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Article

Statistical Analyses of a Class of Random Cyclooctatetraene Chain Networks with Respect to Several Topological Properties

School of Mathematics and Big Data, Anhui University of Science & Technology, Huainan 232001, China
*
Author to whom correspondence should be addressed.
Symmetry 2023, 15(11), 1971; https://doi.org/10.3390/sym15111971
Submission received: 19 September 2023 / Revised: 17 October 2023 / Accepted: 20 October 2023 / Published: 24 October 2023
(This article belongs to the Special Issue Symmetry and Graph Theory)

Abstract

:
In recent years, the research on complex networks has created a boom. The objective of the present paper is to study a random cyclooctatetraene chain whose graph-theoretic mathematical properties arose scientists’ interests. By applying the concept of symmetry and probability theory, we obtain the explicit analytical expressions for the variances of Schultz index, multiplicative degree-Kirchhoff index Gutman index, and additive degree-Kirchhoff index of a random cyclooctatetraene chain with n octagons, which plays a crucial role in the research and application of topological indices.

1. Introduction

In this paper, we just take finite and simple connected graphs into consideration, referring to [1] and the references cited therein. Chemistry is strongly linked to graph theory, and graph theory has been widely used in chemistry. In chemical graph theory, there are some alternatives between atoms that vertices represent the atoms and edges represent the covalent bonds. They are used to depict chemical compounds.
The molecular formula of a compound can represent different molecular structures and characteristics, but theoretical chemists are concerned with the physical and chemical properties of a compound and its relationship with the molecular formula of a compound. The physical and chemical properties of compounds are key areas of concern for theoretical chemists [2,3]. Polygonal chemicals have a wide diversity of molecular structures and their physical and chemical properties are becoming increasingly significant, which is referenced in [4,5,6,7].
There is no octagon in octagonal chains that has more than two cut-vertices, and such a octagonal chain is called a cyclooctatetraene chain. Cyclooctatetraene is the poster child for nonaromatic molecules. Cyclooctatetraene and its derivatives have fascinated chemists for a long time and have a wide range of applications in industry. Cyclooctatetraene differs from benzene in that it is not an aromatic hydrocarbon. It is chemically close to an unsaturated hydrocarbon. Not only can it be subjected to addition reactions, which is easily hydrogenated to form cyclooctane. It also oxidises and polymerises readily. A number of vital compounds of cyclooctatetraene can be served as substrates for the production of scientifically and commercially valuable materials. In this paper, we consider four kinds of indices of cyclooctatetraene chains with n octagons. We simply consider the situation starting from a vertex of a cyclooctatetraene chain, connecting an edge to another octagon. For more information about the cyclooctylene chain, we can refer to [8,9,10,11].
We give some basic notations. Set G = ( V G , E G ) be a graph with vertices denoted V G and edges denoted E G . The number of edges in a graph G is denoted by | E ( G ) | . We claim that two vertices p and m are adjacent (or neighbours) if they are attached by an edge, which we will write as p m . In G, the shortest length p , m -path among the paths between two vertices p and m is denoted as d G ( p , m ) (or simply d ( p , m ) ). The Wiener index of G refers to the aggregate of distances between all the vertex pairs of G. It was created by H. Wiener in 1947 [12], that is
W ( G ) = { p , m } V G d ( p , m ) .
The Wiener index is among the best studied, most understood, and most widely used molecular shape descriptors, and is based on graph theory, see [13,14,15,16].
A graph G = ( V G , E G ) together with the weight function ω : V G N + is known as a weighted graph [17] ( G , ω ) . Let ⊕ denote one of the four arithmetic operations + , , × , ÷ [18]. Consequently, the weighted Wiener index W ( G , ω ) is determined as
W ( G , ω ) = 1 2 p V G m V G ( ω ( p ) ω ( m ) ) d ( p , m ) .
Obviously, if ω 1 and ⊕ denotes the operation ×, then W ( G , ω ) = W ( G ) .
In case ⊕ represents the operation × and ω ( · ) d G ( · ) , then (2) is equivalent to [19]
G u t ( G ) = 1 2 p V G m V G ( d G ( p ) d G ( m ) ) d ( p , m ) = { p . m } V G ( d G ( p ) d G ( m ) ) d ( p , m ) .
This is just the Gutman index. Research on possible chemical applications of the Gutman index and similar quantities and their theoretical study, for which polycyclic molecules are more difficult cases, see [20].
In case ⊕ represents the operation + and ω ( · ) d G ( · ) , then (2) is equivalent to
S ( G ) = 1 2 p V G m V G ( d G ( p ) + d G ( m ) ) d ( p , m ) = { p . m } V G ( d G ( p ) + d G ( m ) ) d ( p , m ) .
