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Article

On the Normalized Laplacian Spectrum of the Linear Pentagonal Derivation Chain and Its Application

College of Mathematics and System Sciences, Xinjiang University, Urumqi 830017, China
*
Author to whom correspondence should be addressed.
Axioms 2023, 12(10), 945; https://doi.org/10.3390/axioms12100945
Submission received: 30 August 2023 / Revised: 26 September 2023 / Accepted: 28 September 2023 / Published: 1 October 2023
(This article belongs to the Special Issue Graph Theory and Discrete Applied Mathematics)

Abstract

:
A novel distance function named resistance distance was introduced on the basis of electrical network theory. The resistance distance between any two vertices u and v in graph G is defined to be the effective resistance between them when unit resistors are placed on every edge of G. The degree-Kirchhoff index of G is the sum of the product of resistance distances and degrees between all pairs of vertices of G. In this article, according to the decomposition theorem for the normalized Laplacian polynomial of the linear pentagonal derivation chain Q P n , the normalize Laplacian spectrum of Q P n is determined. Combining with the relationship between the roots and the coefficients of the characteristic polynomials, the explicit closed-form formulas for degree-Kirchhoff index and the number of spanning trees of Q P n can be obtained, respectively. Moreover, we also obtain the Gutman index of Q P n and we discovery that the degree-Kirchhoff index of Q P n is almost half of its Gutman index.

1. Introduction

Throughout this paper, we handle a simple, finite, and undirected graph. Let G = ( V ( G ) , E ( G ) ) be a graph with vertex set V ( G ) = { v 1 , v 2 , , v n } and edge set E ( G ) . For v i V ( G ) , let N G ( v i ) be the set of neighbors of v i in G. In particular, d i = | N G ( v i ) | is the degree of v i in G. The adjacency matrix of G, written as A ( G ) , is an n × n matrix whose ( i , j ) -entry is 1 if v i v j E ( G ) or 0 otherwise. The Laplacian matrix L ( G ) = D ( G ) A ( G ) , where D ( G ) = d i a g ( d 1 , d 2 , , d n ) is the diagonal matrix of G whose diagonal entry d i is the degree of v i for 1 i n .
The normalized Laplacian matrix [1] of a graph G, L ( G ) , is defined to be
L ( G ) = I D 1 2 ( D 1 A ) D 1 2 = D 1 2 L ( G ) D 1 2 ,
with the convention that D ( G ) 1 ( i , i ) = 0 if d i = 0 . Since the normalized Laplacian matrix is consistent with the eigenvalues in spectral geometry and random walks [1], it has attracted more and more researchers’ attention. From the definition of L ( G ) , it is easy to obtain that:
( L ( G ) ) i j = 1 , if i = j ; 1 d i d j , if i j and v i is   adjacent   to v j ; 0 , otherwise ,
where ( L ( G ) ) i j denotes the ( i , j ) -entry of L ( G ) .
For an n × n matrix M, we denote the characteristic polynomial det ( x I n M ) of M by Φ M ( x ) , where I n is the identity matrix of order n. In particular, for a graph G, Φ L ( G ) ( x ) (respectively, Φ L ( G ) ( x ) ) is the Laplacian (respectively, normalized Laplacian) characteristic polynomial of G, and its roots are the Laplacian (respectively, normalized Laplacian) eigenvalues of G. The collection of eigenvalues of L ( G ) (respectively, L ( G ) ) together with their multiplicities are called the L-spectrum (respectively, L -spectrum) of G.
For a graph G, the distance between vertices v i and v j on G is defined as the length of the shortest path between the two vertices, denoted d i j . One famous distance based parameter called the Wiener index [2], which is defined as the sum of the distances between all the vertices on the graph, was given by W ( G ) = i < j d i j . For more studies on the Wiener index, one may be referred to [3,4,5,6,7,8]. In 1994, Gutman presented an index based on degree and distance of vertex, Gutman index [9], which is G u t ( G ) = i < j d i d j d i j . He also showed that when G is an n-order tree, the close relationship between the Wiener index and the Gutman index is G u t ( G ) = 4 W ( G ) ( 2 n 1 ) ( n 1 ) .
Based on electrical network theory, Klein and Randić [10] proposed a novel distance function named resistance distance. Let G be a connected graph, and the resistance distance between vertices v i and v j , denoted by r i j , is defined as the effective resistance distance between vertices v i and v j in the electrical network obtained by replacing each edge in G with a unit resistance. The resistance distance is a better indicator of the connection between two vertices than the distance. In fact, the resistance distance parameter reflects the intrinsic properties of the graph and has many applications in chemistry [11,12].
One famous parameter called the Kirchhoff index [10], defined as the sum of resistance distances in a simple connected graph, was given by K f ( G ) = i < j r i j . In 1993, Klein and Randić [10] proved that r i j d i j and K f ( G ) W ( G ) with equality if and only if G is a tree. The intrinsic correlation between the Kirchhoff index and the Laplacian eigenvalues of graph G is shown, independently, by Gutman and Mohar [13] and Zhu et al. [14] as
K f ( G ) = i < j r i j = n i = 2 n 1 μ i ,
where n is the number of vertices of the graph G and 0 = μ 1 < μ 2 μ n are the eigenvalues of L ( G ) .
As an analogue to the Gutman index, Chen and Zhang [15] presented another graph parameter, the degree-Kirchhoff index  K f * ( G ) = i < j d i d j r i j . Meanwhile, authors [15] proved that the degree-Kirchhoff index is closely related to the corresponding normalized Laplacian spectrum. Many researchers devote themselves to the study of normalized Laplacian spectrum and the degree-Kirchhoff index of some classes of graphs. One may be referred to those in [16,17,18,19,20,21,22].
As a structured descriptor of chemical molecular graphs, the topological index can reflect some structural characteristics of compounds. Like Kirchhoff index, degree-Kirchhoff index is also a topological index. Unfortunately, it is difficult to compute resistant distance and degree-Kirchhoff index in a graph from their computational complexity. Therefore, it is necessary to find a explicit closed-form formulas for the degree-Kirchhoff index. In fact, the degree-Kirchhoff index is difficult to calculate for general graphs, but it is computable for some graphs with good periodicity and good symmetry. Huang et al. studied the degree-Kirchhoff index of some graphs with a good structure, such as linear polyomino chain [23] and linear hexagonal chain [24]. In addition, there are also some studies on the normalized Laplacian spectrum and the degree-Kirchhoff index of phenylene chains [25,26].
The number of spanning trees of a graph (network) is an important quantity to evaluate the reliability of the graph [27]. Therefore, studying the number of spanning trees of graphs has a very important theoretical and practical significance.
Hexagonal systems are very important in theoretical chemistry because they are natural graphical representations of benzene molecular structures. In recent years, researchers have worked to study the topological index of hexagonal systems [4,28]. The linear pentagonal derivation chain studied in this paper is related to the hexagonal systems. A linear pentagonal chain of length n, denoted by P n , is made up of 2 n pentagons, where every two pentagons with two sides can be seen as a hexagon with one vertex and two sides. Then the linear pentagonal derivation chain, denoted by Q P n , is the graph obtained by attaching four-membered rings to each hexagon composed of two pentagons of P n , as showed in Figure 1. It is not difficult to verify that | V ( Q P n ) | = 7 n + 2 , | E ( Q P n ) | = 10 n + 1 .
The explicit closed-form formulas for Kirchhoff index and the number of spanning trees of the linear pentagonal derivation chain Q P n have been derived from the Laplacian spectrum [29]. Motivated by the above works, we consider the degree-Kirchhoff index and the number of spanning trees of linear pentagonal derivation chain in terms of the normalized Laplacian spectrum. Different from the method in [29], in this paper, we solve the number of spanning trees according to the normalized Laplacian spectrum, which gives a new way for calculating the number of spanning trees of Q P n .
In this article, according to the decomposition theorem for the normalized Laplacian polynomial of the linear pentagonal derivation chain Q P n , the normalized Laplacian spectrum of Q P n is determined. Combining with the relationship between the roots and the coefficients of the characteristic polynomials, the explicit closed-form formulas for degree-Kirchhoff index and the number of spanning trees of Q P n can be obtained, respectively. Meanwhile, we also get the Gutman index of Q P n . For a general graph G, the ratio K f ( G ) W ( G ) is not closely related to K f * ( G ) G u t ( G ) . However, we are surprised to discovery that for Q P n both K f ( Q P n ) W ( Q P n ) 1 2 [29] and K f * ( Q P n ) G u t ( Q P n ) 1 2 (based on our obtained results) as n .

