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Abstract
For a sequence of adjacency matrices, describing the unfolding of a network from the graph of a star, through graphs of a broom, to the graph of a link with constant vertices and edges, we show that the leading eigenvalue (the spectral radius) satisfies a simple algebraic equation. The equation allows easy numerical computation of the leading eigenvalue as well as a direct proof of its monotonicity in terms of the maximal degree of vertices.
PUBLIC INTEREST STATEMENT
In a network of agents susceptible to an infectious disease, assume that we know all details of the structure of the network: whether and how different agents are connected to each other. How can we predict whether the infectious disease will cause an epidemic if one or more agents are infected? How can we design policies to alter the structure of the network in order to reduce the speed at which the disease spreads? Similar problems arise in many other networks. These problems can often be formulated as a mathematical problem of understanding how certain global quantities such as the leading eigenvalue of a nonnegative matrix depends on its entries. In a simple situation when a network in the shape of a star unfolding into a broom and eventually forming a link, we give a complete description of the leading eigenvalue in terms of the network structure.
1. Introduction
Our study of how the leading eigenvalue, or the spectral radius, of an adjacency matrix of a network varies when the structure of the network changes is motivated by recent interests of research in how an infectious disease spreads over a network (Brauer, Citation2008; Diekmann & Heesterbeek, Citation2000; Newman, Citation2002, Citation2010). M.E.J. Newman stated in the introduction to Chapter 16 of (Newman, Citation2010): “once we have measured and quantified the structure of a network, how do we turn the results into predictions or conclusions about how the overall system will behave? Unfortunately, progress in this area has been far slower than progress on characterizing structure … ”. Imagine that we have a network of agents susceptible to an infectious disease just discovered in the network. Assume that
is the transmission rate from agent
to agent
and
is the recovery rate for agent
. Then, there is a close relation between the leading eigenvalue of the matrix
, where
, and the essential parameters of the infectious disease: the reproductive number
, the speed at which the infectious disease can spread in the network, and the rate at which the disease is eradicated from the network (Diekmann & Heesterbeek, Citation2000; Gatto, Mari, & Rinaldo, Citation2013; Jiang, Citation2016; Kostova, Citation2009). When the transmission rates and the recovery rates are independent of individual agent, the study of the leading eigenvalue of the matrix
on its entries is reduced to determining how the leading eigenvalue of an adjacency matrix depends on the topology of the network. There are abundant results in graph theory on this subject, e.g. (Brouwer & Haemers, Citation2010; Brualdi & Hoffman, Citation1985; Bunimovich & Webb, Citation2014; Li & Feng, Citation1979; Liu, Lu, & Tian, Citation2004; Patuzzi, de Freitas, & Del-Vecchio, Citation2014). Many address the dependence of the leading eigenvalue on the underlying undirected connected graph. However, the underlying structure of the graph is usually not motivated by actual problems in applications nor dynamic. In this short paper, our interest is restricted to the study of the follow particular problem: assuming that the structure of a graph of
agents is evolving along a well-defined path, how does its leading eigenvalue change? We solve this problem completely in the simple case where the graph unfolds from a star to a link while both numbers of vertices and edges remain constant. The leading eigenvalue can be uniquely determined by solving a quite simple algebraic equation. As a consequence, we obtain its asymptotic behavior as the size of the network increases and also a direct proof of its monotonicity in terms of the maximal degree of vertices.
2. Main result
Let be the following sequence of undirected connected graphs of vertices
. The set of edges of
is
and for
, the set of edges of
,
. Note that
and
are the same star of
vertices and
is the link between two vertices
and
.
The adjacency matrix of any graph is a square matrix with entries either
or
. An entry
of an Adjacency matrix is
if and only if two vertices
and
are connected by an edge. When a graph is undirected, its adjacency matrix is a symmetric nonnegative matrix. By the Perron-Frobenius theorem, matrix
has an eigenvalue
, the leading eigenvalue, which is simple and greater than the magnitude of any other eigenvalues of
(Berman & Plemmons, Citation1994; Brouwer & Haemers, Citation2010).
For , let
denote the adjacency matrix of the graph
and let
be the leading eigenvalue of
. Let
. We note that the diameter of the graph
is exactly
and the unique maximal degree of vertices of
is
.
Theorem 1.
The leading eigenvalue of ,
, decreases in
,
. For
and
,
where is the unique solution to the equation
Since the one-variable function is an increasing function on the interval
, the monotonicity of
in
follows from the monotonicity of
once the relation (1) is established. A direct estimation of the unique solution
to the equation
leads to the following asymptotic behavior of
when
approaches infinite.
Corollary 1.
