 2 ,   u 3 ,   ,   u n } . Then, the single-valued cross-entropy of H1 and H2 is denoted by CENS (H1, H2) and defined as follows:
CE NS   ( H 1 ,   H 2 ) = 1 2 { i   =   1 n [ 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2 | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ] + [ 2 | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 + 2 | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] + [ 2 | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2 | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] }
Example 7.
Let H1 and H2 be two SVNSs in U, which are given by H1 = {u, (0.7, 0.3, 0.4)| u ∈ U} and H2 = {u, (0.6, 0.4, 0.2)| u ∈ U}. Using Equation (1), the cross entropy value of H1 and H2 is obtained as CE NS ( H 1 ,   H 2 ) = 0.707.
Theorem 1.
Single-valued neutrosophic cross entropy CE NS ( H 1 ,   H 2 ) for any two SVNSs H 1 ,   H 2 , satisfies the following properties:
i.
CE NS ( H 1 ,   H 2 ) 0 .
ii.
CE NS ( H 1 ,   H 2 )   = 0 if and only if T H 1 ( u i ) = T H 2 ( u i ) , I H 1 ( u i ) = I H 2 ( u i ) , F H 1 ( u i ) = F H 2 ( u i ) ,     u i U .
iii.
CE NS ( H 1 ,   H 2 ) = CE NS   ( H 1 c ,   H 2 c )
iv.
CE NS   ( H 1 ,   H 2 ) = CE NS   ( H 2 ,   H 1 )
Proof. 
(i) For all values of u i U , | T H 1 ( u i ) | 0 , | T H 2 ( u i ) | 0 , | T H 1 ( u i ) T H 2 ( u i ) | 0 , 1 + | T H 1 ( u i ) | 2 0 , 1 + | T H 2 ( u i ) | 2 0 , | ( 1 T H 1 ( u i ) ) | 0 , | ( 1 T H 2 ( u i ) ) | 0 , | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 0 , 1 + | ( 1 T H 1 ( u i ) ) | 2 0 , 1 + | ( 1 T H 2 ( u i ) ) | 2 0 .
Then, [ 2 | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2 | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ] 0 .
Similarly, [ 2 | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 + 2 | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] 0 , and [ 2 | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2   | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] 0 .
Therefore, CE NS   ( H 1 ,   H 2 ) 0 .
Hence complete the proof.
(ii) [ 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ] = 0 ,   T H 1 ( u i ) = T H 2 ( u i ) , [ 2   | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u )   | 2 + 2   | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] = 0 I H 1 ( u i ) = I H 2 ( u i ) , and, [ 2   | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2   | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] = 0 , F H 1 ( u i ) = F H 2 ( u i )
Therefore, CE NS ( H 1 ,   H 2 )   = 0 , iff T H 1 ( u i ) = T H 2 ( u i ) , I H 1 ( u i ) = I H 2 ( u i ) , F H 1 ( u i ) = F H 2 ( u i ) ,   u i U .
Hence complete the proof.
(iii) Using Definition 5, we obtain the following expression
CE NS   ( H 1 c ,   H 2 c ) = 1 2 { i   = 1 n [ 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 + 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 ] + [ 2 | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 + 2 | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 ] + [ 2 | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 + 2 | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 ] } = 1 2 { i = 1 n [ 2 | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2 | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ] + [ 2 | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 + 2 | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] + [ 2 | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2 | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] } = CE SN ( H 1 ,   H 2 )