2. Preliminaries

In this section, we will give some notations and terminologies and some known results that will be used in our following section.
An automorphism of G is a permutation π of V ( G ) , with the property that v i v j is an edge of G if and only if π ( v i ) π ( v j ) is an edge of G.
Suppose we mark the vertices of Q P n as shown in Figure 1 and denote V 0 = { 1 , 2 , , n } , V 1 = { 1 , 2 , , 3 n + 1 } , V 2 = { 1 , 2 , , ( 3 n + 1 ) } . Then
π = ( 1 ) ( 2 ) ( n ) ( 1 , 1 ) ( 2 , 2 ) ( 3 n + 1 , ( 3 n + 1 ) )
is an automorphism of Q P n . For convenience, we abbreviate L ( Q P n ) to L . By a suitable arrangement of vertices in Q P n , the normalized Laplacian matrix L can be written as the following block matrix
L = L V 00 L V 01 L V 02 L V 10 L V 11 L V 12 L V 20 L V 21 L V 22 ,
where L V i j is the submatrix composed by rows corresponding to vertices in V i and columns corresponding to vertices in V j for i , j = 0 , 1 , 2 .
Let
T = I n 0 0 0 1 2 I 3 n + 1 1 2 I 3 n + 1 0 1 2 I 3 n + 1 1 2 I 3 n + 1
be the block matrix so that the blocks have the same dimension as the corresponding blocks in L . Note that L V 01 = L V 02 , L V 10 = L V 20 , L V 11 = L V 22 and L V 12 = L V 21 . From the unitary transformation T L T , we obtain
T L T = L A 0 0 L S ,
where
L A = L V 00 2 L V 01 2 L V 10 L V 11 + L V 12 , L S = L V 22 L V 12 .
According to the above analysis process, Huang et al. [24] derived the decomposition theorem of normalized Laplacian characteristic polynomial of G below.
Lemma 1
([24]). Suppose L , L A and L S are defined as above. Then the normalized Laplacian characteristic polynomial of Q P n is as follows
Φ L ( x ) = Φ L A ( x ) Φ L S ( x ) ,
where Φ L ( x ) , Φ L A ( x ) and Φ L S ( x ) are characteristic polynomials of L , L A and L S , respectively.
Lemma 2
([30]). Let M 1 , M 2 , M 3 , M 4 be respectively p × p , p × q , q × p , q × q matrices with M 1 and M 4 being invertible. Then
det M 1 M 2 M 3 M 4 = det ( M 1 ) · det ( M 4 M 3 M 1 1 M 2 ) = det ( M 4 ) · det ( M 1 M 2 M 4 1 M 3 ) ,
where M 4 M 3 M 1 1 M 2 and M 1 M 2 M 4 1 M 3 are called the Schur complements of M 1 and M 4 , respectively.
Lemma 3.
Suppose G is a connected graph of order n with m edges, and { 0 = λ 1 < λ 2 λ n } is the spectrum on the normalized Laplacian matrix L of G. Denote by d i is the degree of v i of G, i = 1 , 2 , , n . Then
(i)
[15] The degree-Kirchhoff index of G is K f * ( G ) = 2 m i = 2 n 1 λ i ;
(ii)
[1] The number τ ( G ) of spanning trees of G is τ ( G ) = i = 1 n d i k = 2 n λ k 2 m .