That’s what the Schultz Index is all about. For additional articles on developing aspects of the topology indexes for [21,22,23,24], including mathematical properties, discrimination and applications, refer to [25].
In case of a , b V ( G ) , the resistance distance between a and b in G, is defined as the effective resistance between nodes a and b in the electrical network, where the nodes correspond to vertices of G and each edge of G is replaced by a resistor of unit resistance. The resistance distance between vertices a and b in G [26] is denoted as r ( a , b ) . For more detailed information, see [27,28,29,30]. It is the Kirchhoff index when the Wiener index is for non-trees, and this distance function is proposed by Klein and Randić [31], defined as
K f ( G ) = { a , b } V G r ( a , b ) .
For a description of the sum of eccentricity distances and the sum of eccentricity resistance-distances, refer to [32,33,34,35,36].
K f * ( G ) was introduced by Chen and Zhang in 2007 [37] (see [38] for details), which is defined as
K f * ( G ) = { a , b } V G d ( a ) d ( b ) r ( a , b ) ,
Thus, the invariance of this graph is represented as
K f * ( G ) = 2 | E G | i = 2 n 1 λ i ,
from which 0 = λ 1 < λ 2 λ n are the eigenvalues of l ( G ) . Moreover, l ( G ) is the normalized Laplacian matrix of G, as proposed by Chung [39]. The normalized Laplacian index and multiplicative degree-Kirchhoff index play an essential application in mathematical chemistry and statistics. Research on these topics has attracted a wide range of attention from researchers.
K f + ( G ) was introduced by Gutman, Feng and Yu in 2012 [40], which is defined as
K f + ( G ) = { a , b } V G ( d ( a ) + d ( b ) ) r ( a , b ) .
Probability properties are an important component of chemical graphs, which can more broadly describe the topological properties and structures of chemical graphs. In this paper, we focus on the cyclooctatetraene chain G n with n octagons, which is formed as follows.
Firstly, G 1 is an octagon and G 2 is the graph with two octagons, as shown in Figure 1.
Secondly, by appending a new terminal octagon H n + 1 to G n , the random cyclooctatetraene chain G n + 1 with n octagons can be constructed. We illustrates this process in Figure 2. As demonstrated in Figure 3, we can append the terminal octagon H n + 1 to G n with four methods and indicate the generated figures with G n + 1 1 , G n + 1 2 , G n + 1 3 , and G n + 1 4 , respectively.
At each step, randomly pick one of the following possible outcomes:
  • p 1 is the probability that G n G n + 1 1 ;
  • p 2 is the probability that G n G n + 1 2
  • p 3 is the probability that G n G n + 1 3
  • p 4 = 1 p 1 p 2 p 3 is the probability that G n G n + 1 4 .
We consider four random variables Z n 1 , Z n 2 , Z n 3 , and Z n 4 for our choice. When i = 1 , 2 , 3 , 4 , in case our selection is G n + 1 i , we have Z n i = 1 ; otherwise, Z n i = 0 , and we can easily derive that
P ( Z n i = 1 ) = p i , P ( Z n i = 0 ) + P ( Z n i = 1 ) = 1
and Z n 1 + Z n 2 + Z n 3 + Z n 4 = 1 .
Through the above process, we get a random cyclooctatetraene chain G n ( p 1 , p 2 , p 3 , p 4 ) . We always abbreviate G n ( p 1 , p 2 , p 3 , p 4 ) to G n . All of S ( G n ) , K f * ( G n ) , G u t ( G n ) and K f + ( G n ) are random variables in probability by noting that G n is a random graph. From a probabilistic point of view, a natural question arises: when n is big enough, will the distribution of S ( G n ) , K f * ( G n ) , G u t ( G n ) and K f + ( G n ) look like a probability distribution or not.
In this paper, we make researches on S ( G n ) , K f * ( G n ) , G u t ( G n ) and K f + ( G n ) . There is a huge amount of relevant literature. For random polyphenylene chain, J.I. Zhang, X.H. Peng, H.I. Chen [18] established the limiting behaviours of S ( G n ) , K f * ( G n ) , G u t ( G n ) and K f + ( G n ) . Here it is natural and interesting to consider limiting behaviours of S ( G n ) , K f * ( G n ) , G u t ( G n ) and K f + ( G n ) for random cyclooctatetraene chain. In this paper, by applying the concept of symmetry and probability theory, we derive definite analytical expressions for the variance of the Schultz index, multiplicative degree-Kirchhoff index, Gutman index and additive degree-Kirchhoff index of a random cyclooctatetraene chain with n octagons, which plays a crucial role in the research and application of topological indices.
In this paper, in order to better describe the probability properties of cyclooctylene chain, we propose the following hypothesis.
Hypothesis 1.
We choose to attach the new terminal octagon H n + 1 to G n , where n = 2 , 3 , . . . , and it is random and independent. More precisely, a range of random variables Z n 1 , Z n 2 , Z n 3 , Z n 4 n = 2 is independent and has the same law (9). With regard to some i 1 , 2 , 3 , 0 < p i < 1 is obvious. Based on Hypothesis 1, we present analytical expressions for the variances of S ( G n ) , K f * ( G n ) , G u t ( G n ) and K f + ( G n ) .