For each fixed ,
Remarks
1. The monotonicity of in
is known. It follows from a theorem in (Li & Feng, Citation1979) and also from Corollary 2.2 in (Patuzzi et al., Citation2014). Showing that the leading eigenvalue
satisfying the equations (1) and (2) is new. The equations give not only an alternative direct proof of the monotonicity of
in
, but also a way to estimate the rate of change of
in
. 2. This formulation of the leading eigenvalue is reminiscent of another interesting result concerning the limit points of all leading eigenvalues of trees with
(Hoffman, Citation1972). 3. The graph
is called a broom in (Del-Vecchio, Gutman, Trevisan, & Vinagre, Citation2009).
The rest of the paper is devoted to the proof the main theorem. In Section 3.1, using the standard cofactor expansion, we first show the leading eigenvalue of the adjacency matrix
satisfies a recursive relation of characteristic polynomials of the tri-diagonal adjacency matrices. Solving this recursive relation, we obtain a representation of the eigenvalue
in terms of the unique solution of a simple algebraic equation. The monotonicity of
in terms of
follows easily. A detailed proof of the monotonicity of
in
via the implicit differentiation is in Section 3.2.
3. Proofs
For , let
denote the characteristic polynomial of the adjacency matrix
. Let
denote the characteristic polynomial of the tri-diagonal adjacency matrix
. We can directly verify via cofactor expansion that
and
possess the following properties. The second recursive relation is obtained by expanding the determinant along the last column first and then the last row. Iterating the recursive relation, we obtain the third equation. The details of the proof of these recursive relations are omitted since the verification of them is straightforward. See also (Del-Vecchio et al., Citation2009; Kulkarni, Schmidt, & Tsui, Citation1999).
Proposition 1
(1)
(2)
(3) .
3.1. Eigenvalue ![](//:0)
satisfying the equations (1) and (2)
By Proposition 1 (3), the leading eigenvalue of
satisfies the equation
For convenience, we let . For
,
. We have the following characterization of
when
.
Lemma 1 When , the leading eigenvalue
has the properties
and
, where
is the unique real solution to the equation
Proof.
We consider the recursive relation (1) in Proposition 1, ,
. Let
. The equation has a unique real solution for
if and only if
. Otherwise,
is a complex number. We have
and thus,
Iterate Equation (6) and notice that and
. Since
, we have
Further iterate the last recursive relation, we have for ,
Thus, when ,
Sum up the geometric progression we have, for ,
We now solve the equation
Use the formulas and
. We have
Multiply both sides by and simplify. We have
Or,
Let and
. So we have
We conclude that has a real positive solution
if and only if the equation
has a real positive solution in
. The existence and uniqueness of the solution to the equation
in the interval
are proved in the next lemma.
Lemma 2. For and
, the equation
has a unique solution
and
increases in
.
Proof.
Notice that when
. So possible solutions to
are located in
.
is always a solution. But the corresponding values
and
do not satisfy the equation
when
and
.
Let and
. We have
when
. But
. Thus, for
and
is sufficiently close to
, we have
. On the other hand
while
is finite. So,
must have at least one solution in
.
To see the solution is unique, we take the logarithm of both and
. Let
and
. Let
be the smallest solution to the equation
in
. We show that
for all
and thus
for all
. Since there is no solution to
in the interval
and
, we have
for
, which implies
.
To see that for
. We start with
, i.e.,
or
We have
We now show that the function is increasing in
by showing its derivative is positive in the interval
. Taking the derivative, we have
To see that it is positive, we need to show , i.e.,
Since increases in
,
as a function of
increases in
. We now consider the value of
when
or
. We have
. Simplify the equation. We have
since we are looking for solutions in
. we have
when
. Thus, for
,
, the smallest solution to the equation
in
satisfies the inequality
. Note that when
,
. Thus, we have for
,
It yields that for ,
i.e., So, the solution to
is unique in
.
3.2. Monotonicity of ![](//:0)
in ![](//:0)
: ![](//:0)
![](//:0)
The characterization of the leading eigenvalue of the adjacency matrix provides a direct way to prove its monotonicity in
. Let
denote the unique solution to the equation
.
Proposition 2. When and
,
.
Proof. We treat as a continuous variable and denote by
the derivative
. Multiply
to both sides of the equation. We have
With fixed, taking the derivative with respect to
, we have
Thus,
We now show
and
under the conditions and
.
Divide the expression by
. We have
When ,
Since and
, we have
The function in the last equation decreases in when
and has a negative value at
. So,
To see , we again divide the expression by
: we have
.
Since , we replace
by the
in the last expression. We now have
Let and
. We show that
. Indeed,
when and
. Thus, for
and
,
This means
We thus conclude that when
and
.
The function is also monotonic in
when
. We leave the proofs to interested readers in these special cases.