3. The Normalized Laplacian Spectrum of QP n

In this part, from Lemma 1, we first derive the normalized Laplacian eigenvalues of linear pentagonal derivation chain Q P n . Then we present a complete description of the sum of the normalized Laplacian eigenvalues’ reciprocals and the product of the normalized Laplacian eigenvalues which will be used in getting the degree-Kirchhoff index and the number of spanning trees of Q P n , respectively.
Given an n × n square matrix M, then we will use M [ i , j , , k ] to denote the sub-matrix obtained by deleting the i-th, j-th, , k-th rows and corresponding columns of M. In view of (1), L V 00 , L V 01 , L V 12 and L V 11 are given as follows:
L V 00 = I n , L V 01 = 0 1 6 0 0 0 0 0 0 0 0 0 0 1 6 0 0 0 0 0 0 0 0 1 6 0 0 n × ( 3 n + 1 ) ,
L V 11 = 1 1 6 0 0 0 0 1 6 1 1 3 0 0 0 0 1 3 1 0 0 0 0 0 0 1 1 3 0 0 0 0 1 3 1 1 6 0 0 0 0 1 6 1 ( 3 n + 1 ) × ( 3 n + 1 ) ,
L V 12 = 1 2 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 3 0 0 0 0 0 0 0 0 1 3 0 0 0 0 0 0 0 0 1 3 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 1 3 0 0 0 0 0 0 0 0 1 2 ( 3 n + 1 ) × ( 3 n + 1 ) .
Since L V 10 = L V 01 T , L V 22 = L V 11 , and L A = L V 00 2 L V 01 2 L V 10 L V 11 + L V 12 , L S = L V 22 L V 12 (see (2)),
we have
L A = 1 0 0 0 1 3 0 0 0 0 0 0 0 1 0 0 0 0 0 1 3 0 0 0 0 0 1 0 0 0 0 0 1 3 0 0 0 0 0 1 2 1 6 0 0 0 0 0 0 1 3 0 0 1 6 1 1 3 0 0 0 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 0 0 0 0 1 3 1 0 0 0 0 0 1 3 0 0 0 0 0 1 1 3 0 0 0 0 0 0 0 0 0 1 3 2 3 1 6 0 0 0 0 0 0 0 0 0 1 6 1 2 ( 4 n + 1 ) × ( 4 n + 1 ) ,
and
L S = 3 2 1 6 0 0 0 0 0 0 0 0 1 6 1 1 3 0 0 0 0 0 0 0 0 1 3 4 3 1 3 0 0 0 0 0 0 0 0 1 3 4 3 1 3 0 0 0 0 0 0 0 0 1 3 1 1 3 0 0 0 0 0 0 0 0 1 3 4 3 0 0 0 0 0 0 0 0 0 0 4 3 1 3 0 0 0 0 0 0 0 0 1 3 1 1 3 0 0 0 0 0 0 0 0 1 3 4 3 1 6 0 0 0 0 0 0 0 0 1 6 3 2 ( 3 n + 1 ) × ( 3 n + 1 ) .
It is easy to see that the normalized Laplacian spectrum of Q P n consists of eigenvalues of L A and L S from Lemma 1. Now, suppose that the eigenvalues of L A and L S are, respectively, denoted by α 0 α 1 α 4 n and β 1 β 2 β 3 n + 1 . Note that L ( Q P n ) is positive semi-definite (see [1]). Hence, the eigenvalues of L ( Q P n ) are non-negative. That is to say, L A and L S are positive semi-definite. And then, it is not difficult to verify that α 0 = 0 , α i > 0 ( i = 1 , 2 , , 4 n ) and β j > 0 ( j = 1 , 2 , , 3 n + 1 ) .