2. The Variances for the Gutman Index and Schultz Index of a Random Cyclooctatetraene Chain

For all G n , the Gutman index and Schultz index of a random cyclooctatetraene chain are random variables. We are going to take the variances of G u t ( G n ) and S ( G n ) into consideration in this section. Actually, G n + 1 is G n connected by an edge to a new terminal octagon H n + 1 , where H n + 1 is extended by vertices x 1 , x 2 , x 3 , x 4 , x 5 , x 6 , x 7 , and x 8 , and p n x 1 is the new edge; see Figure 2. On the one hand, for all m V G n ,
d ( x 1 , m ) = d ( p n , m ) + 1 , d ( x 2 , m ) = d ( p n , m ) + 2 , d ( x 3 , m ) = d ( p n , m ) + 3 , d ( x 4 , m ) = d ( p n , m ) + 4 ,
d ( x 5 , m ) = d ( p n , m ) + 5 , d ( x 6 , m ) = d ( p n , m ) + 4 , d ( x 7 , m ) = d ( p n , m ) + 3 , d ( x 2 , m ) = d ( p n , m ) + 2 ,
m V G n d G n + 1 ( m ) = 18 n 1 .
on the other hand, for all t { 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 }
t = 1 8 d ( x t ) d ( x 1 , x t ) = 32 , t = 1 8 d ( x t ) d ( x 2 , x t ) = 33 , t = 1 8 d ( x t ) d ( x 3 , x t ) = 34 , t = 1 8 d ( x t ) d ( x 4 , x t ) = 35 ,
t = 1 8 d ( x t ) d ( x 5 , x t ) = 36 , t = 1 8 d ( x t ) d ( x 6 , x t ) = 35 , t = 1 8 d ( x t ) d ( x 7 , x t ) = 34 , t = 1 8 d ( x t ) d ( x 8 , x t ) = 33 .
In [41] Theorem 1, the author proves that
E ( G u t ( G n ) ) = ( 270 162 p 1 108 p 2 54 p 3 ) n 3 + ( 486 p 1 + 324 p 2 + 162 p 3 90 ) n 2 + ( 77 324 p 1 216 p 2 108 p 3 ) n 1 .
where E ( G u t ( G n ) is the mathematical expectations of G u t ( G n ) .
We now present the first main result of this section.
Theorem 1.
The results are as follows, if Hypothesis 1 holds. As to the random cyclooctatetraene chain G n , the variance of Gutman index G u t ( G n ) , computed as
V a r ( G u t ( G n ) ) = 1 30 ( σ 2 n 5 5 r n 4 + 10 σ ˜ 2 n 3 + ( 65 r 30 σ 2 45 σ ˜ 2 ) n 2 + ( 120 r + 59 σ 2 + 65 σ ˜ 2 ) n + ( 60 r 30 σ 2 30 σ ˜ 2 ) ) .
where
σ 2 = 648 2 p 1 + 972 2 p 2 + 1296 2 p 3 + 1620 2 p 4 ( 648 p 1 + 972 p 2 + 1296 p 3 + 1620 p 4 ) 2 σ ˜ 2 = 90 2 p 1 + 414 2 p 2 + 738 2 p 3 + 1062 2 p 4 ( 90 p 1 + 414 p 2 + 738 p 3 + 1062 p 4 ) 2 r = 648 · 90 · p 1 + 972 · 414 · p 2 + 1296 · 738 · p 3 + 1620 · 1062 · p 4 ( 648 p 1 + 972 p 2 + 1296 p 3 + 1620 p 4 ) · ( 90 p 1 + 414 p 2 + 738 p 3 + 1062 p 4 )
Proof. 
Let
A n : = 18 m V G n d ( m ) d ( p n , m ) .
then, by (5.1) of [41], we obtain
G u t ( G n + 1 ) = G u t ( G n ) + A n + 882 n + 239 .
Recalling from Section 1 that Z n 1 , Z n 2 , Z n 3 , and Z n 4 are random variables, this indicates our option in constructing G n + 1 from G n . We have four equalities as follows:
Equality 1.
A n Z n 1 = ( A n 1 + 648 n 90 ) Z n 1 .
If Z n 1 = 0 , the equality mentioned above is evident. Thus, we only have to regard the case Z n 1 = 1 , which means that G n G n + 1 1 . In this view, p n (of G n ) is coincident with the vertex labeled x 2 or x 8 (of H n ), see Figure 4. In this scenario, A n turns into
18 m V G n d ( m ) d ( x 2 , m ) = 18 m V G n 1 d ( m ) d ( x 2 , m ) + 18 m V H n d ( m ) d ( x 2 , m ) = 18 m V G n 1 d ( m ) ( d ( m , p n 1 ) + d ( x 2 , p n 1 ) ) + 18 × 33 = 18 m V G n 1 d ( m ) ( d ( m , p n 1 ) + 2 ) + 18 × 33 = A n 1 + 36 m V G n 1 d ( m ) + 594 = A n 1 + 36 ( 18 n 19 ) + 594 = A n 1 + 648 n 90 ,
