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Article

On the Sum and Spread of Reciprocal Distance Laplacian Eigenvalues of Graphs in Terms of Harary Index

1
Department of Mathematics, University of Kashmir, Srinagar 190006, India
2
Department of Computer and Information Sciences, Northumbria University, Newcastle upon Tyne NE1 8ST, UK
*
Authors to whom correspondence should be addressed.
Symmetry 2022, 14(9), 1937; https://doi.org/10.3390/sym14091937
Submission received: 31 July 2022 / Revised: 29 August 2022 / Accepted: 16 September 2022 / Published: 17 September 2022

Abstract

:
The reciprocal distance Laplacian matrix of a connected graph G is defined as R D L ( G ) = R T ( G ) R D ( G ) , where R T ( G ) is the diagonal matrix of reciprocal distance degrees and R D ( G ) is the Harary matrix. Clearly, R D L ( G ) is a real symmetric matrix, and we denote its eigenvalues as λ 1 ( R D L ( G ) ) λ 2 ( R D L ( G ) ) λ n ( R D L ( G ) ) . The largest eigenvalue λ 1 ( R D L ( G ) ) of R D L ( G ) , denoted by λ ( G ) , is called the reciprocal distance Laplacian spectral radius. In this paper, we obtain several upper bounds for the sum of k largest reciprocal distance Laplacian eigenvalues of G in terms of various graph parameters, such as order n, maximum reciprocal distance degree R T m a x , minimum reciprocal distance degree R T m i n , and Harary index H ( G ) of G. We determine the extremal cases corresponding to these bounds. As a consequence, we obtain the upper bounds for reciprocal distance Laplacian spectral radius λ ( G ) in terms of the parameters as mentioned above and characterize the extremal cases. Moreover, we attain several upper and lower bounds for reciprocal distance Laplacian spread R D L S ( G ) = λ 1 ( R D L ( G ) ) λ n 1 ( R D L ( G ) ) in terms of various graph parameters. We determine the extremal graphs in many cases.