4. Degree-Kirchhoff Index and the Number of Spanning Trees of QP n

In this section, we first introduce the following lemma which is a direct result of Lemma 3(i). Note that | E ( Q P n ) | = 10 n + 1 .
Lemma 4.
Suppose Q P n is a linear pentagonal derivation chain with length n. Then we have
K f * ( Q P n ) = 2 ( 10 n + 1 ) ( i = 1 4 n 1 α i + j = 1 3 n + 1 1 β j ) ,
where 0 = α 0 < α 1 α 4 n and 0 < β 1 β 2 β 3 n + 1 are eigenvalues of L A and L S , respectively.
Lemma 5.
Let 0 = α 0 < α 1 α 4 n be eigenvalues of L A . Then
i = 1 4 n 1 α i = 50 n 3 + 25 n 2 + n 10 n + 1 .
Proof.
According to the relationship between the roots and coefficients of Φ L A ( x ) , i = 1 4 n 1 α i are obtained respectively. Since Φ L A ( x ) = x 4 n + 1 + a 1 x 4 n + + a 4 n 1 x 2 + a 4 n x with a 4 n 0 and α 1 , α 2 , , α 4 n are the roots of Φ L A ( x ) = 0 . By Vieta’s Formula [31], we get
i = 1 4 n 1 α i = i = 1 4 n i = 1 , i i 4 n α i i = 1 4 n α i = a 4 n 1 a 4 n .
In the subsequent of this part, it suffices to determine a 4 n and a 4 n 1 in Equation (3), respectively.
Claim 1.
a 4 n = 10 n + 1 12 1 3 3 n 2 .
Proof.
One can see that the number a 4 n ( = ( 1 ) 4 n a 4 n ) is the sum of the determinants obtained by deleting the i-th row and corresponding column of L A for i = 1 , 2 , , 4 n + 1 (see also in [32]), that is
a 4 n = i = 1 4 n + 1 det L A [ i ] .
Case 1.  1 i n . According to the structure of L A (see details in (2)), deleting the i-th row and corresponding column of L A is equivalent to deleting the i-th row and corresponding column of I n , the i-th row of 2 L V 01 and the i-th column of 2 L V 10 . We mark the resulting blocks of L A [ i ] , by I n 1 , B ( n 1 ) × ( 3 n + 1 ) , B ( n 1 ) × ( 3 n + 1 ) T , C ( 3 n + 1 ) × ( 3 n + 1 ) , respectively. Then applying Lemma 2 to the resulting matrix, one has
det L A [ i ] = I n 1 B ( n 1 ) × ( 3 n + 1 ) B ( n 1 ) × ( 3 n + 1 ) T C ( 3 n + 1 ) × ( 3 n + 1 ) = I n 1 0 0 C ( 3 n + 1 ) × ( 3 n + 1 ) B ( n 1 ) × ( 3 n + 1 ) T B ( n 1 ) × ( 3 n + 1 ) = C ( 3 n + 1 ) × ( 3 n + 1 ) B ( n 1 ) × ( 3 n + 1 ) T B ( n 1 ) × ( 3 n + 1 ) ,
where
C B T B = 1 2 1 6 0 0 0 0 0 0 1 6 2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 6 0 0 0 0 0 0 1 6 1 2 ( 3 n + 1 ) × ( 3 n + 1 ) ,
and there’s only one 1 on the diagonal in the ( 3 i 1 ) -th row of C B T B for 1 i n . By a direct calculation, we have det ( C 1 2 B T B ) = 1 4 1 3 3 n 1 . Therefore, for 1 i n , we obtain
det L A [ i ] = 1 4 1 3 3 n 1 .
Case 2.  n + 1 i 4 n + 1 . In this case, according to the structure of L A , deleting the i-th row and corresponding column of L A is equal to deleting the ( i n ) -th row and corresponding column of L V 11 + L V 12 , the ( i n ) -th column of 2 L V 01 and the ( i n ) -th row of 2 L V 10 . Expressing the resulting blocks, respectively, as I n , B n × 3 n , B n × 3 n T , C 3 n × 3 n . Then by Lemma 2, we obtain
det L A [ i ] = I n B n × 3 n B n × 3 n T C 3 n × 3 n = I n 0 0 C 3 n × 3 n B n × 3 n T B n × 3 n = C 3 n × 3 n B n × 3 n T B n × 3 n ,
where
C B T B = E ( i n 1 ) × ( i n 1 ) 0 0 F ( 4 n + 1 i ) × ( 4 n + 1 i ) 3 n × 3 n ,
and the E , F are as follows:
E = 1 2 1 6 0 0 0 0 1 6 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 ( i n 1 ) × ( i n 1 ) , F = 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 6 0 0 0 0 1 6 1 2 ( 4 n + 1 i ) × ( 4 n + 1 i ) .
By a direct calculation, we get
det L A [ i ] = det ( C B T B ) = 1 2 1 3 3 n 1 , i = n + 1 , i = 4 n + 1 ; 1 4 1 3 3 n 2 , n + 2 i 4 n .
Together with (4)–(6) we have
a 4 n = i = 1 4 n + 1 det L A [ i ] = i = 1 n det L A [ i ] + i = n + 1 4 n + 1 det L A [ i ] = 10 n + 1 12 1 3 3 n 2 .
Claim 2.
a 4 n 1 = 50 n 3 + 25 n 2 + n 36 1 3 3 n 3 .
Proof.
One can see that a 4 n 1 ( = ( 1 ) 4 n 1 a 4 n 1 ) is the sum of the determinants of the resulting matrix by deleting the i-th row, i-th column and the j-th row, j-th column for some 1 i < j 4 n + 1 in L A . That is
a 4 n 1 = 1 i < j 4 n + 1 det L A [ i , j ] .
Case 1.  1 i < j n . In this case, deleting the i-th and j-th rows and corresponding columns of L A is to deleting the i-th and j-th rows and corresponding columns of I n , the i-th and j-th rows of 2 L V 01 and the i-th and j-th columns of 2 L V 10 . Denote the resulting blocks, respectively, as I n 2 , B ( n 2 ) × ( 3 n + 1 ) , B ( n 2 ) × ( 3 n + 1 ) T and C ( 3 n + 1 ) × ( 3 n + 1 ) and apply Lemma 2 to the resulting matrix. Then we have
det L A [ i , j ] = I n 2 B ( n 2 ) × ( 3 n + 1 ) B ( n 2 ) × ( 3 n + 1 ) T C ( 3 n + 1 ) × ( 3 n + 1 ) = | C B T B | ,
where
C B T B = 1 2 1 6 0 0 0 0 0 0 0 1 6 2 3 1 3 0 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 1 3 1 0 0 0 0 0 0 0 0 0 1 1 3 0 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 1 3 2 3 1 6 0 0 0 0 0 0 0 1 6 1 2 ( 3 n + 1 ) × ( 3 n + 1 ) ,
and there exists one 1 on the diagonal in the ( 3 i 1 ) -th and ( 3 j 1 ) -th rows of C B T B for 1 i < j n , respectively.
By a direct computing, we have
det L A [ i , j ] = | C B T B | = 1 4 1 3 3 n 1 ( 3 j 3 i + 2 ) , 1 i < j n .
Case 2.  n + 1 i < j 4 n + 1 . In this case, deleting the i-th and j-th rows and corresponding columns of L A is to deleting the ( i n ) -th and ( j n ) -th rows and corresponding columns of L V 11 + L V 12 , the ( i n ) -th and ( j n ) -th columns of 2 L V 01 and the ( i n ) -th and ( j n ) -th rows of 2 L V 10 . Similarly, denote the resulting blocks, respectively, as C ( 3 n 1 ) × ( 3 n 1 ) , B n × ( 3 n 1 ) , B n × ( 3 n 1 ) T and I n . Then by Lemma 2 to the resulting matrix, we have