In the foregoing, we utilised (10)–(12). As a result, we arrive at the required equivalence conclusion.
Equality 2.
A n Z n 2 = ( A n 1 + 972 n 414 ) Z n 2 .
As in the proof of Equality 1, we only have to regard the case Z n 2 = 1 , which is G n G n + 1 2 . The proof process is analogous, and we leave out the details.
Equality 3.
A n Z n 3 = ( A n 1 + 1296 n 738 ) Z n 3
We have to regard the case Z n 3 = 1 , which is G n G n + 1 3 . The proof is the same as Equality 1 and we omit the details.
Equality 4.
A n Z n 4 = ( A n 1 + 1620 n 1062 ) Z n 4
We have to regard the case Z n 4 = 1 , which is G n G n + 1 4 . The proof process is also analogous, and we leave out the details.
Recalling that Z n 1 + Z n 2 + Z n 3 + Z n 4 = 1 , according to the above discussion, it holds that
A n = A n ( Z n 1 + Z n 2 + Z n 3 + Z n 4 ) = ( A n 1 + 648 n 90 ) Z n 1 + ( A n 1 + 972 n 414 ) Z n 2 + ( A n 1 + 1296 n 738 ) Z n 3 + ( A n 1 + 1620 n 1062 ) Z n 4 = A n 1 + ( 648 Z n 1 + 972 Z n 2 + 1296 Z n 3 + 1620 Z n 4 ) n ( 90 Z n 1 + 414 Z n 2 + 738 Z n 3 + 1062 Z n 4 ) = A n 1 + n · U n V n .
For each n, it indicates that U n = 648 Z n 1 + 972 Z n 2 + 1296 Z n 3 + 1620 Z n 4 , V n = 90 Z n 1 + 414 Z n 2 + 738 Z n 3 + 1062 Z n 4 .
Therefore, by (15) we obtain
G u t ( G n ) = G u t ( G 1 ) + t = 1 n 1 A t + t = 1 n 1 ( 882 t + 239 ) = G u t ( G 1 ) + t = 1 n 1 ( q = 1 t 1 ( A q + 1 A q ) + A 1 ) + t = 1 n 1 ( 882 t + 239 ) = G u t ( G 1 ) + t = 1 n 1 q = 1 t 1 ( A q + 1 A q ) + ( n 1 ) A 1 + t = 1 n 1 ( 882 t + 239 ) = G u t ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + ( n 1 ) A 1 + t = 1 n 1 ( 882 t + 239 ) = G u t ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + O ( n 2 )
where O ( n 2 ) representing high-order infinitesimal of n 2 .
By direct calculation, one sees that V a r ( U q ) = σ 2 , V a r ( V q ) = σ ˜ 2 , and C o v ( U q , V q ) = r , where for any two random variables X and Y, C o v ( X , Y ) = E ( X Y ) E ( X ) · E ( Y ) . Based on the nature of the variance and the order in which the sums are exchanged, it can be concluded that
V a r ( G u t ( G n ) ) = V a r ( t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) ) = V a r ( q = 1 n 2 t = q + 1 n 1 ( ( q + 1 ) U q + 1 V q + 1 ) ) = V a r ( q = 1 n 2 ( ( q + 1 ) U q + 1 V q + 1 ) ( n q 1 ) ) = q = 1 n 2 ( n q 1 ) 2 V a r ( ( q + 1 ) U q + 1 V q + 1 ) = q = 1 n 2 ( n q 1 ) 2 C o v ( ( q + 1 ) U q + 1 V q + 1 , ( q + 1 ) U q + 1 V q + 1 ) = q = 1 n 2 ( n q 1 ) 2 ( ( q + 1 ) 2 C o v ( U q + 1 , U q + 1 ) 2 ( q + 1 ) C o v ( U q + 1 , V q + 1 ) + C o v ( V q + 1 , V q + 1 ) ) = q = 1 n 2 ( n q 1 ) 2 ( ( q + 1 ) 2 σ 2 2 ( q + 1 ) r + σ ˜ 2 ) .
By means of computational, ad hoc tools, the above equality gives the required results, V a r ( G u t ( G n ) ) .
Now, we discuss the variance of the Schultz index.
By Theorem 2.3 of [41], we have
E ( S ( G n ) ) = ( 240 144 p 1 96 p 2 48 p 3 ) n 3 + ( 432 p 1 + 288 p 2 + 144 p 3 40 ) n 2 + ( 56 288 p 1 192 p 2 96 p 3 ) n .
After that we illustrate our results.
Theorem 2.
Supposing that Hypothesis 1, then the following results are true. As to the random cyclooctatetraene chain G n , the variance of Schultz index S ( G n ) , computed as