Therefore, CE NS ( H 1 ,   H 2 ) = CE NS ( H 1 c ,   H 2 c ) .
Hence complete the proof.
(iv) Since, | T H 1 ( u i ) T H 2 ( u i ) | = | T H 2 ( u i ) T H 1 ( u i ) | , | I H 1 ( u i ) I H 2 ( u i ) | = | I H 2 ( u i ) I H 1 ( u i ) | , | F H 1 ( u i ) F H 2 ( u i ) | = | F H 2 ( u i ) F H 1 ( u i ) | , | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | = | ( 1 T H 2 ( u i ) ) (   1 T H 1 ( u i ) ) | , | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | = | ( 1 I H 2 ( u i ) ) ( 1 I H 1 ( u i ) ) | , | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | = | ( 1 F H 2 ( u i ) ) ( 1 F H 1 ( u i ) ) | , then, 1 + | T H 1 ( u i ) | 2   +   1 + | T H 2 ( u i ) | 2 = 1 + | T H 2 ( u i ) | 2   + 1 + | T H 1 ( u i ) | 2 , 1 + | I H 1 ( u i ) | 2   +   1 + | I H 2 ( u i ) | 2 = 1 + | I H 2 ( u i ) | 2   + 1 + | I H 1 ( u i ) | 2 , 1 + | F H 1 ( u i ) | 2   +   1 + | F H 2 ( u i ) | 2 = 1 + | F H 2 ( u i ) | 2   + 1 + | F H 1 ( u i ) | 2 , 1 + | ( 1 T H 1 ( u i ) ) | 2   +   1 + | ( 1 T H 2 ( u i ) ) | 2 = 1 + | ( T H 2 ( u i )   ) | 2   + 1 + | ( 1 T H 1 ( u i ) ) | 2 , 1 + | ( 1 I H 1 ( u i ) ) | 2   +   1 + | ( 1 I H 2 ( u i ) ) | 2 = 1 + | ( 1 I H 2 ( u i ) ) | 2   + 1 + | ( 1 I H 1 ( u i ) ) | 2 , 1 + | ( 1 F H 1 ( u i ) ) | 2   +   1 + | ( 1 F H 2 ( u i ) ) | 2 = 1 + | ( 1 F H 2 ( u i ) ) | 2   + 1 + | ( 1 F H 1 ( u i ) ) | 2 ,   u i U .
Therefore, CE NS ( H 1 ,   H 2 ) = CE NS   ( H 2 ,   H 1 ) .
Hence complete the proof. ☐
Definition 9 Weighted NS-cross entropy measure.
We consider the weight wi (i = 1, 2, ..., n) for the element ui (i = 1, 2, .., n) with the conditions w i     [ 0 ,   1 ]   a n d   i = 1 n w i =   1 .
Then the weighted cross entropy between SVNSs H1 and H2 can be defined as follows:
CE NS w   ( H 1 ,   H 2 ) = 1 2 i   =   1 n w i { [ 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ]   + [ 2   | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i )   | 2 + 1 + | I H 2 ( u ) | 2 + 2   | ( 1 I H 1 ( u i ) )   ( 1 I H 2 ( u i ) ) | 1 + | ( 1   I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] + [ 2   | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2   | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] }
Theorem 2.
Single-valued neutrosophic weighted NS-cross-entropy (defined in Equation (2)) satisfies the following properties:
i.
CE NS w   ( H 1 ,   H 2 ) 0 .
ii.
CE NS w   ( H 1 ,   H 2 ) = 0 , if and only if T H 1 ( u i ) = T H 2 ( u i )   I H 1 ( u i ) = I H 2 ( u i ) , F H 1 ( u i ) = F H 2 ( u i ) ,   u i U .
iii.
CE NS w   ( H 1 ,   H 2 ) = CE NS w   ( H 1 c ,   H 2 c )
iv.
CE NS w   ( H 1 ,   H 2 ) =   CE NS w   (   H 2 ,   H 1 )
Proof. 
(i). For all values of   u i U , | T H 1 ( u i )   | 0   | T H 2 ( u i )   | 0 , | T H 1 ( u i ) T H 2 ( u i ) | 0 , 1 + | T H 1 ( u i ) | 2   0 , 1 + | T H 2 ( u i ) | 2   0 , | ( 1 T H 1 ( u i ) ) | 0 , | ( 1 T H 2 ( u i ) )   | 0 , | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 0 , 1 + | ( 1 T H 1 ( u i ) ) | 2   0 , 1 + | ( 1   T H 2 ( u i ) )   | 2   0 , then, [ 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ] 0 .
Similarly, [ 2   | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 + 2   | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] 0 , and [ 2   | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2   | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] 0 .
Since w i   [ 0 ,   1 ]   and   i = 1 n w i =   1 , therefore, CE NS w   ( H 1 ,   H 2 ) 0 .