1. Introduction

Let G = ( V ( G ) , E ( G ) ) be a connected simple graph with vertex set V ( G ) and edge set E ( G ) . The order and size of G are | V ( G ) | = n and | E ( G ) | = m , respectively. The degree of a vertex v , denoted by d ( v ) , is the number of edges incident on the vertex v. Other undefined notations and terminology can be seen in [1].
The adjacency matrix A ( G ) = ( a i j ) of G is an n × n matrix in which ( i , j ) -entry is equal to 1 if there is an edge between vertex v i and vertex v j and equal to 0 otherwise. Let D e g ( G ) = diag ( d ( v 1 ) , d ( v 2 ) , , d ( v n ) ) be the diagonal matrix of vertex degrees d G ( v i ) , i = 1 , 2 , , n . The positive semi-definite matrix L ( G ) = D e g ( G ) A ( G ) is the Laplacian matrix of G. The eigenvalues of L ( G ) are called the Laplacian eigenvalues of G, which are denoted by μ 1 ( G ) , μ 2 ( G ) , , μ n ( G ) and are ordered as μ 1 ( G ) μ 2 ( G ) μ n ( G ) .
In G, the distance between two vertices v i , v j V ( G ) , denoted by d ( v i , v j ) , is defined as the length of a shortest path between v i and v j . The diameter of G, denoted by d ( G ) , is the length of a longest path among the distance between every two vertices of G. The distance matrix of G is denoted by D ( G ) and is defined as D ( G ) = ( d ( v i , v j ) ) v 1 , v j V ( G ) .
The transmission  T r G ( v i ) (or briefly, T r i if graph G is understood) of a vertex v i is defined as the sum of the distances from v i to all other vertices in G:
T r G ( v i ) = v j V ( G ) d ( v i . v j ) .
Let T r ( G ) = d i a g ( T r 1 , T r 2 , , T r n ) be the diagonal matrix of vertex transmissions of G. In [2], Aouchiche and Hansen introduced the Laplacian for the distance matrix of a connected graph. The matrix D L ( G ) = T r ( G ) D ( G ) is called the distance Laplacian matrix of G.
The Harary matrix of graph G, which is also called as the reciprocal distance matrix, denoted by R D ( G ) , is an n by n matrix defined as [3]
R D i j = 1 d ( v i , v j ) if i j 0 if i = j .
Henceforward, we consider i j for d ( v i , v j ) .
The reciprocal distance degree of a vertex v i , denoted by R T r G ( v i ) (or shortly R T i ), is given by
R T r G ( v i ) = v j V ( G ) v i v j 1 d ( v i , v j ) .
Let R T ( G ) be an n × n diagonal matrix defined by R T i i = R T r G ( v i ) .
The Harary index of a graph G, denoted by H ( G ) , is defined in [3] as
H ( G ) = 1 2 i = 1 n j = 1 n R D i j = 1 2 v j V ( G ) v i v j 1 d ( v i , v j ) .
Clearly,
H ( G ) = 1 2 v i V ( G ) R T r G ( v i ) .
To see more work performed on the Harary matrix, we refer the reader to [4,5,6] and the references therein.
In [7], the authors defined the reciprocal distance Laplacian matrix as R D L ( G ) = R T ( G ) R D ( G ) . Since R D L ( G ) is a real symmetric matrix, we can denote by
λ 1 ( R D L ( G ) ) λ 2 ( R D L ( G ) ) λ n ( R D L ( G ) )
the eigenvalues of R D L ( G ) . Since R L ( G ) is a positive semidefinite matrix, we will denote the spectral radius of R D L ( G ) by λ ( G ) = λ 1 ( R D L ( G ) ) , called the reciprocal distance Laplacian spectral radius. More work on the matrix R D L ( G ) can be seen in [8,9,10,11].
Let S k ( G ) = i = 1 k μ i ( G ) be the sum of the k largest Laplacian eigenvalues of G. Several researchers have been investigating the parameter S k ( G ) because of its importance in dealing with many problems in the theory, for instance, Brouwer’s conjecture and Laplacian energy. We refer the reader to [12,13,14,15] for recent work conducted on the graph invariant S k ( G ) . Motivated by the parameter S k ( G ) of the Laplacian matrix, we define the following. For 1 k n 1 , let R U k ( G ) denote the sum of the k largest reciprocal distance Laplacian eigenvalues:
R U k ( G ) = i = 1 k λ i ( R D L ( G ) ) .
The Laplacian spread of a graph G is defined as L S ( G ) = μ 1 ( G ) μ n 1 ( G ) , where μ 1 ( G ) and μ n 1 ( G ) are, respectively, the largest and second smallest Laplacian eigenvalues of G. More on L S ( G ) can be found in [16,17,18].
Since 0 is always a simple eigenvalue of the the reciprocal distance Laplacian matrix, we define the reciprocal distance Laplacian spread of a connected graph G such as the Laplacian spread as
R D L S ( G ) = λ 1 ( R D L ( G ) λ n 1 ( R D L ( G ) ,
where λ 1 ( R D L ( G ) and λ n 1 ( R D L ( G ) are, respectively, the largest and second smallest reciprocal distance Laplacian eigenvalues of G.
The rest of the paper is organized as follows. In Section 2, we obtain several upper bounds for the graph invariant R U k ( G ) in terms of various graph parameters, such as order n, maximum reciprocal distance degree R T m a x , minimum reciprocal distance degree R T m i n , and Harary index H ( G ) of G. We characterize the extremal cases corresponding to these bounds as well. As a consequence, we obtain the upper bounds for reciprocal distance Laplacian spectral radius λ ( G ) in terms of the same parameters as mentioned above and determine the extremal graphs. In Section 3, we find several upper and lower bounds for reciprocal distance Laplacian spread R D L S ( G ) in terms of various graph parameters. We characterize the extremal graphs in many cases.