V a r ( S ( G n ) ) = 1 30 ( σ 2 n 5 5 r n 4 + 10 σ ˜ 2 n 3 + ( 65 r 30 σ 2 45 σ ˜ 2 ) n 2 + ( 120 r + 59 σ 2 + 65 σ ˜ 2 ) n + ( 60 r 30 σ 2 30 σ ˜ 2 ) ) .
where
σ 2 = 576 2 p 1 + 864 2 p 2 + 1152 2 p 3 + 1440 2 p 4 ( 576 p 1 + 864 p 2 + 1152 p 3 + 1440 p 4 ) 2 σ ˜ 2 = 40 2 p 1 + 328 2 p 2 + 616 2 p 3 + 904 2 p 4 ( 40 p 1 + 328 p 2 + 616 p 3 + 904 p 4 ) 2 r = 576 · 40 · p 1 + 864 · 328 · p 2 + 1152 · 616 · p 3 + 1440 · 904 · p 4 ( 576 p 1 + 864 p 2 + 1152 p 3 + 1440 p 4 ) · ( 40 p 1 + 328 p 2 + 616 p 3 + 904 p 4 )
Proof. 
By [41] (5.2), we obtain
S ( G n + 1 ) = S ( G n ) + 18 m V G n d ( p n , m ) + 8 m V G n d ( m ) d ( p n , m ) + 824 n + 248 .
and
B n : = m V G n ( 18 + 8 d ( m ) ) d ( p n , m ) .
S ( G n + 1 ) = S ( G n ) + B n + 824 n + 248 .
After similar discussions, we have four equalities as follows:
Equality 1.
B n Z n 1 = ( B n 1 + 576 n 40 ) Z n 1
If Z n 1 = 0 , the equality mentioned above is evident, so we only have to regard the case Z n 1 = 1 , which means that G n G n + 1 1 . In this view, p n (of G n ) is coincident with the vertex labeled x 2 or x 8 (of H n ), see Figure 4. In this scenario, B n turns into
B n = m V G n ( 18 + 8 d ( m ) ) d ( x 2 , m ) = m V G n 1 ( 18 + 8 d ( m ) ) d ( x 2 , m ) + m V H n ( 18 + 8 d ( m ) ) d ( x 2 , m ) = m V G n 1 ( 18 + 8 d ( m ) ) ( d ( p n 1 , m ) + 2 ) + 18 × 16 + 8 × 33 = m V G n 1 ( 18 + 8 d ( m ) ) d ( p n 1 , m ) + 2 m V G n 1 ( 18 + 8 d ( m ) ) + 18 × 16 + 8 × 33 = m V G n 1 ( 18 + 8 d ( m ) ) d ( p n 1 , m ) + 2 ( 18 × 8 ( n 1 ) + 8 × ( 18 ( n 1 ) 1 ) ) + 18 × 16 + 8 × 33 = B n 1 + 2 ( 288 n 296 ) + 552 = B n 1 + 576 n 40
In the foregoing, we utilised (10)–(12). As a result, we arrive at the required equivalence conclusion.
Equality 2.
B n Z n 2 = ( B n 1 + 864 n 328 ) Z n 2
As in the proof of Equality 1, we only have to regard the case Z n 2 = 1 , which is G n G n + 1 2 . The proof process is analogous, and we leave out the details.
Equality 3.
B n Z n 3 = ( B n 1 + 1152 n 616 ) Z n 3
We have to regard the case Z n 3 = 1 , which is G n G n + 1 3 . The proof is the same as Equality 1 and we omit the details.
Equality 4.
B n Z n 4 = ( B n 1 + 1440 n 904 ) Z n 4
We have to regard the case Z n 4 = 1 , which is G n G n + 1 4 . The proof process is also analogous, and we leave out the details.
Recalling that Z n 1 + Z n 2 + Z n 3 + Z n 4 = 1 , according to the above discussion, it holds that
B n = B n ( Z n 1 + Z n 2 + Z n 3 + Z n 4 ) = B n 1 + n · U n V n
where for each n, U n = 576 Z n 1 + 864 Z n 2 + 1152 Z n 3 + 1440 Z n 4 , V n = 40 Z n 1 + 328 Z n 2 + 616 Z n 3 + 904 Z n 4 .
Therefore, by (15)
S ( G n ) = S ( G 1 ) + t = 1 n 1 B t + t = 1 n 1 ( 824 t + 248 ) = S ( G 1 ) + t = 1 n 1 ( q = 1 t 1 ( B q + 1 B q ) + B 1 ) + t = 1 n 1 ( 824 t + 2489 ) = S ( G 1 ) + t = 1 n 1 q = 1 t 1 ( B q + 1 B q ) + ( n 1 ) B 1 + t = 1 n 1 ( 824 t + 248 ) = S ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + ( n 1 ) B 1 + t = 1 n 1 ( 824 t + 248 ) = S ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + O ( n 2 ) .
If we replace G u t ( G n ) from the proof of Theorem 1 by S ( G n ) , the rest of the proof of this theorem is the same as the proof of Theorem 1, and therefore the details are omitted.