Hence complete the proof.
(ii) Since, [ 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ] = 0 ,     T H 1 ( u i ) = T H 2 ( u i ) , [ 2   | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i )   | 2 + 1 + | I H 2 ( u )   | 2 + 2   | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] = 0 , I H 1 ( u i ) = I H 2 ( u i ) , [ 2   | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2   | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] = 0 ,   F H 1 ( u i ) = F H 2 ( u i ) and w i   [ 0 ,   1 ]   ,   i = 1 n w i =   1 , w i 0 . Therefore, CE NS w   ( H 1 ,   H 2 ) = 0 iff T H 1 ( u i ) = T H 2 ( u i ) , I H 1 ( u i ) = I H 2 ( u i ) , F H 1 ( u i ) = F H 2 ( u i ) ,   u i U .
Hence complete the proof.
(iii) Using Definition 5, we obtain the following expression
CE NS w   ( H 1 c ,   H 2 c ) = 1 2 { i   = 1 n w i [ 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 + 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 ]   + [ 2   | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 + 2   | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 ] + [ 2   | ( 1 F H 1 ( u i ) )   ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 + 2   | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 ] } =   1 2 { i   = 1 n w i [ 2   | T H 1 ( u i ) T H 2 ( u i ) | 1 + | T H 1 ( u i ) | 2 + 1 + | T H 2 ( u i ) | 2 + 2   | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | 1 + | ( 1 T H 1 ( u i ) ) | 2 + 1 + | ( 1 T H 2 ( u i ) ) | 2 ]   + [ 2   | I H 1 ( u i ) I H 2 ( u i ) | 1 + | I H 1 ( u i ) | 2 + 1 + | I H 2 ( u ) | 2 + 2   | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | 1 + | ( 1 I H 1 ( u i ) ) | 2 + 1 + | ( 1 I H 2 ( u i ) ) | 2 ] + [ 2   | F H 1 ( u i ) F H 2 ( u i ) | 1 + | F H 1 ( u i ) | 2 + 1 + | F H 2 ( u i ) | 2 + 2   | ( 1 F H 1 ( u i ) )   ( 1 F H 2 ( u i ) ) | 1 + | ( 1 F H 1 ( u i ) ) | 2 + 1 + | ( 1 F H 2 ( u i ) ) | 2 ] } = CE NS w   ( H 1 ,   H 2 )
Therefore, CE NS w   ( H 1 ,   H 2 ) = CE NS w   ( H 1 c ,   H 2 c ) .
Hence complete the proof.
(iv) Since | T H 1 ( u i ) T H 2 ( u i ) | = | T H 2 ( u i ) T H 1 ( u i ) | , | I H 1 ( u i ) I H 2 ( u i ) | = | I H 2 ( u i ) I H 1 ( u i ) | , | F H 1 ( u i ) F H 2 ( u i ) | = | F H 2 ( u i ) F H 1 ( u i ) | , | ( 1 T H 1 ( u i ) ) ( 1 T H 2 ( u i ) ) | = | ( 1 T H 2 ( u i ) ) ( 1 T H 1 ( u i ) ) | , | ( 1 I H 1 ( u i ) ) ( 1 I H 2 ( u i ) ) | = | ( 1 I H 2 ( u i ) ) ( 1 I H 1 ( u i ) ) | , | ( 1 F H 1 ( u i ) ) ( 1 F H 2 ( u i ) ) | = | ( 1 F H 2 ( u i ) ) ( 1 F H 1 ( u i ) ) | , we obtain 1 + | T H 1 ( u i ) | 2   +   1 + | T H 2 ( u i ) | 2 = 1 + | T H 2 ( u i ) | 2   + 1 + | T H 1 ( u i ) | 2 , 1 + | I H 1 ( u i ) | 2   +   1 + | I H 2 ( u i ) | 2 = 1 + | I H 2 ( u i ) | 2   + 1 + | I H 1 ( u i ) | 2 , 1 + | F H 1 ( u i ) | 2   +   1 + | F H 2 ( u i ) | 2 = 1 + | F H 2 ( u i ) | 2   + 1 + | F H 1 ( u i ) | 2 , 1 + | ( 1 T H 1 ( u i ) ) | 2   +   1 + | ( 1 T H 2 ( u i ) ) | 2 = 1 + | ( T H 2 ( u i )   ) | 2   + 1 + | ( 1 T H 1 ( u i ) ) | 2 , 1 + | ( 1 I H 1 ( u i ) ) | 2   +   1 + | ( 1 I H 2 ( u i ) ) | 2 = 1 + | ( 1 I H 2 ( u i ) ) | 2   + 1 + | ( 1 I H 1 ( u i ) ) | 2 , 1 + | ( 1 F H 1 ( u i ) ) | 2   +   1 + | ( 1 F H 2 ( u i ) ) | 2 = 1 + | ( 1 F H 2 ( u i ) ) | 2   + 1 + | ( 1 F H 1 ( u i ) ) | 2 ,   u i U and w i   [ 0 ,   1 ]   ,   i = 1 n w i =   1 .
Therefore, CE NS w   ( H 1 ,   H 2 ) = CE NS w   ( H 2 ,   H 1 ) .
Hence complete the proof. ☐