2. Sum of the Reciprocal Distance Laplacian Eigenvalues

We begin with the following lemma.
Lemma 1.
[7] For any connected graph G, 0 is a simple eigenvalue of R D L ( G ) .
Proposition 1.
Let G be a connected graph with n vertices. Then,
(i) 
i = 1 n 1 λ i ( R D L ( G ) ) = 2 H ( G ) .
(ii) 
i = 1 n 1 λ i 2 ( R D L ( G ) ) = i = 1 n R T i 2 + 2 1 i < j n 1 d i j 2 .
Proof. 
( i ) Using the fact that the sum of eigenvalues is equal to the trace of a matrix and using Lemma 1, we have
i = 1 n λ i ( R D L ( G ) ) = i = 1 n 1 λ i ( R D L ( G ) ) = i = 1 n R T i = 2 H ( G ) .
The proof for ( i i ) follows arguments similar to those for ( i ) . □
Proposition 2.
Let G be a connected graph with n vertices. Then,
1 i < j n 1 d i j 2 n ( n 1 ) 2
with equality if and only if G K n .
Proof. 
For each 1 i < j n , we have d i j 1 so that 1 d i j 1 . Thus,
1 i < j n 1 d i j 2 1 i < j n 1 = n 2 = n ( n 1 ) 2 ,
which proves the required inequality.
Assume that the equality holds in the above inequality. Then, each d i j = 1 , whenever 1 i < j n , which is only possible if G K n .
For the converse, we observe that the equality holds for K n . □
Lemma 2.
[19Let x = ( x 1 , x 2 , x n ) and y = ( y 1 , y 2 , y n ) be n-tuples of real numbers satisfying 0 m 1 x i M 1 , 0 m 2 y i M 2 with i = 1 , 2 , , n and M 1 M 2 0 . Let α = m 1 M 1 and β = m 2 M 2 . If ( 1 + α ) ( 1 + β ) 2 , then
i = 1 n x i 2 i = 1 n y i 2 i = 1 n x i y i 2 n 2 4 ( M 1 M 2 m 1 m 2 ) 2 .
Let R T m a x = max { R T i : i = 1 , 2 , , n } and R T m i n = min { R T i : i = 1 , 2 , , n } be the maximum reciprocal distance degree and the minimum reciprocal distance degree of the graph G, respectively. Using Lemma 2, we obtain an upper bound for the graph invariant i = 1 n R T i 2 in terms of Harary index H ( G ) and order n of graph G.
Lemma 3.
Let G be a connected graph with n vertices. Then,
i = 1 n R T i 2 n 4 ( R T m a x R T m i n ) 2 + 4 H 2 ( G ) n .
Moreover, inequality is sharp, as shown by all of the reciprocal distance degree regular graphs.
Proof. 
In Lemma 2, we take x = ( R T 1 , R T 2 , , R T n ) , y = ( 1 , 1 , , 1 ) , M 1 = R T m a x , m 1 = R T m i n and M 2 = m 2 = 1 . With these values, it is straightforward to check that the condition ( 1 + α ) ( 1 + β ) 2 in Lemma 2 gets satisfied. Thus, from Inequality 1, we have
i = 1 n R T i 2 i = 1 n 1 i = 1 n R T i 2 n 2 4 ( R T m a x R T m i n ) 2
n i = 1 n R T 2 ( i ) 4 H 2 ( G ) n 2 4 ( R T m a x R T m i n ) 2
i = 1 n R T i 2 n 4 ( R T m a x R T m i n ) 2 + 4 H 2 ( G ) n .
Assume that G is k-reciprocal distance degree regular. Then, the left hand side of Inequality 2 becomes n k 2 and the right hand side becomes 4 H 2 ( G ) n = k 2 n 2 n = n k 2 , which shows that the equality holds for reciprocal distance degree regular graphs. □