3. The Variances of Multiplicative and Additive Degree-Kirchhoff Indices of a Random Cyclooctatetraene Chain

In the section, we talk about the variances for the multiplicative degree-Kirchhoff index K f * ( G n ) and the additive degree-Kirchhoff index K f + ( G n ) . For a random cyclooctatetraene chain G n , K f * ( G n ) and K f + ( G n ) are random variables.
Recall that G n + 1 is G n connected by an edge to a new terminal octagon H n + 1 , where H n + 1 is extended by vertices x 1 , x 2 , x 3 , x 4 , x 5 , x 6 , x 7 , and x 8 , and p n x 1 is the new edge; see Figure 2. On the one hand, for all m V G n ,
r ( x 1 , m ) = r ( p n , m ) + 1 , r ( x 2 , m ) = r ( p n , m ) + 1 + 7 8 , r ( x 3 , m ) = r ( p n , m ) + 1 + 12 8 , r ( x 4 , m ) = r ( p n , m ) + 1 + 15 8 ,
r ( x 5 , m ) = r ( p n , m ) + 1 + 16 8 , r ( x 6 , m ) = r ( p n , m ) + 1 + 15 8 , r ( x 7 , m ) = r ( p n , m ) + 1 + 12 8 , r ( x 8 , m ) = r ( p n , m ) + 1 + 7 8 .
m V G n d G n + 1 ( m ) = 18 n 1 .
On the other hand, for all t { 1 , 2 , 3 , 4 , 5 , 6 , 7 , 8 }
t = 1 8 d ( x t ) r ( x 1 , x t ) = 21 , t = 1 8 d ( x t ) r ( x 2 , x t ) = 175 8 , t = 1 8 d ( x t ) r ( x 3 , x t ) = 45 2 , t = 1 8 d ( x t ) r ( x 4 , x t ) = 183 8 ,
t = 1 8 d ( x t ) r ( x 5 , x t ) = 23 , t = 1 8 d ( x t ) r ( x 6 , x t ) = 183 8 , t = 1 8 d ( x t ) r ( x 7 , x t ) = 45 2 , t = 1 8 d ( x t ) r ( x 8 , x t ) = 175 8 .
By Theorem 3.1 of [41], we have
E ( K f * ( G n ) ) = ( 162 243 4 p 1 27 p 2 27 4 p 3 ) n 3 + ( 36 + 729 4 p 1 + 81 p 2 + 81 4 p 3 ) n 2 ( 29 + 243 2 p 1 + 54 p 2 + 27 2 p 3 ) n 1 .
we now present the first main result of this section.
Theorem 3.
The results are as follows, if Hypothesis 1 holds. As to the random cyclooctatetraene chain G n , the variance of the multiplicative degree-Kirchhoff index K f * ( G n ) , computed as
V a r ( K f * ( G n ) ) = 1 30 ( σ 2 n 5 5 r n 4 + 10 σ ˜ 2 n 3 + ( 65 r 30 σ 2 45 σ ˜ 2 ) n 2 + ( 120 r + 59 σ 2 + 65 σ ˜ 2 ) n + ( 60 r 30 σ 2 30 σ ˜ 2 ) ) .
where
σ 2 = ( 1215 2 ) 2 p 1 + 810 2 p 2 + ( 1863 2 ) 2 p 3 + 972 2 p 4 ( 1215 2 p 1 + 810 p 2 + 1863 2 p 3 + 972 p 4 ) 2 σ ˜ 2 = ( 495 2 ) 2 p 1 + 450 2 p 2 + ( 1143 2 ) 2 p 3 + 612 2 p 4 ( 495 2 p 1 + 450 p 2 + 1143 2 p 3 + 612 p 4 ) 2 r = 1215 2 · 495 2 · p 1 + 810 · 450 · p 2 + 1863 2 · 1143 2 · p 3 + 972 · 612 · p 4 ( 1215 2 p 1 + 810 p 2 + 1863 2 p 3 + 972 p 4 ) · ( 495 2 p 1 + 450 p 2 + 1143 2 p 3 + 612 p 4 )
Proof. 
By [41] (5.3), we have
K f * ( G n + 1 ) = K f * ( G n ) + 18 m V G n d ( m ) r ( p n , m ) + 684 n + 151 .
and
C n : = 18 m V G n d ( m ) r ( p n , m ) .
K f * ( G n + 1 ) = K f * ( G n ) + C n + 684 n + 151 .
Recalling from Section 1 that Z n 1 , Z n 2 , Z n 3 , and Z n 4 are random variables, this indicates our option in constructing G n + 1 from G n . We have four equalities as follows:
Equality 1.
C n Z n 1 = ( C n 1 + 1215 2 n 495 2 ) Z n 1
If Z n 1 = 0 , the above equality is obvious, so we only need to consider the case Z n 1 = 1 , which implies G n G n + 1 1 . In this view, p n (of G n ) is coincident with the vertex labeled x 2 or x 8 (of H n ), see Figure 4. In this scenario, C n turns into
C n = 18 m V G n d ( m ) r ( x 2 , m ) = 18 m V G n 1 d ( m ) r ( x 2 , m ) + 18 m V H n d ( m ) r ( x 2 , m ) = 18 m V G n 1 d ( m ) ( 1 + 7 8 + r ( p n 1 , m ) ) + 175 8 × 18 = 18 m V G n 1 d ( m ) r ( p n 1 , m ) + 270 8 m V G n 1 d ( m ) + 175 8 × 18 = C n 1 + 270 8 ( 18 n 19 ) + 3150 8 = C n 1 + 1215 2 n 495 2
In the foregoing, we utilised (17)–(19). As a result, we arrive at the required equivalence conclusion.
Equality 2.
C n Z n 2 = ( C n 1 + 810 n 450 ) Z n 2
As in the proof of Equality 1, we only have to regard the case Z n 2 = 1 , which is G n G n + 1 2 . The proof process is analogous, and we leave out the details.
Equality 3.
C n Z n 3 = ( C n 1 + 1863 2 n 1143 2 ) Z n 3
We have to regard the case Z n 3 = 1 , which is G n G n + 1 3 . The proof is the same as Equality 1 and we omit the details.
Equality 4.
C n Z n 4 = ( C n 1 + 972 n 612 ) Z n 4
We have to regard the case Z n 4 = 1 , which is G n G n + 1 4 . The proof process is also analogous, and we leave out the details.
Recalling that Z n 1 + Z n 2 + Z n 3 + Z n 4 = 1 , according to the above discussion, it holds that