4. MAGDM Strategy Using Proposed Ns-Cross Entropy Measure under SVNS Environment

In this section, we develop a new MAGDM strategy using the proposed NS-cross entropy measure.
Description of the MAGDM Problem
Assume that A =   { A 1 ,   A 2 ,   A 3 ,   ,   A m } and G =   { G 1 ,   G 2 ,   G 3 ,   ,   G n } be the discrete set of alternatives and attributes respectively and W =   { w 1 ,   w 2 ,   w 3 ,   ,   w n } be the weight vector of attributes G j (j = 1, 2, 3, …, n), where w j   0 and j = 1 n w j =   1 . Assume that E =   { E 1 ,   E 2 ,   E 3 ,   ,   E ρ } be the set of decision-makers who are employed to evaluate the alternatives. The weight vector of the decision-makers E k   ( k = 1 , 2 , 3 , , ρ ) is λ =   { λ 1 ,   λ 2 ,   λ 3 ,   ,   λ ρ } (where, λ k 0   and   k = 1 ρ λ k = 1 ), which can be determined according to the decision-makers’ expertise, judgment quality and domain knowledge.
Now, we describe the steps of the proposed MAGDM strategy (see Figure 1) using NS-cross entropy measure.
MAGDM Strategy Using Ns-Cross Entropy Measure
Step 1. Formulate the decision matrices
For MAGDM with SVNSs information, the rating values of the alternatives A i   ( i = 1 ,   2 ,   3 ,   ,   m ) based on the attribute G j   (   j = 1 ,   2 ,   3 ,   ,   n ) provided by the k-th decision-maker can be expressed in terms of SVNN as a i j k = < T i j k ,   I i j k ,   F i j k > (i = 1, 2, 3, …, m; j = 1, 2, 3, …, n; k = 1, 2, 3, …, ρ). We present these rating values of alternatives provided by the decision-makers in matrix form as follows:
M k = ( G 1 G 2 . G n A 1 a 11 k a 12 k a 1 n k A 2 a 21 k a 2 n k a 22 k . . . A m a m 1 k a m 2 k a mn k )
Step 2. Formulate priori/ideal decision matrix
In the MAGDM, the a priori decision matrix has been used to select the best alternatives among the set of collected feasible alternatives. In the decision-making situation, we use the following decision matrix as a priori decision matrix.
P = ( G 1 G 2 . G n A 1 a 11 * a 12 * a 1 n * A 2 a 21 * a 22 * a 2 n * . . . A m a m 1 * a m 2 * a mn * )
where, a ij * = < max i   ( T i j k ) ,   min i   ( I i j k ) , min i   ( F i j k ) > ) corresponding to benefit attributes and a ij * = < min i   ( T i j k ) ,   max i   ( I i j k ) , max i   ( F i j k ) > corresponding to cost attributes, and (i = 1, 2, 3, …, m; j = 1, 2, 3, …, n; k = 1, 2, 3, …, ρ).
Step 3. Determinate the weights of decision-makers
To find the decision-makers’ weights we introduce a model based on the NS-cross entropy measure. The collective NS-cross entropy measure between M k and P (Ideal matrix) is defined as follows:
C E N S c ( M k ,   P ) = 1 m i = 1 m C E N S ( M k ( A i ) ,   P ( A i ) )
where, C E N S ( M k ( A i ) ,   P ( A i ) ) = j = 1 n C E N S ( M k ( A i ( G j ) ) ,   P ( A i ( G j ) ) ) .
Thus, we can introduce the following weight model of the decision-makers:
λ K = ( 1 ÷   C E N S c ( M k ,   P ) ) k = 1 ρ ( 1 ÷   C E N S c ( M k ,   P ) )
where, 0 λ K 1 and k = 1 ρ λ K = 1 for k = 1, 2, 3, …, ρ.
Step 4. Formulate the weighted aggregated decision matrix
For obtaining one group decision, we aggregate all the individual decision matrices ( M k ) to an aggregated decision matrix (M) using single valued neutrosophic weighted averaging (SVNWA) operator ([51]) as follows:
a ij = S V N S W A λ (   a ij 1 ,   a ij 2 ,   a ij 3 ,   ,   a ij ρ ) = ( λ 1 a i j 1 λ 2 a i j 2 λ 3 a i j 3 λ ρ a i j ρ ) = <   1 k = 1 ρ ( 1   T i j k ) λ k ,   k = 1 ρ ( I i j k ) λ k ,   k = 1 ρ ( F i j k ) λ k >
Therefore, the aggregated decision matrix is defined as follows:
M = ( G 1 G 2 .... G n A 1 a 11 a 12 a 1 n A 2 a 21 a 22 a 2 n . . . A m a m 1 a m 2 a m n )
where, a ij = < T i j ,   I i j ,   F i j   > , (i = 1, 2, 3, …, m; j = 1, 2, 3, …, n; k = 1, 2, 3, …, ρ).
Step 5. Determinate the weight of attributes
To find the attributes weight we introduce a model based on the NS-cross entropy measure. The collective NS-cross entropy measure between M (Weighted aggregated decision matrix) and P (Ideal matrix) for each attribute is defined by
C E N S j ( M ,   P ) = 1 m i = 1 m C E N S   ( M ( A i ( G j ) ) ,   P ( A i ( G j ) ) )
where, i = 1, 2, 3, …, m; j = 1, 2, 3, …, n.
Thus, we defined a weight model for attributes as follows:
w j =   ( 1 ÷   C E N S j ( M ,   P ) ) J = 1 n ( 1 ÷   C E N S j ( M ,   P ) )
where, 0 w j 1 and j = 1 n w j =   1 for j = 1, 2, 3, …, n.
Step 6. Calculate the weighted NS-cross entropy measure
Using Equation (2), we calculate weighted cross entropy value between weighted aggregated matrix and priori matrix. The cross entropy values can be presented in matrix form as follows:
M C E w N S = ( CE NS w   ( A 1 ) CE NS w   ( A 2 ) ............... ................. CE NS w   ( A m ) )
Step 7. Rank the priority
Smaller value of the cross entropy reflects that an alternative is closer to the ideal alternative. Therefore, the preference priority order of all the alternatives can be determined according to the increasing order of the cross entropy values CE NS w   ( A i ) (i = 1, 2, 3, …, m). Smallest cross entropy value indicates the best alternative and greatest cross entropy value indicates the worst alternative.
Step 8. Select the best alternative
From the preference rank order (from step 7), we select the best alternative.