det L A [ i , j ] = I n B n × ( 3 n 1 ) B n × ( 3 n 1 ) T C ( 3 n 1 ) × ( 3 n 1 ) = | C B T B | ,
where
C B T B = E ( i n 1 ) × ( i n 1 ) 0 0 0 F ( j i 1 ) × ( j i 1 ) 0 0 0 G ( 4 n + 1 j ) × ( 4 n + 1 j ) ( 3 n 1 ) × ( 3 n 1 ) ,
and the E , F , G are as follows:
E = 1 2 1 6 0 0 0 0 1 6 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 ( i n 1 ) × ( i n 1 ) , F = 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 ( j i 1 ) × ( j i 1 ) ,
G = 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 6 0 0 0 0 1 6 1 2 ( 4 n + 1 j ) × ( 4 n + 1 j ) .
By a direct calculation, we have
det L A [ i , j ] = det ( C B T B ) = 1 4 ( j i ) 1 3 3 n 3 , n + 2 i < j 4 n ; 1 2 ( j n 1 ) 1 3 3 n 2 , i = n + 1 , n + 2 j 4 n ; 1 2 ( 4 n i + 1 ) 1 3 3 n 2 , n + 2 i 4 n , j = 4 n + 1 ; 3 n 1 3 3 n 1 , i = n + 1 , j = 4 n + 1 .
Case 3.  1 i n , n + 1 j 4 n + 1 . By using a similar method, deleting the i-th and j-th rows and corresponding columns of L A is to deleting the i-th row and i-th column of I n , the ( j n ) -th row and ( j n ) -th column of L V 11 + L V 12 , the i-th row and ( j n ) -th column of 2 L V 01 and the ( j n ) -th row and i-th column of 2 L V 10 . We denote the resulting blocks, respectively, as I ( n 1 ) , C 3 n × 3 n , B ( n 1 ) × 3 n and B ( n 1 ) × 3 n T and apply Lemma 2 to the resulting matrix. Then we get
det L A [ i , j ] = I n 1 B ( n 1 ) × 3 n B ( n 1 ) × 3 n T C 3 n × 3 n = | C B T B | .
Subcase 3.1. If 1 i n , j = n + 1 , then the matrix C B T B is
2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 6 0 0 0 0 0 0 1 6 1 2 3 n × 3 n ,
and there is only one 1 on the diagonal in the ( 3 i 2 ) -th row of C B T B for 1 i n .
Subcase 3.2. If 1 i n , j = 4 n + 1 , then the matrix C B T B is
1 2 1 6 0 0 0 0 0 0 1 6 2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 0 2 3 1 3 0 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 0 1 3 2 3 3 n × 3 n ,
and there is only one 1 on the diagonal in the ( 3 i 1 ) -th row of C B T B for 1 i n .
Subcase 3.3. If 1 i n , n + 2 j 4 n , then the matrix
C B T B = E ( j n 1 ) × ( j n 1 ) 0 0 F ( 4 n + 1 j ) × ( 4 n + 1 j ) 3 n × 3 n ,
where
E = 1 2 1 6 0 0 0 0 0 1 6 2 3 1 3 0 0 0 0 0 1 3 2 3 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 2 3 1 3 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 1 3 2 3 ( j n 1 ) × ( j n 1 ) ,
F = 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 6 0 0 0 0 1 6 1 2 ( 4 n + 1 j ) × ( 4 n + 1 j ) ,
and there is only one 1 in the ( 3 i 1 ) -th row of E, or
C B T B = E ( 3 i 2 ) × ( 3 i 2 ) 0 0 F ( 3 n 3 i + 2 ) × ( 3 n 3 i + 2 ) 3 n × 3 n ,
where
E = 1 2 1 6 0 0 0 0 1 6 2 3 1 3 0 0 0 0 1 3 2 3 0 0 0 0 0 0 2 3 1 3 0 0 0 0 1 3 2 3 1 3 0 0 0 0 1 3 2 3 ( 3 i 2 ) × ( 3 i 2 ) ,
F = 2 3 1 3 0 0 0 0 0 1 3 2 3 1 3 0 0 0 0 0 1 3 2 3 0 0 0 0 0 0 0 1 0 0 0 0 0 0 0 2 3 1 3 0 0 0 0 0 1 3 2 3 1 6 0 0 0 0 0 1 6 1 2 ( 3 n 3 i + 2 ) × ( 3 n 3 i + 2 ) .
Hence, for 1 i n ,
det L A [ i , j ] = det ( C B T B ) = 1 2 ( 3 i 1 ) 1 3 3 n 1 , j = n + 1 ; 1 2 ( n i + 1 ) 1 3 3 n 2 , j = 4 n + 1 ; 1 4 ( | j n 3 i + 1 | + 1 ) 1 3 3 n 2 , n + 2 j 4 n .
Combining with (7)–(10), we obtain
a 4 n 1 = 1 i < j 4 n + 1 det L A [ i , j ] = 1 i < j n det L A [ i , j ] + n + 1 i < j 4 n + 1 det L A [ i , j ] + 1 i n , n + 1 j 4 n + 1 det L A [ i , j ] = n 3 + 2 n 2 3 n 8 1 3 3 n 1 + 27 n 3 + 9 n 2 + 2 n 24 1 3 3 n 3 + 18 n 3 + 21 n 2 n 72 1 3 3 n 3 = 50 n 3 + 25 n 2 + n 36 1 3 3 n 3 .
Finally, substituting Claims 1 and 2 into (3), Lemma 5 holds directly. □
Lemma 6.
Let 0 < β 1 β 2 β 3 n + 1 be eigenvalues of L S . Then
j = 1 3 n + 1 1 β j = [ ( 15,429 1365 + 569,985 ) n + 3356 1365 + 124,042 ] ( 37 + 1365 ) n 1 [ ( 5135 1365 + 189,735 ) ( 37 + 1365 ) n 1 + ( 5135 1365 189,735 ) ( 37 1365 ) n 1 ] + [ ( 15,429 1365 569,985 ) n + 3356 1365 124,042 ] ( 37 1365 ) n 1 [ ( 5135 1365 + 189,735 ) ( 37 + 1365 ) n 1 + ( 5135 1365 189,735 ) ( 37 1365 ) n 1 ] .
Proof.
Similarly, for Φ L S ( x ) = x 3 n + 1 + b 1 x 3 n + + b 3 n 1 x 2 + b 3 n x + b 3 n + 1 with b 3 n + 1 0 , we know β 1 , β 2 , , β 3 n + 1 are the roots of the Φ L S ( x ) = 0 . Applying Vieta’s Formulas [31], we get
j = 1 3 n + 1 1 β j = j = 1 3 n + 1 j = 1 , j j 3 n + 1 β j j = 1 3 n + 1 β j = ( 1 ) 3 n b 3 n det L S .
In order to determine ( 1 ) 3 n b 3 n and det L S in (11), we consider the k order principal submatrix W k consisting of the first k rows and the first k columns of L S , k = 1 , 2 , , 3 n + 1 . Put w k : = det W k . Let’s prove the following fact first.
Fact 1. For 7 k 3 n , w k satisfy the recurrence
w k = 37 27 w k 3 1 729 w k 6 ,
with the initial conditions w 1 = 3 2 , w 2 = 4 3 , w 3 = 29 18 , w 4 = 54 27 , w 5 = 295 162 , and w 6 = 536 243 .
Proof.
By a direct calculation, we obtain that w 1 = 3 2 , w 2 = 4 3 , w 3 = 29 18 , w 4 = 54 27 , w 5 = 295 162 , and w 6 = 536 243 , expanding det W k with regard to its last row, we have
w 3 i + 2 = w 3 i + 1 1 9 w 3 i , i = 1 , 2 , , n 1 ; w 3 i = 4 3 w 3 i 1 1 9 w 3 i 2 , i = 1 , 2 , , n ; w 3 i + 1 = 4 3 w 3 i 1 9 w 3 i 1 , i = 1 , 2 , , n 1 .
For 0 i n 1 , let e i = w 3 i + 2 , for 1 i n , let f i = w 3 i and for 0 i n 1 , let g i = w 3 i + 1 . Then
e i = g i 1 9 f i f i = 4 3 e i 1 1 9 g i 1 g i = 4 3 f i 1 9 e i 1 .
Hence, e i = 37 27 e i 1 1 729 e i 2 , f i = 37 27 f i 1 1 729 f i 2 and g i = 37 27 g i 1 1 729 g i 2 . Therefore, for 7 k 3 n , w k satisfies the recurrence