C n = C n ( Z n 1 + Z n 2 + Z n 3 + Z n 4 ) = C n 1 + n · U n V n
where for each n, U n = 1215 2 Z n 1 + 810 Z n 2 + 1863 2 Z n 3 + 972 Z n 4 , V n = 495 2 Z n 1 + 450 Z n 2 + 1143 2 Z n 3 + 612 Z n 4 .
Therefore, by (22)
K f * ( G n ) = K f * ( G 1 ) + t = 1 n 1 C t + t = 1 n 1 ( 684 t + 151 ) = K f * ( G 1 ) + t = 1 n 1 ( q = 1 t 1 ( C q + 1 C q ) + C 1 ) + t = 1 n 1 ( 684 t + 151 ) = K f * ( G 1 ) + t = 1 n 1 q = 1 t 1 ( C q + 1 C q ) + ( n 1 ) C 1 + t = 1 n 1 ( 684 t + 151 ) = K f * ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + ( n 1 ) C 1 + t = 1 n 1 ( 684 t + 151 ) = K f * ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + O ( n 2 )
Now, we consider K f + ( G n ) . By Theorem 3.3 of [41] we have
E ( K f + ( G n ) ) = ( 144 54 p 1 24 p 2 6 p 3 ) n 3 + ( 61 + 162 p 1 + 72 p 2 + 18 p 3 ) n 2 ( 37 + 108 p 1 + 48 p 2 + 12 p 3 ) n .
V a r ( K f + ( G n ) ) is given by
Theorem 4.
V a r ( K f + ( G n ) ) = 1 30 ( σ 2 n 5 5 r n 4 + 10 σ ˜ 2 n 3 + ( 65 r 30 σ 2 45 σ ˜ 2 ) n 2 + ( 120 r + 59 σ 2 + 65 σ ˜ 2 ) n + ( 60 r 30 σ 2 30 σ ˜ 2 ) ) .
where
σ 2 = 540 2 p 1 + 720 2 p 2 + 828 2 p 3 + 864 2 p 4 ( 540 p 1 + 720 p 2 + 828 p 3 + 864 p 4 ) 2 σ ˜ 2 = 191 2 p 1 + 371 2 p 2 + 479 2 p 3 + 515 2 p 4 ( 191 p 1 + 371 p 2 + 479 p 3 + 515 p 4 ) 2 r = 540 · 191 · p 1 + 720 · 371 · p 2 + 828 · 479 · p 3 + 864 · 515 · p 4 ( 540 p 1 + 720 p 2 + 828 p 3 + 864 p 4 ) · ( 191 p 1 + 371 p 2 + 479 p 3 + 515 p 4 )
Proof. 
By [41] (5.4), we see that
K f + ( G n + 1 ) = K f + ( G n ) + 18 m V G n r ( p n , m ) + 8 m V G n d ( m ) r ( p n , m ) + 637 n + 160 .
where
D n : = m V G n ( 18 + 8 d ( m ) ) r ( p n , m ) .
K f + ( G n + 1 ) = K f + ( G n ) + D n + 637 n + 160 .
Recalling from Section 1 that Z n 1 , Z n 2 , Z n 3 , and Z n 4 are random variables, this indicates our option in constructing G n + 1 from G n . We have four equalities as follows:
Equality 1.
D n Z n 1 = ( D n 1 + 540 n 191 ) Z n 1
If Z n 1 = 0 , the equality mentioned above is evident, so we only have to regard the case Z n 1 = 1 , which means that G n G n + 1 1 . In this view, p n (of G n ) is coincident with the vertex labeled x 2 or x 8 (of H n ), see Figure 4. In this scenario, D n turns into
m V G n ( 18 + 8 d ( m ) ) r ( x 2 , m ) = 18 m V G n d ( m ) r ( x 2 , m ) = m V G n 1 ( 18 + 8 d ( m ) ) r ( x 2 , m ) + m V H n ( 18 + 8 d ( m ) ) r ( x 2 , m ) = m V G n 1 ( 18 + 8 d ( m ) ) ( r ( p n 1 , m ) + 1 + 7 8 ) + 18 m V H n r ( x 2 , x i ) + 8 m V H n d ( x i ) r ( x 2 , x i ) = m V G n 1 ( 18 + 8 d ( m ) ) r ( p n 1 , m ) + 15 8 m V G n 1 ( 18 + 8 d ( m ) ) + 364 = D n 1 + 15 8 ( 288 n 296 ) + 364 = D n 1 + 540 n 191
In the foregoing, we utilised (17)–(19). As a result, we arrive at the required equivalence conclusion.
Equality 2.
D n Z n 2 = ( D n 1 + 720 n 371 ) Z n 2
As in the proof of Equality 1, we only have to regard the case Z n 2 = 1 , which is G n G n + 1 2 . The proof process is analogous, and we leave out the details.
Equality 3.
D n Z n 3 = ( D n 1 + 828 n 479 ) Z n 3
We have to regard the case Z n 3 = 1 , which is G n G n + 1 3 . The proof is the same as Equality 1 and we omit the details.
Equality 4.
D n Z n 4 = ( D n 1 + 864 n 515 ) Z n 4
We have to regard the case Z n 4 = 1 , which is G n G n + 1 4 . The proof process is also analogous, and we leave out the details.
Recalling that Z n 1 + Z n 2 + Z n 3 + Z n 4 = 1 , according to the above discussion, it holds that
D n = D n ( Z n 1 + Z n 2 + Z n 3 + Z n 4 ) = D n 1 + n · U n V n
where for each n, U n = 540 Z n 1 + 720 Z n 2 + 828 Z n 3 + 864 Z n 4 , V n = 191 Z n 1 + 371 Z n 2 + 479 Z n 3 + 515 Z n 4 .
Therefore, by (25)
K f + ( G n ) = K f + ( G 1 ) + t = 1 n 1 D t + t = 1 n 1 ( 637 t + 160 ) = K f + ( G 1 ) + t = 1 n 1 ( q = 1 t 1 ( D q + 1 D q ) + D 1 ) + t = 1 n 1 ( 637 t + 160 ) = K f + ( G 1 ) + t = 1 n 1 q = 1 t 1 ( D q + 1 D q ) + ( n 1 ) D 1 + t = 1 n 1 ( 637 t + 160 ) = K f + ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + ( n 1 ) D 1 + t = 1 n 1 ( 637 t + 160 ) = K f + ( G 1 ) + t = 1 n 1 q = 1 t 1 ( ( q + 1 ) U q + 1 V q + 1 ) + O ( n 2 )
If we replace G u t ( G n ) with K f + ( G n ) in the proof of Theorem 1, the rest of the proof of this theorem is the same as that in the proof of Theorem 1; we thus omit the details.

