Home Mathematics Computing the determinant of a signed graph
Article Open Access

Computing the determinant of a signed graph

  • Bader Alshamary EMAIL logo and Zoran Stanić
Published/Copyright: March 25, 2024

Abstract

A signed graph is a simple graph in which every edge has a positive or negative sign. In this article, we employ several algebraic techniques to compute the determinant of a signed graph in terms of the spectrum of a vertex-deleted subgraph. Particular cases, including vertex-deleted subgraphs without repeated eigenvalues or singular vertex-deleted subgraphs are considered. As applications, an algorithm for the determinant of a signed graph with pendant edges is established, the determinant of a bicyclic graph and the determinant of a chain graph are computed. In the end, the uniqueness of the polynomial reconstruction for chain graphs is proved.

MSC 2010: 05C50; 05C22

1 Introduction

A signed graph G ˙ is a finite, undirected graph without loops or parallel edges, in which every edge is assigned either positive or negative sign. The vertex set is denoted by V ( G ˙ ) , and the order n is the number of vertices of G ˙ . The adjacency matrix A G ˙ has + 1 or 1 for adjacent vertices, depending on the sign of the connecting edge. The sign of an edge e is denoted by σ ( e ) , and σ can be seen as the sign function (or the signature) that maps the edge set to { + 1 , 1 } . In this context, an ordinary (unsigned) graph is interpreted as a signed graph without negative edges. In this case, the graph is simply denoted by G , i.e., the absence of a dot symbol refers to the all-positive edge signature. The negation G ˙ of G ˙ is obtained by reversing the sign of every edge of G ˙ . A cycle C ˙ in G ˙ is positive if the product of its edge signs σ ( C ˙ ) is 1. Otherwise, it is negative.

The characteristic polynomial Φ G ˙ ( x ) = i = 0 n a i x n i of G ˙ is the characteristic polynomial of A G ˙ . To designate the signed graph, we occasionally write a i ( G ˙ ) for the corresponding coefficients. Similarly, the determinant det ( G ˙ ) of G ˙ is the determinant of A G ˙ , meaning det ( G ˙ ) = ( 1 ) n a 0 = ( 1 ) n i = 1 n λ i , i.e., det ( G ˙ ) equals the product of the eigenvalues taken with multiplicities. We say that G ˙ is singular if its determinant is zero, or if zero is one of its eigenvalues.

We recall that the coefficients of the characteristic polynomial can be computed by the Sachs formula for signed graphs [1]. Accordingly, a basic figure in a signed graph is a disjoint union of edges and cycles (without isolated vertices), and

(1) a i = B i ( 1 ) p ( B ) 2 c ( B ) σ ( B ) ,

where i is the set of basic figures on i vertices in G , p ( B ) is the number of components of B , c ( B ) is the set of cycles in B and σ ( B ) = C ˙ c ( B ) σ ( C ˙ ) .

Therefore, we have noted two possible ways to compute the determinant det ( G ˙ ) : the first is based on the eigenvalues, and the second is based on basic figures. In this work, we put focus on vertex-deleted subgraphs of G ˙ and express det ( G ˙ ) in terms of their eigenvalues. (A vertex-deleted subgraph is obtained by removing a single vertex from G ˙ and all edges incident to it.) Particular cases concerning vertex-deleted subgraphs without repeated eigenvalues and singular vertex-deleted subgraphs are considered. We also compute the determinant of two standard products, the tensor product and the Cartesian product, of signed graphs in terms of the eigenvalues of the corresponding graphs.

We recall from the study by Zaslavsky [2] that a fundamental operation on signed graphs is switching. It means reversing the sign of every edge located between a vertex subset and its complement. Signed graphs obtained in this way are said to be switching equivalent, and they share the same spectrum. Consequently, they share the same determinant. This means that once we have computed the determinant of a single signed graph, it remains unchanged for the entire switching class. Since an ordinary graph is interpreted as a signed graph, the results obtained in this study remain valid for ordinary graphs and also for signed graphs that are switching equivalent to them; they are also known as balanced signed graphs. Even more, signed graphs are switching isomorphic if one of them is isomorphic to a signed graph that switches to the other one. Again, the determinant is unchanged.

We apply our results to derive several consequences. First, an algorithm for the determinant of a signed graph with pendant edges is provided. Next, the determinant of an ordinary bicyclic graph and an ordinary chain graph is computed (definitions of these graphs are given in the last section). Finally, we show that the polynomial reconstruction of a chain graph from the collection of characteristic polynomials of its vertex-deleted subgraphs is unique.