5. Illustrative Example

In this section, we solve an illustrative example adapted from [12] of MAGDM problems to reflect the feasibility, applicability and efficiency of the proposed strategy under the SVNS environment.
Now, we use the example [12] for cultivation and analysis. A venture capital firm intends to make evaluation and selection of five enterprises with the investment potential:
(1)
Automobile company (A1)
(2)
Military manufacturing enterprise (A2)
(3)
TV media company (A3)
(4)
Food enterprises (A4)
(5)
Computer software company (A5)
On the basis of four attributes namely:
(1)
Social and political factor (G1)
(2)
The environmental factor (G2)
(3)
Investment risk factor (G3)
(4)
The enterprise growth factor (G4).
The investment firm makes a panel of three decision-makers.
The steps of decision-making strategy (4.1.1.) to rank alternatives are presented as follows:
Step: 1. Formulate the decision matrices
We represent the rating values of alternatives A i (i = 1, 2, 3, 4, 5) with respects to the attributes G j (j = 1, 2, 3, 4) provided by the decision-makers E k (k = 1, 2, 3) in matrix form as follows:
Decision matrix for E 1 decision-maker
M 1 = ( G 1 G 2 G 3 G 4 A 1 ( 0.9 , 0.5 ,   0.4 ) ( 0.7 , 0.4 ,   0.4 ) ( 0.7 ,   0.3 , 0.4 ) ( 0.5 , 0.4 , 0.9 ) A 2 ( 0.7 , 0.2 , 0.3 ) ( 0.8 ,   0.4 ,   0.3 ) ( 0.9 ,   0.6 ,   0.5 ) ( 0.9 ,   0.1 ,   0.3 ) A 3 ( 0.8 ,   0.4 ,   0.4 ) ( 0.7 ,   0.4 ,   0.2 ) ( 0.9 ,   0.7 ,   0.6 ) ( 0.7 ,   0.3 ,   0.3 ) A 4 ( 0.5 ,   0.8 ,   0.7 ) ( 0.6 ,   0.3 ,   0.4 ) ( 0.7 ,   0.2 ,   0.5 ) ( 0.5 ,   0.4 ,   0.7 ) A 5 ( 0.8 ,   0.4 ,   0.3 ) ( 0.5 ,   0.4 ,   0.5 ) ( 0.6 ,   0.4 ,   0.4 ) ( 0.9 ,   0.7 ,   0.5 ) )
Decision matrix for E 2 decision-maker
M   2 = ( G 1 G 2 G 3 G 4 A 1 ( 0.7 ,   0.2 ,   0.3 ) ( 0.5 ,   0.4 ,   0.5 ) ( 0.9 ,   0.4 ,   0.5 ) ( 0.6 ,   0.5 ,   0.3 ) A 2 ( 0.7 ,   0.4 ,   0.4 ) ( 0.7 ,   0.3 ,   0.4 ) ( 0.7 ,   0.3 ,   0.4 ) ( 0.6 ,   0.4 ,   0.3 ) A 3 ( 0.6 ,   0.4 ,   0.4 ) ( 0.5 ,   0.3 ,   0.5 ) ( 0.9 ,   0.5 ,   0.4 ) ( 0.6 ,   0.5 ,   0.6 ) A 4 ( 0.7 ,   0.5 ,   0.3 ) ( 0.6 ,   0.3 ,   0.6 ) ( 0.7 ,   0.4 ,   0.4 ) ( 0.8 ,   0.5 ,   0.4 ) A 5 ( 0.9 , 0.4 ,   0.3 ) ( 0.6 ,   0   .4 ,   0.5 ) ( 0.8 ,   0.5 ,   0.6 ) ( 0.5 ,   0.4 ,   0.5 ) )
Decision matrix for E 3 decision-maker
M   3 = ( G 1 G 2 G 3 G 4 A 1 ( 0.7 ,   0.2 ,   0.5 ) ( 0.6 ,   0.4 ,   0.4 ) ( 0.7 ,   0.4 ,   0.5 ) ( 0.9 ,   0.4 ,   0.3 ) A 2 ( 0.6 ,   0.5 ,   0.5 ) ( 0.9 ,   0.3 ,   0.4 ) ( 0.7 ,   0.4 ,   0.3 ) ( 0.8 ,   0.4 ,   0.5 ) A 3 ( 0.8 ,   0.3 ,   0.5 ) ( 0.9 ,   0.3 ,   0.4 ) ( 0.8 ,   0.3 ,   0.4 ) ( 0.7 ,   0.3 ,   0.4 ) A 4 ( 0.9 ,   0.3 ,   0.4 ) ( 0.6 ,   0.3 ,   0.4 ) ( 0.5 ,   0.2 ,   0.4 ) ( 0.7 ,   0.3 ,   0.5 ) A 5 ( 0.8 ,   0.3 ,   0.3 ) ( 0.6 ,   0.4 ,   0.3 ) ( 0.6 ,   0.3 ,   0.4 ) ( 0.7 ,   0.3 ,   0.5 ) )
Step: 2. Formulate priori/ideal decision matrix
A priori/ideal decision matrix Please provide a sharper picture