w k = 37 27 w k 3 1 729 w k 6 ,
where w 1 = 3 2 , w 2 = 4 3 , w 3 = 29 18 , w 4 = 54 27 , w 5 = 295 162 , and w 6 = 536 243 .
Claim 3.
det L S = 79 72 + 973 24 1365 37 + 1365 54 n 1 + 79 72 973 24 1365 37 1365 54 n 1 .
Proof.
By Fact 1, the characteristic equations of e i is x 2 = 37 27 x 1 729 , whose roots are x 1 = 37 + 1365 54 , x 2 = 37 1365 54 . Suppose that e i = y 1 ( 37 + 1365 54 ) i + y 2 ( 37 1365 54 ) i . Then according to the initial conditions e 0 = w 2 = 4 3 , e 1 = w 5 = 295 162 , we have the systems of equations
y 1 + y 2 = 4 3 y 1 37 + 1365 54 + y 2 37 1365 54 = 295 162 .
The only solution of this system of equations is y 1 = 2 3 + 49 2 1365 , y 2 = 2 3 49 2 1365 , so
e i = ( 2 3 + 49 2 1365 ) ( 37 + 1365 54 ) i + ( 2 3 49 2 1365 ) ( 37 1365 54 ) i .
By using a similar method, we can get f i and g i below
f i = 3 4 + 63 4 1365 37 + 1365 54 i + 3 4 63 4 1365 37 1365 54 i g i = 3 4 + 105 4 1365 37 + 1365 54 i + 3 4 105 4 1365 37 1365 54 i .
Since w 3 i = f i , w 3 i + 1 = g i and w 3 i + 2 = e i , we get
w i = 3 4 + 63 4 1365 37 + 1365 54 i 3 + 3 4 63 4 1365 37 1365 54 i 3 , i f i 0 ( mod 3 ) 3 4 + 105 4 1365 37 + 1365 54 i 1 3 + 3 4 105 4 1365 37 1365 54 i 1 3 , i f i 1 ( mod 3 ) 2 3 + 49 2 1365 37 + 1365 54 i 2 3 + 2 3 49 2 1365 37 1365 54 i 2 3 , i f i 2 ( mod 3 ) .
By expansion-formula, we can see det L S with respect to its last row as
det L S = 3 2 det W 3 n 1 6 det W 3 n 1 = 3 2 w 3 n 1 6 w 3 n 1 = 3 2 3 4 + 63 4 1365 37 + 1365 54 n + 3 4 63 4 1365 37 1365 54 n 1 6 2 3 + 49 2 1365 37 + 1365 54 n 1 + 2 3 49 2 1365 37 1365 54 n 1 = 79 72 + 973 24 1365 37 + 1365 54 n 1 + 79 72 973 24 1365 37 1365 54 n 1 .
It completes the proof of Claim 3. □
Claim 4.
( 1 ) 3 n b 3 n = 15,429 n + 3356 4680 + 569,985 n + 124,042 4680 1365 37 + 1365 54 n 1 + 15,429 n + 3356 4680 569,985 n + 124,042 4680 1365 37 1365 54 n 1 .
Proof.
Since ( 1 ) 3 n b 3 n is the sum of all those principal minors of L S each of which is of size 3 n × 3 n , we have
( 1 ) 3 n b 3 n = i = 1 3 n + 1 det L S [ i ] = i = 1 3 n + 1 W i 1 0 0 H = i = 1 3 n + 1 det W i 1 det H .
Note that H is a ( 3 n + 1 i ) × ( 3 n + 1 i ) matrix obtain from L S deleting the first i rows and corresponding columns. Let q 3 n + 1 i = det H . Then we get q i = 37 27 q i 3 1 729 q i 6 , where q 1 = 3 2 , q 2 = 11 6 , q 3 = 5 3 , q 4 = 109 54 , q 5 = 203 81 , q 6 = 1109 486 . Thus
q l = 3 4 + 69 4 1365 37 + 1365 54 l 3 + 3 4 69 4 1365 37 1365 54 l 3 , i f l 0 ( mod 3 ) 3 4 + 107 4 1365 37 + 1365 54 l 1 3 + 3 4 107 4 1365 37 1365 54 l 1 3 , i f l 1 ( mod 3 ) 11 12 + 135 4 1365 37 + 1365 54 l 2 3 + 11 12 135 4 1365 37 1365 54 l 2 3 , i f l 2 ( mod 3 ) .
Therefore, by (13),
( 1 ) 3 n b 3 n = i = 1 3 n + 1 w i 1 q 3 n + 1 i = i = 0 3 n w i q 3 n i = l = 0 n w 3 l q 3 n 3 l + l = 0 n 1 w 3 l + 1 q 3 n ( 3 l + 1 ) + l = 0 n 1 w 3 l + 2 q 3 n ( 3 l + 2 ) .
Combining (12) with (14), we know
l = 0 n w 3 l q 3 n 3 l = l = 1 n 1 w 3 l q 3 n 3 l + w 0 q 3 n + q 0 w 3 n = l = 1 n 1 3 4 + 63 4 1365 37 + 1365 54 l + 3 4 63 4 1365 37 1365 54 l · 3 4 + 69 4 1365 37 + 1365 54 n l + 3 4 69 4 1365 37 1365 54 n l + 3 2 + 132 4 1365 37 + 1365 54 n + 3 2 132 4 1365 37 1365 54 n = 369 n + 195 520 + 12,870 n + 11283 520 1365 37 + 1365 54 n + 369 n + 195 520 12,870 n + 11283 520 1365 37 1365 54 n ,
l = 0 n 1 w 3 l + 1 q 3 n ( 3 l + 1 ) = l = 0 n 1 3 4 + 105 4 1365 37 + 1365 54 l + 3 4 105 4 1365 37 1365 54 l · 11 12 + 135 4 1365 37 + 1365 54 n l 1 + 11 12 135 4 1365 37 1365 54 n l 1 = 139 n + 4 104 + 5135 n + 148 104 1365 37 + 1365 54 n 1 + 139 n + 4 104 5135 n + 148 104 1365 37 1365 54 n 1 ,
and
l = 0 n 1 w 3 l + 2 q 3 n ( 3 l + 2 ) = l = 0 n 1 2 3 + 49 2 1365 37 + 1365 54 l + 2 3 49 2 1365 37 1365 54 l · 3 4 + 107 4 1365 37 + 1365 54 n l 1 + 3 4 107 4 1365 37 1365 54 n l 1 = 1529 n + 31 1560 + 56 , 485 n + 1147 1560 1365 37 + 1365 54 n 1 + 1529 n + 31 1560 56,485 n + 1147 1560 1365 37 1365 54 n 1 .
Hence, putting (16)–(18) into (15), Claim 4 follows immediately. □
In view of (11) and Claims 3 and 4, Lemma 6 holds directly. □
Note that | E ( Q P n ) | = 10 n + 1 . Substituting Lemmas 5 and 6 into Lemma 4, we can easily obtain the following main result.
Theorem 1.
Suppose Q P n is a linear pentagonal derivation chain with length n. Then
K f * ( Q P n ) = 2 ( 10 n + 1 ) ( a 4 n 1 a 4 n + ( 1 ) 3 n b 3 n det L S ) = 100 n 3 + 50 n 2 + 2 n + ( 20 n + 2 ) [ ( 15,429 1365 + 569,985 ) n + 3356 1365 + 124,042 ] ( 37 + 1365 ) n 1 [ ( 5135 1365 + 189,735 ) ( 37 + 1365 ) n 1 + ( 5135 1365 189,735 ) ( 37 1365 ) n 1 ] + ( 20 n + 2 ) [ ( 15,429 1365 569,985 ) n + 3356 1365 124,042 ] ( 37 1365 ) n 1 [ ( 5135 1365 + 189,735 ) ( 37 + 1365 ) n 1 + ( 5135 1365 189,735 ) ( 37 1365 ) n 1 ] .
According to Theorem 1, we can have the degree-Kirchhoff indices of linear pentagonal derivation chains from Q P 1 to Q P 40 , as shown in Table 1.
Now, we consider the explicit closed-form formula of the number of spanning trees of Q P n . Note that
i = 1 7 n + 2 d i ( Q P n ) = 2 n + 4 · 3 6 n 2 , | E ( Q P n ) | = 10 n + 1 .
Based on Claims 1, 3 and Lemma 3, we can get the same results as the Theorem 3 [29], which further proves that the result of our calculation (Theorem 2) is correct.
Theorem 2.
Let Q P n denote a linear pentagonal derivation chain with length n. Then
τ ( Q P n ) = 2 n 1 79 2 + 2919 2 1365 37 + 1365 2 n 1 + 79 2 2919 2 1365 37 1365 2 n 1 .