Now, we obtain an upper bound for the graph invariant R U k ( G ) in terms of various graph parameters.
Theorem 1.
Let G be a connected graph with n vertices and Harary index H ( G ) . For 1 k n 2 , we have
R U k ( G ) 2 H ( G ) k n 1 + k ( n k 1 ) n 2 ( n 1 ) ( R T m a x R T m i n ) 2 + 4 ( n 1 ) 16 H 2 ( G ) 2 ( n 1 ) n
with equality if and only if G K n . For k = n 1 , equality always holds.
Proof. 
Let R U k ( G ) = R k . For 1 k n 2 , using Proposition 1 and Cauchy–Schwarz inequality, we have
λ k + 1 ( R D L ( G ) ) + + λ n 1 ( R D L ( G ) ) 2 = ( 2 H ( G ) R k ) 2 ( n k 1 ) λ k + 1 2 ( R D L ( G ) ) + + λ n 1 2 ( R D L ( G ) ) = ( n k 1 ) i = 1 n R T i 2 + 2 1 i < j n 1 d i j 2 ( λ 1 2 ( R D L ( G ) ) + + λ k 2 ( R D L ( G ) ) ) ( n k 1 ) i = 1 n R T i 2 + 2 1 i < j n d i j 2 R k 2 k .
Further simplification gives
R k 2 4 k H ( G ) R k n 1 + 4 k H 2 ( G ) n 1 k ( n k 1 ) n 1 i = 1 n R T i 2 + 2 1 i < j n 1 d i j 2 0 .
Therefore,
R k 2 H ( G ) k + k ( n k 1 ) ( n 1 ) i = 1 n R T i 2 + 2 1 i < j n 1 d i j 2 4 H 2 ( G ) n 1 .
Using Proposition 2, Lemma 3 in Inequality 3 and after simplifications, we have
R k 2 H ( G ) k n 1 + k ( n k 1 ) n 2 ( n 1 ) ( R T m a x R T m i n ) 2 + 4 ( n 1 ) 16 H 2 ( G ) 2 ( n 1 ) n ,
which proves the required inequality.
Assume that equality holds in the above inequality. Then, equality must hold simultaneously in the Cauchy–Schwarz inequality, Proposition 2, and Lemma 3, which is only possible if G K n .
Conversely, if G K n , then the left hand side of the main equality is equal to k n . After performing the necessary calculations, the right-hand side reduces to 2 H ( K n ) k n 1 + 0 = n ( n 1 ) k n 1 = k n , which proves the converse part.
Using the fact that traces of a matrix are equal to the sum of its eigenvalues and noting that 2 H ( G ) = R n 1 , we easily see that equality always holds when k = n 1 in the main inequality. □
Taking k = 1 in Theorem 1, we obtain an upper bound for the reciprocal distance Laplacian spectral radius λ ( G ) of a connected graph G in terms of the maximum reciprocal distance degree R T m a x , minimum reciprocal distance degree R T m i n , order n, and Harary index H ( G ) .
Theorem 2.
Let G be a connected graph with n vertices and Harary index H ( G ) . Then,
λ ( G ) 2 H ( G ) n 1 + ( n 2 ) n 2 ( n 1 ) ( R T m a x R T m i n ) 2 + 4 ( n 1 ) 16 H 2 ( G ) 2 ( n 1 ) n
with equality if and only if G K n .
Lemma 4.
[20] Let [ n ] = { 1 , 2 , , n } be the canonical n-element set, and let [ n ] ( 2 ) denote the set of two-element subsets of [n], that is, the edge set of K n . To each entry { i , j } = i j in [ n ] ( 2 ) , associate a real variable z i j ; then, for n 2 , and for all z i j s , we have