P = ( G 1 G 2 G 3 G 4 A 1 ( 0.9 ,   0.2 ,   0.3 ) ( 0.7 ,   0.4 ,   0.4 ) ( 0.9 ,   0.3 ,   0.4 ) ( 0.9 ,   0.4 ,   0.3 ) A 2 ( 0.7 ,   0.2 ,   0.3 ) ( 0.9 ,   0.3 ,   0.3 ) ( 0.9 ,   0.3 ,   0.3 ) ( 0.9 ,   0.1 ,   0.3 ) A 3 ( 0.8 ,   0.3 ,   0.4 ) ( 0.9 ,   0.3 ,   0.2 ) ( 0.9 ,   0.3 ,   0.4 ) ( 0.7 ,   0.3 ,   0.3 ) A 4 ( 0.9 ,   0.3 ,   0.3 ) ( 0.6 ,   0.3 ,   0.4 ) ( 0.7 ,   0.2 ,   0.4 ) ( 0.7 ,   0.3 ,   0.4 ) A 5 ( 0.9 ,   0.3 ,   0.3 ) ( 0.6 ,   0.4 ,   0.3 ) ( 0.8 ,   0.3 ,   0.4 ) ( 0.9 ,   0.3 ,   0.5 ) )
Step: 3. Determine the weight of decision-makers
By using Equations (5) and (6), we determine the weights of the three decision-makers as follows:
λ 1 =   ( 1 ÷   0.9 ) 3.37 0.33 ,   λ 2 =   ( 1 ÷   1.2 ) 3.37 0.25   λ 1 =   ( 1 ÷   .07 ) 3.37 0.42 .
Step: 4. Formulate the weighted aggregated decision matrix
Using Equation (7) the weighted aggregated decision matrix is presented as follows:
Weighted Aggregated decision matrix
M = ( G 1 G 2 G 3 G 4 A 1 ( 0.8 , 0.3 ,   0.4 ) ( 0.6 ,   0.4 ,   0.4 ) ( 0.8 , 0.4 ,   0.4 ) ( 0.7 , 0.4 ,   0.5 ) A 2 ( 0.7 ,   0.3 , 0   .4 ) ( 0.8 ,   0.3 ,   0.4 ) ( 0.8 ,   0.4 ,   0.4 ) ( 0.8 ,   0.2 ,   0.3 ) A 3 ( 0.8 ,   0.4 ,   0.4 ) ( 0.8 , 0.3 ,   0.3 ) ( 0.9 ,   0.5 ,   0.5 ) ( 0.7 ,   0.3 ,   0.4 ) A 4 ( 0.7 , 0.5 ,   0.5 ) ( 0.6 ,   0.3 ,   0.4 ) ( 0.6 ,   0.2 , 0.4 ) ( 0.7 ,   0.4 ,   0.5 ) A 5 ( 0.8 ,   0.4 ,   0.4 ) ( 0.6 ,   0.4 ,   0.4 ) ( 0.7 ,   0.4 ,   0.4 ) ( 0.8 ,   0.5 ,   0.5 ) )
Step: 5. Determinate the weight of the attributes
By using Equations (9) and (10), we determine the weights of the four attribute as follows:
w 1 =   ( 1 ÷ 0.26 ) 25 0.16 ,   w 2 =   ( 1 ÷ 0.11 ) 25 0.37 ,   w 3 =   ( 1 ÷ 0.20 ) 25 0.20 ,   w 4 =   ( 1 ÷ 0.15 ) 25 0.27 .
Step: 6. Calculate the weighted SVNS cross entropy matrix
Using Equation (2) and weights of attributes, we calculate the weighted NS-cross entropy values between ideal matrix and weighted aggregated decision matrix.
M C E w N S = ( 0.195 0.198 0.168 0.151 0.184 )
Step: 7. Rank the priority
The cross entropy values of alternatives are arranged in increasing order as follows:
0.151 < 0.168 < 0.184 < 0.195 < 0.198.
Alternatives are then preference ranked as follows:
A4 > A3 > A5 > A1 > A2.
Step: 8. Select the best alternative
From step 7, we identify A4 is the best alternative. Hence, Food enterprises (A4) is the best alternative for investment.
In Figure 2, we draw a bar diagram to represent the cross entropy values of alternatives which shows that A4 is the best alternative according our proposed strategy.
In Figure 3, we represent the relation between cross entropy values and acceptance values of alternatives. The range of acceptance level for five alternatives is taken by five points. The high acceptance level of alternatives indicates the best alternative for acceptance and low acceptance level of alternative indicates the poor acceptance alternative.
We see from Figure 3 that alternative A4 has the smallest cross entropy value and the highest acceptance level. Therefore A4 is the best alternative for acceptance. Figure 3 indicates that alternative A2 has highest cross entropy value and lowest acceptance value that means A2 is the worst alternative. Finally, we conclude that the relation between cross entropy values and acceptance value of alternatives is opposite in nature.