5. A Relation between the Gutman Index and Degree-Kirchhoff of QP n

At the end of this paper, we calculate the Gutman index and show that the degree-Kirchhoff index of Q P n is about half of its Gutman index.
Theorem 3.
Let Q P n denote a linear pentagonal derivation chain with length n. Then
G u t ( Q P n ) = 200 n 3 + 181 n 2 + 31 n + 1 .
Proof.
Let the vertices of Q P n be labeled as in Figure 1. Recall that G u t ( G ) = i < j d i d j d i j . Therefore, we evaluated d i d j d i j for all vertices, and then we summed them and divided by two. First, compute d i d j d i j for each type of vertices separately and the expression of each type of vertices are as follows:
▸ Fixed the vertices 1 or 1 of Q P n :
f 1 ( 1 , j ) = j 1 d 1 d j d 1 j = 2 × 2 × [ 3 n + 1 + ( 3 n + 1 ) + k = 0 n 1 ( 3 k + 2 ) ] + 2 × 3 × ( k = 1 3 n 1 k + k = 2 3 n k ) = 60 n 2 + 26 n + 2 .
▸ Fixed the vertices 2 or 2 of Q P n :
f 2 ( 2 , j ) = j 2 d 2 d j d 2 j = 2 × 3 × [ 1 + ( 3 n 1 ) + 2 + 3 n + k = 0 n 1 ( 3 k + 1 ) ] + 3 × 3 × ( k = 1 3 n 2 k + k = 2 3 n 1 k + 2 ) = 90 n 2 21 n + 30 .
▸ Fixed the vertices 3 l or 3 l ( 1 l n ) of Q P n :
f 3 ( 3 l , j ) = j 3 l d 3 l d j d 3 l j = 2 × 3 × [ ( 3 l 1 ) + ( 3 n 3 l + 1 ) + ( 3 n 3 l + 2 ) + 3 l + k = 0 l 1 ( 3 k + 2 ) + k = 1 n l 3 k ] + 3 × 3 × ( k = 1 3 l 2 k + k = 1 3 n 3 l k + k = 1 3 n 3 l + 1 k + k = 2 3 l 1 k ) = 90 n 2 + 180 l 2 180 n l 114 l + 99 n + 21 .
▸ Fixed the vertices 3 l + 1 or 3 l + 1 ( 1 l n 1 ) of Q P n :
f 4 ( 3 l + 1 , j ) = j 3 l + 1 d 3 l + 1 d j d ( 3 l + 1 ) j = 2 × 3 × [ 3 l + ( 3 n 3 l ) + ( 3 l + 1 ) + ( 3 n 3 l + 1 ) + k = 1 l 3 k + k = 0 n l 1 ( 3 k + 2 ) ] + 3 × 3 × ( k = 1 3 l 1 k + k = 1 3 n 3 l 1 k + k = 1 3 n 3 l k + k = 2 3 l k ) = 90 n 2 + 180 l 2 180 n l + 6 l + 39 n + 3 .
▸ Fixed the vertices 3 l + 2 or 3 l + 2 ( 1 l n 2 ) of Q P n :
f 5 ( 3 l + 2 , j ) = j 3 l + 2 d 3 l + 2 d j d ( 3 l + 2 ) j = 2 × 3 × [ ( 3 l + 1 ) + ( 3 n 3 l 1 ) + ( 3 l + 2 ) + ( 3 n 3 l ) + k = 1 l ( 3 k + 1 ) + k = 0 n l 1 ( 3 k + 1 ) ] + 3 × 3 × ( k = 1 3 l k + k = 1 3 n 3 l 2 k + k = 2 3 n 3 l 1 k + k = 2 3 l + 1 k + 2 ) = 90 n 2 + 180 l 2 180 n l + 126 l 21 n + 30 .
▸ Fixed the vertices 3 n 1 or 3 n 1 of Q P n :
f 6 ( 3 n 1 , j ) = j 3 n 1 d 3 n 1 d j d ( 3 n 1 ) j = 2 × 3 × [ ( 3 n 2 ) + 2 + 3 + ( 3 n 1 ) + k = 0 n 1 ( 3 k + 1 ) ] + 3 × 3 × ( k = 1 3 n 3 k + 1 + 2 + 2 + k = 2 3 n 2 k ) = 90 n 2 75 n + 84 .
▸ Fixed the vertices 3 n + 1 or 3 n + 1 of Q P n :
f 7 ( 3 n + 1 , j ) = j 3 n + 1 d 3 n + 1 d j d ( 3 n + 1 ) j = 2 × 2 × [ 3 n + 1 + ( 3 n + 1 ) + k = 1 n 3 k ] + 2 × 3 × ( k = 1 3 n 1 k + k = 2 3 n k ) = 60 n 2 + 30 n + 2 .
▸ Fixed the vertex 1 of Q P n :
f 8 ( 1 , j ) = j 1 d 1 d j d 1 j = 2 × 2 × [ 2 × 2 + 2 × 3 n + k = 1 n 1 ( 3 k + 2 ) ] + 2 × 3 × ( 2 × k = 1 3 n 1 k ) = 60 n 2 + 8 n + 8 .
▸ Fixed the vertices l ( 2 l n 1 ) of Q P n :
f 9 ( l , j ) = j l d l d j d l j = 2 × 2 × [ 2 × ( 3 l 1 ) + 2 × ( 3 n 3 l + 3 ) + k = 1 l 1 ( 3 k + 2 ) + k = 1 n l ( 3 k + 2 ) ] + 2 × 3 × ( 2 × k = 1 3 l 2 k + 2 × k = 2 3 n 3 l + 2 k ) = 60 n 2 + 120 l 2 120 n l + 128 n 156 l + 44 .
▸ Fixed the vertex n of Q P n :
f 10 ( n , j ) = j n d n d j d n j = 2 × 2 × [ 2 × 3 + 2 × ( 3 n 1 ) + k = 1 n 1 ( 3 k + 2 ) ] + 2 × 3 × ( 2 × 2 + 2 × k = 1 3 n 2 k ) = 60 n 2 28 n + 44 .
Hence,
G u t ( Q P n ) = 1 2 × [ 2 × ( f 1 ( 1 , j ) + f 2 ( 2 , j ) + l = 1 n f 3 ( 3 l , j ) + l = 1 n 1 f 4 ( 3 l + 1 , j ) + l = 1 n 2 f 5 ( 3 l + 2 , j ) + f 6 ( 3 n 1 , j ) + f 7 ( 3 n + 1 , j ) ) + f 8 ( 1 , j ) + l = 2 n 1 f 9 ( l , j ) + f 10 ( n , j ) ] = 200 n 3 + 181 n 2 + 31 n + 1 .
Together with Theorems 1 and 3, Corollary 1 follows immediately.
Corollary 1.
Let Q P n denote a linear pentagonal derivation chain with length n. Then
lim n K f * ( Q P n ) G u t ( Q P n ) = 1 2 .