i j z i j 2 + n 1 2 i j z i j 2 n 1 2 i j i z i j 2 0 .
Now, we obtain an upper bound for the sum of the squares of the reciprocal distance degrees in terms of the Harary index H ( G ) and the order n of the graph G.
Lemma 5.
Let G be a connected graph with order n and having diameter d. Then
i R T i 2 n ( n 1 ) ( n 2 ) 2 + 2 H 2 ( G ) n 1
with equality if and only if G K n .
Proof. 
Put 1 d i j for z i j in Lemma 4 and observe that with each 1 d i j 1 , we have
i j 1 d i j 2 + n 1 2 i j 1 d i j 2 n 1 2 i j i 1 d i j 2 0 or H 2 ( G ) + n 1 2 i j 1 d i j 2 n 1 2 i R T i 2 0 .
Simplifying further, we have
i R T i 2 2 n 1 ( n 1 ) ( n 2 ) 2 n ( n 1 ) 2 + 2 H 2 ( G ) n 1 or i R T i 2 n ( n 1 ) ( n 2 ) 2 + 2 H 2 ( G ) n 1 .
proving the required inequality.
Assume that the equality holds in the above inequality. Then, each 1 d i j = 1 or d i j = 1 which is only possible if G is the complete graph K n .
Conversely, assume that G K n . Then, we observe that H ( G ) = n ( n 1 ) 2 and i R T i 2 = n ( n 1 ) 2 . Substituting these values in the main inequality, we see that the equality holds. □
A similar argument has been adopted in studying Estrada index [21]. Using Lemma 5, we have the following upper bound for the graph invariant R U k ( G ) in terms of order n and Haray index H(G). This bound seems to be more elegant than the bound in Theorem 1 since it uses relatively less number of parameters.
Theorem 3.
Let G be a connected graph with n vertices and Harary index H ( G ) . For 1 k n 2 , we have
R U k ( G ) 2 H ( G ) k n 1 + k ( n k 1 ) n ( n 1 ) 2 H ( G ) n ( n 1 ) + 2 H ( G ) ( n 1 ) 2
with equality if and only if G K n . For k = n 1 , equality always holds.
Proof. 
We proceed exactly as in Theorem 1 upto Inequality 3, then use Lemma 5 and Proposition 2, and obtain
R k 2 H ( G ) k + k ( n k 1 ) ( n 1 ) n ( n 1 ) ( n 2 ) 2 + 2 H 2 ( G ) n 1 + n ( n 1 ) 4 H 2 ( G ) n 1 .
Simplifying further, we have
R k 2 H ( G ) k + k ( n k 1 ) n 2 ( n 1 ) 2 2 2 H 2 ( G ) n 1 .
or
R k 2 H ( G ) k n 1 + k ( n k 1 ) n ( n 1 ) 2 H ( G ) n ( n 1 ) + 2 H ( G ) ( n 1 ) 2
which is the inequality in the statement of theorem.
The remaining part of the proof follows by using similar arguments as in Theorem 1. □
As a consequence of Theorem 3, we obtain the following upper bound for reciprocal distance Laplacian spectral radius λ ( G ) of a connected graph G in terms of the Harary index H ( G ) and order n of the graph G.
Theorem 4.
Let G be a connected graph with n vertices and Harary index H ( G ) . Then,
λ ( G ) 2 H ( G ) n 1 + ( n 2 ) n ( n 1 ) 2 H ( G ) n ( n 1 ) + 2 H ( G ) ( n 1 ) 2
with equality if and only if G K n .