6. Comparative Study and Discussion

In literature only two MADM strategies [144,145] have been proposed. No MADGM strategy is available. So the proposed MAGDM is novel and non-comparable with the existing cross entropy under SVNS for numerical example.
i.
The MADM strategies [144,145] are not applicable for MAGDM problems. The proposed MAGDM strategy is free from such drawbacks.
ii.
Ye [144] proposed cross entropy that does not satisfy the symmetrical property straightforward and is undefined for some situations but the proposed strategy satisfies symmetric property and is free from undefined phenomenon.
iii.
The strategies [144,145] cannot deal with the unknown weight of the attributes whereas the proposed MADGM strategy can deal with the unknown weight of the attributes
iv.
The strategies [144,145] are not suitable for dealing with the unknown weight of decision-makers, whereas the essence of the proposed NS-cross entropy-based MAGDM is that it is capable of dealing with the unknown weight of the decision-makers.

7. Conclusions

In this paper, we have defined a novel cross entropy measure in SVNS environment. The proposed cross entropy measure in SVNS environment is free from the drawbacks of asymmetrical behavior and undefined phenomena. It is capable of dealing with the unknown weight of attributes and the unknown weight of decision-makers. We have proved the basic properties of the NS-cross entropy measure. We also defined weighted NS-cross entropy measure and proved its basic properties. Based on the weighted NS-cross entropy measure, we have developed a novel MAGDM strategy to solve neutrosophic multi-attribute group decision-making problems. We have at first proposed a novel MAGDM strategy based on NS-cross entropy measure with technique to determine the unknown weight of attributes and the unknown weight of decision-makers. Other existing cross entropy measures [144,145] can deal only with the MADM problem with single decision-maker and known weight of the attributes. So in general, our proposed NS-cross entropy-based MAGDM strategy is not comparable with the existing cross-entropy-based MADM strategies [144,145] under the single-valued neutrosophic environment. Finally, we solve a MAGDM problem to show the feasibility, applicability and efficiency of the proposed MAGDM strategy. The proposed NS-cross entropy-based MAGDM can be applied in teacher selection, pattern recognition, weaver selection, medical treatment selection options, and other practical problems. In future study, the proposed NS-cross entropy-based MAGDM strategy can be also extended to the interval neutrosophic set environment.

Acknowledgments

The authors are very grateful to the anonymous reviewers for their insightful and constructive comments and suggestions that have led to an improved version of this paper.

Author Contributions

Surapati Pramanik conceived and designed the problem; Surapati Pramanik and Shyamal Dalapati solved the problem; Surapati Pramanik, Shariful Alam, Florentin Smarandache and Tapan Kumar Roy analyzed the results; Surapati Pramanik and Shyamal Dalapati wrote the paper.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. Decision-making procedure of the proposed MAGDM strategy.
Figure 1. Decision-making procedure of the proposed MAGDM strategy.
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Figure 2. Bar diagram of alternatives versus weighted NS-cross entropy values of alternatives.
Figure 2. Bar diagram of alternatives versus weighted NS-cross entropy values of alternatives.
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Figure 3. Relation between weighted NS-cross entropy values and acceptance level line of alternatives.
Figure 3. Relation between weighted NS-cross entropy values and acceptance level line of alternatives.
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MDPI and ACS Style

Pramanik, S.; Dalapati, S.; Alam, S.; Smarandache, F.; Roy, T.K. NS-Cross Entropy-Based MAGDM under Single-Valued Neutrosophic Set Environment. Information 2018, 9, 37. https://doi.org/10.3390/info9020037

AMA Style

Pramanik S, Dalapati S, Alam S, Smarandache F, Roy TK. NS-Cross Entropy-Based MAGDM under Single-Valued Neutrosophic Set Environment. Information. 2018; 9(2):37. https://doi.org/10.3390/info9020037

Chicago/Turabian Style

Pramanik, Surapati, Shyamal Dalapati, Shariful Alam, Florentin Smarandache, and Tapan Kumar Roy. 2018. "NS-Cross Entropy-Based MAGDM under Single-Valued Neutrosophic Set Environment" Information 9, no. 2: 37. https://doi.org/10.3390/info9020037

APA Style

Pramanik, S., Dalapati, S., Alam, S., Smarandache, F., & Roy, T. K. (2018). NS-Cross Entropy-Based MAGDM under Single-Valued Neutrosophic Set Environment. Information, 9(2), 37. https://doi.org/10.3390/info9020037

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