6. Conclusions

In this paper, the degree-Kirchhoff index, Gutman index and the number of spanning trees of linear pentagonal derivation chain are calculated. Moreover, we show that the degree-Kirchhoff index of the linear pentagonal derivation chain is approximately to one half of its Gutman index. For some linear chains, the method applied in this paper could be effective. But for some other family of graphs, it is difficult to obtain the closed formulas of the degree-Kirchhoff index. So we must look for new methods. This will be the direction we will study later.

Author Contributions

Y.Z. and X.M. contributed equally to conceptualization, methodology, software, validation, formal analysis; Investigation, Y.Z.; Supervision, X.M.; Writing-original draft, Y.Z.; Writing-review and editing X.M. All authors have read and agreed to the published version of the manuscript.

Funding

The author’s research is supported by the National Natural Science Foundation of China (No. 12161085) and the Natural Science Foundation of Xinjiang Province (No. 2021D01C069).

Data Availability Statement

Not applicable.

Acknowledgments

The authors would like to thank the editor and anonymous reviewers for their helpful comments and suggestions which helped to improve the quality of our present paper.

Conflicts of Interest

The authors declare that they have no conflict of interest.

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Figure 1. The linear pentagonal derivation chain Q P n .
Figure 1. The linear pentagonal derivation chain Q P n .
Axioms 12 00945 g001
Table 1. The degree-Kirchhoff indices of linear pentagonal derivation chains from Q P 1 to Q P 40 .
Table 1. The degree-Kirchhoff indices of linear pentagonal derivation chains from Q P 1 to Q P 40 .
n Kf * ( QP n ) n Kf * ( QP n ) n Kf * ( QP n ) n Kf * ( QP n )
1232.4811146,653.8421975,092.77313,085,549.27
21283.8212188,906.94221,118,547.63323,390,205.89
33755.3413238,580.22231,275,422.66333,714,282.68
48247.0414296,273.67241,446,317.87344,058,379.65
515,358.9115362,587.30251,631,833.26354,423,096.79
625,690.9616438,121.11261,832,568.82364,809,034.11
739,843.1917523,475.09272,049,124.56375,216,791.60
858,415.5918619,249.25282,282,100.48385,646,969.27
982,008.1619726,043.58292,532,096.5639610,0167.12
10111,220.9120844,458.09302,799,712.83406,576,985.14
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Zhang, Y.; Ma, X. On the Normalized Laplacian Spectrum of the Linear Pentagonal Derivation Chain and Its Application. Axioms 2023, 12, 945. https://doi.org/10.3390/axioms12100945

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Zhang Y, Ma X. On the Normalized Laplacian Spectrum of the Linear Pentagonal Derivation Chain and Its Application. Axioms. 2023; 12(10):945. https://doi.org/10.3390/axioms12100945

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Zhang, Yuqing, and Xiaoling Ma. 2023. "On the Normalized Laplacian Spectrum of the Linear Pentagonal Derivation Chain and Its Application" Axioms 12, no. 10: 945. https://doi.org/10.3390/axioms12100945

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