3. Reciprocal Distance Laplacian Spread

We begin this section with the following observations.
Lemma 6.
[7] Let G be a connected graph on n vertices with diameter d = 2 . Then,
λ i ( R D L ( G ) ) = n + μ i ( G ) 2
for i = 1 , 2 , , n 1 . Furthermore, n + μ i ( G ) 2 and μ i ( G ) both have the same multiplicity for i = 1 , 2 , , n .
A special case of the well-known m i n m a x t h e o r e m is the following result.
Lemma 7.
[22] If M is a symmetric n × n matrix with eigenvalues δ 1 δ 2 δ n , then for any x R n ( x 0 ) ,
δ 1 x T N x x T x .
Equality holds if and only if x is an eigenvector of M corresponding to the largest eigenvalue δ 1 .
Lemma 8.
[7] If G is a graph on n > 2 vertices, then the multiplicity of λ ( G ) is always less than or equal to n 1 with equality if and only if G is the complete graph.
Lemma 9.
[23] Let G be a connected graph of order n 2 . Then, μ 1 ( G ) ( G ) + 1 , with equality if and only if ( G ) = n 1 .
Theorem 5.
Let G be a connected graph with n vertices having Harary index H ( G ) . Then,
RDSL ( G ) ( n 2 ) n ( n 1 ) 2 H ( G ) n ( n 1 ) + 2 H ( G ) 2
Equality holds if and only if G K n .
Proof. 
To prove the inequality, we consider 2 H ( G ) = λ 1 ( R D L ( G ) ) + λ 2 ( R D L ( G ) ) + + λ n 1 ( R D L ( G ) ) , which gives 2 H ( G ) ( n 2 ) λ 1 ( R D L ( G ) ) + λ n 1 ( R D L ( G ) ) or λ n 1 ( R D L ( G ) ) 2 W ( G ) ( n 2 ) λ 1 ( R D L ( G ) ) . Therefore,
RDLS ( G ) = λ 1 ( R D L ( G ) ) λ n 1 ( R D L ( G ) ) λ 1 ( R D L ( G ) ) 2 H ( G ) + ( n 2 ) λ 1 ( R D L ( G ) ) ,
which gives
R D S L ( G ) ( n 1 ) λ 1 ( R D L ( G ) ) 2 H ( G ) .
Using Theorem 4 in Inequality 5, we have
RDSL ( G ) ( n 2 ) n ( n 1 ) 2 H ( G ) n ( n 1 ) + 2 H ( G ) 2 ,
proving the required inequality.
From Inequality 5 and Theorem 4, we see that equality holds in Inequality 4 if and only if λ 1 ( R D L ( G ) ) = λ 2 ( R D L ( G ) ) = = λ n 2 ( R D L ( G ) ) and G K n .
Since the reciprocal distance Laplacian spectrum of K n is { n ( n 1 ) , 0 } , therefore, equality holds in Inequality 4 if and only if G K n . □
If we use Theorem 2 instead of Theorem 4 in the above result, we have the following theorem:
Theorem 6.
Let G be a connected graph with n vertices having Wiener index W ( G ) . Then,
RDSL ( G ) ( n 2 ) n 2 ( n 1 ) ( R T m a x R T m i n ) 2 + 4 ( n 1 ) 16 H 2 ( G ) 2 n .