4. Concluding Remarks

In this paper, we obtain explicit analytical expressions for the variances of Schultz index, multiplicative degree-Kirchhoff index, Gutman index and additive degree-Kirchhoff index of a random cyclooctatetraene chain with n octagons. All of these results will contribute to the study of Schultz index, multiplicative degree-Kirchhoff index, Gutman index and additive degree-Kirchhoff index of graphs. With the continuous development and progress of science, more and more molecules are being discovered and created.
The polygonal chain problem in chemical graph theory has been extensively studied and discussed by researchers. For the variance of some certain indices of a random polygon chain that has n regular polygons, it is feasible to establish exact formulas.
Not only that, through these studies, we can hopefully obtain the variance of the n sided chain graph and some of their physicochemical properties in the near future.

Author Contributions

Conceptualization, C.T., S.T. and X.G.; methodology, C.T.; software, C.T.; validation, C.T. and X.G.; formal analysis, C.T.; investigation, C.T.; resources, S.T.; data curation, C.T.; writing—original draft preparation, C.T.; writing—review and editing, C.T.; visualization, S.T.; supervision, C.T.; project administration, C.T.; funding acquisition, X.G. All authors have read and agreed to the published version of the manuscript.

Funding

The research is partially supported by National Science Foundation of China (Grant No. 12171190) and Natural Science Foundation of Anhui Province (Grant No. 2008085MA01).

Data Availability Statement

Not applicable.

Acknowledgments

The authors are very grateful to the helpful comments and suggestions. The research is partially supported by National Science Foundation of China (Grant No. 12171190) and Natural Science Foundation of Anhui Province (Grant No. 2008085MA01).

Conflicts of Interest

The authors declare no conflict of interest.

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Figure 1. Graph G 2 .
Figure 1. Graph G 2 .
Symmetry 15 01971 g001
Figure 2. The construction of G n + 1 from G n and H n + 1 .
Figure 2. The construction of G n + 1 from G n and H n + 1 .
Symmetry 15 01971 g002
Figure 3. Four ways to attach the new terminal octagon H n + 1 to G n .
Figure 3. Four ways to attach the new terminal octagon H n + 1 to G n .
Symmetry 15 01971 g003
Figure 4. G n G n + 1 1 .
Figure 4. G n G n + 1 1 .
Symmetry 15 01971 g004
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Tao, C.; Tang, S.; Geng, X. Statistical Analyses of a Class of Random Cyclooctatetraene Chain Networks with Respect to Several Topological Properties. Symmetry 2023, 15, 1971. https://doi.org/10.3390/sym15111971

AMA Style

Tao C, Tang S, Geng X. Statistical Analyses of a Class of Random Cyclooctatetraene Chain Networks with Respect to Several Topological Properties. Symmetry. 2023; 15(11):1971. https://doi.org/10.3390/sym15111971

Chicago/Turabian Style

Tao, Chen, Shengjun Tang, and Xianya Geng. 2023. "Statistical Analyses of a Class of Random Cyclooctatetraene Chain Networks with Respect to Several Topological Properties" Symmetry 15, no. 11: 1971. https://doi.org/10.3390/sym15111971

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