When and
, using the equation
and the monotonicity of
in
, we can conclude that
since
(see also the proof of Lemma 2 for a better estimate). For each fixed
,
now can be estimated when
:
. We see that
converges to
exponentially fast. Thus, for each fixed
, the leading eigenvalue
converges to
. Corollary 1 follows immediately from this direct estimation of
:
Proposition 3 For and
,
Acknowledgements
The authors thank Kenneth Berenhaut for discussions and comments and anonymous reviewers for their comments and suggestions.
Additional information
Funding
Notes on contributors
William D. Fries
Mr. William D. Fries is currently a Ph.D. student in Graduate Studies in Applied Mathematics at University of Arizona. He graduated in 2016 with a B.A. in Mathematics and Religious Studies from Washington and Lee University and in 2018 with a M.A. in Mathematics from Wake Forest University. This work was part of his master's degree thesis.
Miaohua Jiang
Dr. Miaohua Jiang is a professor in the Department of Mathematics and Statistics at Wake Forest University in North Carolina. U.S.A. He received a B.S. and an M.S. in Mathematics from Wuhan University and East China Normal University in China, respectively, and a Ph.D. in Mathematics from the Pennsylvania State University. Prior to starting his current position, Dr. Jiang held post-doctoral positions at the Center for Dynamical Systems and Nonlinear Studies at Georgia Institute of Technology and the Institute for Mathematics and its Applications at University of Minnesota. Dr. Jiangs research interests include smooth dynamical systems and ergodic theory and their applications in economics and biology.
References
- Berman, A., & Plemmons, R. J. (1994). Nonnegative matrices in the mathematical sciences (pp. 27). Philadelphia: SIAM.
- Brauer, F. (2008). An introduction to networks in epidemic modeling. In Mathematical epidemiology (pp. 133–8). Lecture Notes in Math., 1945, Math. Biosci. Subser., Berlin: Springer.
- Brouwer, A. E., & Haemers, W. H. (2010). Spectra of graphs (pp. 33). New York, Dordrecht, Heidelberg and London: Spinger.
- Brualdi, R. A., & Hoffman, A. J. (1985). On the spectral radius of (0,1)-matrices. Linear Algebra and Its Applications, 65, 133–146. doi:10.1016/0024-3795(85)90092-8
- Bunimovich, L., & Webb, B. (2014). Isospectral transformations (pp. 20). New York: Springer.
- Del-Vecchio, R. R., Gutman, I., Trevisan, V., & Vinagre, C. T. M. (2009). On the spectral and energies of double-broom-like trees. Kragujevac Journal of Science, 31, 45–58.
- Diekmann, O., & Heesterbeek, J. (2000). Mathematical epidemiology of infectious diseases: Model building, analysis and interpretation (pp. 73–77). Chichester: John Wiley.
- Gatto, M., Mari, L., & Rinaldo, A. (2013, Sept). Leading eigenvalues and the spread of cholera. SIAM News, 43, 3.
- Hoffman, A. J. (1972). On limit points of spectral radii of non-negative symmetric integral matrices. In Graph theory and applications (Vol. 303, pp. 165–172). Lecture Notes in Math. Berlin: Springer.
- Jiang, M. (2016). Approximating individual risk of infection in a markov chain epidemic network model with a deterministic system. Journal of Difference Equations Applications, 22(10), 1438–1451. doi:10.1080/10236198.2016.1201476
- Kostova, T. (2009). Interplay of node connectivity and epidemic rates in the dynamics of epidemic networks. Journal of Difference Equations Applications, 15(4), 415–428. doi:10.1080/10236190902766835
- Kulkarni, D., Schmidt, D., & Tsui, S.-K. (1999). Eigenvalues of tridiagonal pseduo-teoplitz matrices. Linear Algebra and Its Applications, 297(1), 63–80. doi:10.1016/S0024-3795(99)00114-7
- Li, Q., & Feng, K. Q. (1979). On the largest eigenvalue of a graph (Chinese). Acta Mathematicae Applicatae Sinica, 2(2), 157–175.
- Liu, H., Lu, M., & Tian, F. (2004). On the spectral radius of graphs with cut edges. Linear Algebra and Its Applications, 389(Supplement C), 139–145. doi:10.1016/j.laa.2004.03.026
- Newman, M. (2002, Jul). Spread of epidemic disease on networks. Physical Review E, 66, 016128. doi:10.1103/PhysRevE.66.016128
- Newman, M. (2010). Networks, an introduction (pp. 591). New York, NY, USA: Oxford University Press, Inc.
- Patuzzi, L., de Freitas, M., & Del-Vecchio, R. R. (2014). Indices for special classes of trees. Linear Algebra and Its Applications, 442, 106–114. doi:10.1016/j.laa.2013.07.007