Equality holds if and only if G K n .
Let S d = 1 + 1 2 + 1 3 + + 1 d . The following lemma gives the lower bound for the reciprocal distance Laplacian spectral radius in terms of order n, diameter d, and S d .
Lemma 10.
Let G be a connected graph on n vertices having diameter d. Then,
λ ( G ) S d + ( n d 2 ) d .
Proof. 
Let v 1 v 2 v d + 1 be the diametral path in G such that d G ( v 1 , v d + 1 ) = d . Consider the n-vector x = ( x 1 , x 2 , , x d 1 , x d , x d + 1 , , x n ) T defined by
x i = 1 2 if i = 1 , d + 1 0 otherwise .
By Lemma 7, we have
λ ( G ) x T D Q y y T y = R T 1 + R T d + 1 2 1 d G ( v 1 , v d + 1 ) = R T 1 + R T d + 1 2 1 d .
It can be easily seen that
R T 1 1 + 1 2 + 1 3 + + 1 d + ( n d 1 ) d = S d + ( n d 1 ) d
Similarly,
R T d + 1 S d + ( n d 1 ) d .
On substituting inequalities 7, 8 in Inequality 6, we have
λ ( G ) S d + ( n d 1 ) d 1 d = S d + ( n d 2 ) d .
 □
Theorem 7.
Let G be a connected graph with order n having diameter d. Then,
RDLS ( G ) S d + ( n d 2 ) d 2 H ( G ) n 1 .
Proof. 
Note that i = 1 n 1 λ i ( R D L ( G ) ) = 2 H ( G ) . From this equality, we see that
λ n 1 ( R D L ( G ) ) 2 H ( G ) n 1 .
Using Lemma 10 and Inequality 9, we have
RDSL ( G ) = λ 1 ( R D L ( G ) ) λ n 1 ( R D L ( G ) ) S d + ( n d 2 ) d 2 H ( G ) n 1 .
Theorem 8.
Let G be a connected graph on n 3 vertices having diameter d 2 . Then,
R D L S ( G ) n + ( G ) + 1 2 2 H ( G ) n 1 .
Equality holds if and only if d = 1 , that is, G K n .
Proof. 
First, we show that equality holds for K n . Note that the reciprocal distance Laplacian spectrum of the complete graph K n is { n ( n 1 ) , 0 } so that R D L S ( K n ) = λ 1 ( R D L ( K n ) ) λ n 1 ( R D L ( K n ) ) = n n = 0 . Additionally, the right-hand side of Inequality 10 for K n is equal to ( K n ) + 1 2 H ( K n ) n 1 = n 1 + 1 n ( n 1 ) n 1 = 0 . Thus, from the above arguments, we see that equality holds in Inequality 10 when G is a complete graph.
Now, let G be a graph with diameter d = 2 . Using Lemma 6, we have
R D L S ( G ) = λ 1 ( R D L ( G ) ) λ n 1 ( R D L ( G ) ) = n + μ 1 2 λ n 1 ( R D L ( G ) ) .
By Lemma 8, we see that Inequality 9 is strict since G is a noncomplete graph, that is, λ n 1 ( R D L ( G ) ) < 2 H ( G ) n 1 . Using this observation with Lemma 9 in Equality 11, we have
R D L S ( G ) > n + ( G ) + 1 2 2 H ( G ) n 1 .

Author Contributions

Investigation, S.K., S.P. and Y.S.; writing—original draft preparation, S.K., S.P. and Y.S.; writing—review and editing, S.K., S.P. and Y.S. All authors have read and agreed to the published version of the manuscript.

Funding

The research of S. Pirzada is supported by the SERB-DST research project number CRG/2020/000109.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Not applicable.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Pirzada, S. An Introduction to Graph Theory; Universities Press, Orient BlackSwan: Hyderabad, India, 2012. [Google Scholar]
  2. Aouchiche, M.; Hansen, P. Two Laplacians for the distance matrix of a graph. Linear Algebra Appl. 2013, 439, 21–33. [Google Scholar] [CrossRef]
  3. Plavsić, D.; Nikolić, S.; Trinajstić, N.; Mihalić, Z. On the Harary index for the characterization of chemical graphs. J. Math. Chem. 1993, 12, 235–250. [Google Scholar] [CrossRef]
  4. Das, K.C. Maximum eigenvalue of the reciprocal distance matrix. J. Math. Chem. 2010, 47, 21–28. [Google Scholar] [CrossRef]
  5. Huang, F.; Li, X.; Wang, S. On graphs with maximum Harary spectral radius. arXiv 2014, arXiv:1411.6832v1. [Google Scholar] [CrossRef]
  6. Zhou, B.; Trinajstić, N. Maximum eigenvalues of the reciprocal distance matrix and the reverse Wiener matrix. Int. J. Quantum Chem. 2008, 108, 858–864. [Google Scholar] [CrossRef]
  7. Bapat, R.; Panda, S.K. The spectral radius of the reciprocal distance Laplacian matrix of a graph. Bull. Iranian Math. Soc. 2018, 44, 1211–1216. [Google Scholar] [CrossRef]
  8. Baghipur, M.; Ghorbani, M.; Ganie, H.A.; Shang, Y. On the second-largest reciprocal distance signless Laplacian eigenvalue. Mathematics 2021, 9, 512. [Google Scholar] [CrossRef]
  9. Medina, L.; Trigo, M. Upper bounds and lower bounds for the spectral radius of reciprocal distance, reciprocal distance Laplacian and reciprocal distance signless Laplacian matrices. Linear Algebra Appl. 2021, 609, 386–412. [Google Scholar] [CrossRef]
  10. Medina, L.; Trigo, M. Bounds on the reciprocal distance energy and reciprocal distance Laplacian energies of a graph. In Linear Multilinear Algebra; Abingdon, UK, 2020. [Google Scholar] [CrossRef]
  11. Trigo, M. On Hararay energy and reciprocal distance Laplacian energies. J. Phys. Conf. Ser. 2021, 2090, 012102. [Google Scholar] [CrossRef]
  12. Alhevaz, A.; Baghipur, M.; Pirzada, S.; Shang, Y. Some inequalities involving the distance signless Laplacian eigenvalues of graphs. Trans. Combin. 2021, 10, 9–29. [Google Scholar] [CrossRef]
  13. Ganie, H.A.; Pirzada, S.; Trevisan, V. On the sum of k largest Laplacian eigenvalues of a graph and clique number. Mediterr. J. Math. 2021, 18, 15. [Google Scholar] [CrossRef]
  14. Ganie, H.A.; Pirzada, S.; Bilal, A.R.; Ul Shaban, R. On Laplacian eigenvalues of graphs and Brouwer’s conjecture. J. Ramanujan Math. Soc. 2021, 36, 13–21. [Google Scholar] [CrossRef]
  15. Ganie, H.A.; Pirzada, S.; Bilal, A.R.; Trevisan, V. Further developments on Brouwer’s conjecture for the sum of Laplacian eigenvalues of graphs. Linear Algebra Appl. 2020, 588, 1–18. [Google Scholar] [CrossRef]
  16. Fan, Y.Z.; Xu, J.; Wang, Y.; Liang, D. The Laplacian spread of a tree. Discrete Math. Theor. Comput. Sci. 2018, 10, 79–86. [Google Scholar] [CrossRef]
  17. Golberg, F. Bounding the gap between extremal Laplacian eigenvalues of graphs. Linear Algebra Appl. 2006, 416, 68–74. [Google Scholar] [CrossRef]
  18. You, Z.; Liu, B. The Laplacian spread of graphs. Czechoslovak Math. J. 2012, 62, 155–168. [Google Scholar] [CrossRef]
  19. Izumino, S.; Mori, H.; Seo, Y. On Ozeki’s inequality. J. Inequal. Appl. 1998, 2, 235–253. [Google Scholar] [CrossRef]
  20. Caen, D.D. An upper bound on the sum of squares of degrees in a graph. Discrete Math. 1998, 185, 245–248. [Google Scholar] [CrossRef]
  21. Shang, Y. On the number of spanning trees, the Laplacian eigenvalues, and the Laplacian Estrada index of subdivided-line graphs. Open Math. 2016, 14, 641–648. [Google Scholar] [CrossRef]
  22. Zhang, F. Matrix Theory: Basic Results and Techniques; Springer: New York, NY, USA, 1999. [Google Scholar]
  23. Grone, R.; Merris, R. The Laplacian spectrum of a graph II. SIAM J. Discrete Math. 1994, 7, 229–237. [Google Scholar] [CrossRef]
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Khan, S.; Pirzada, S.; Shang, Y. On the Sum and Spread of Reciprocal Distance Laplacian Eigenvalues of Graphs in Terms of Harary Index. Symmetry 2022, 14, 1937. https://doi.org/10.3390/sym14091937

AMA Style

Khan S, Pirzada S, Shang Y. On the Sum and Spread of Reciprocal Distance Laplacian Eigenvalues of Graphs in Terms of Harary Index. Symmetry. 2022; 14(9):1937. https://doi.org/10.3390/sym14091937

Chicago/Turabian Style

Khan, Saleem, Shariefuddin Pirzada, and Yilun Shang. 2022. "On the Sum and Spread of Reciprocal Distance Laplacian Eigenvalues of Graphs in Terms of Harary Index" Symmetry 14, no. 9: 1937. https://doi.org/10.3390/sym14091937

APA Style

Khan, S., Pirzada, S., & Shang, Y. (2022). On the Sum and Spread of Reciprocal Distance Laplacian Eigenvalues of Graphs in Terms of Harary Index. Symmetry, 14(9), 1937. https://doi.org/10.3390/sym14091937

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