In relation to our results on bicyclic graphs, we observe that the determinant of a tree is ( 1 ) n 2 if it has a perfect matching and 0 otherwise, while the determinant of a unicyclic graph is computed in the study by Simić and Stanić [3] (see also [4]), and thus, the result reported in this article figures as the next natural step.

Concerning the polynomial reconstruction, it is worth mentioning that this is a challenging open problem considered in many references published in the last 50 years, so far without any counterexample [4].

Finally, the results obtained in this article can be compared to the results obtained in the study by Liu and You [5] where the authors computed the nullity of a signed bicyclic graph, i.e., the multiplicity of zero in the corresponding spectrum. Evidently, the nullity is nonzero if and only if the same holds for the determinant.

Our terminology is standard, and some notation is introduced in the following sections. For undefined notions, we refer to [2,6].

In Section 2, we compute the determinant of G ˙ . Section 3 is devoted to the aforementioned applications.

2 Determinant of G ˙

We start this section by recalling a lemma that will be needed in the sequel.

Lemma 2.1

[7] Let G ˙ be obtained from a signed graph H ˙ of order n 1 by adding a new vertex whose neighborhood in H ˙ is determined by the characteristic ( 0 , 1 , 1 ) -vector r . The characteristic polynomial of G ˙ is given as follows:

Φ G ˙ ( x ) = Φ H ˙ ( x ) x i = 1 m Q i r 2 x μ i ,

where μ 1 , μ 2 , , μ m are the distinct eigenvalues of H ˙ and Q 1 , Q 2 , , Q m are the matrices of the orthogonal projections of R n 1 onto the eigenspaces of H ˙ with respect to the canonical basis.

Next, we express det ( G ˙ ) in terms of eigenvalues of its vertex-deleted subgraph.

Theorem 2.2

Let G ˙ be a signed graph of order n and H ˙ a subgraph obtained by deleting a vertex whose neighborhood in H ˙ is determined by the characteristic ( 0 , 1 , 1 ) -vector r . If μ 1 , μ 2 , , μ k are distinct eigenvalues of H ˙ and m 1 , m 2 , , m k are their multiplicities, then the determinant of G ˙ is

(2) det ( G ˙ ) = i = 1 k α i μ i m i 1 j i μ j m j ,

where α i = j = 1 m i ( r x j i ) 2 and x 1 i , x 2 i , , x m i i are mutually orthogonal unit vectors that make an eigenbasis of μ i .

Proof

The orthogonal projection of R n 1 onto the eigenspace of μ i is realized by the matrix Q i = j = 1 m i x j i x i j [6, p. 11]. It follows

Q i r 2 = j = 1 m i x j i x j i r j = 1 m i x j i x j i r = r j = 1 m i x j i x j i j = 1 m i x j i x j i r = r j = 1 m i x j i x j i j = 1 m i x j i x j i r = r j = 1 m i x j i x j i x j i x j i r = r j = 1 m i x j i x j i r = j = 1 m i ( r x j i ) 2 = α i ,

where the fourth equality follows since distinct eigenvectors are mutually orthogonal, and the fifth equality follows since the eigenvectors are unit. If m H ˙ ( x ) denotes the minimal polynomial of H ˙ , then on the basis of Lemma 2.1, we compute

Φ G ˙ ( x ) = Φ H ˙ ( x ) x i = 1 k α i x μ i = x Φ H ˙ ( x ) Φ H ˙ ( x ) m H ˙ ( x ) i = 1 k α i j i ( x μ j ) .

In particular, this means that the constant term a n of Φ G ˙ ( x ) is equal to the constant term of Φ H ˙ ( x ) m H ˙ ( x ) i = 1 k α i j i ( x μ j ) , and thus

a n = ( 1 ) n 1 i = 1 k μ i m i ( 1 ) k i = 1 k μ i i = 1 k α i ( 1 ) k 1 j i μ j = ( 1 ) n 1 i = 1 k μ i m i 1 i = 1 k α i j i μ j = ( 1 ) n 1 i = 1 k α i μ i m i 1 j i μ j m j .

The desired result follows from det ( G ˙ ) = ( 1 ) n a n .□

There are some consequences of Theorem 2.2.

Corollary 2.3

Let G ˙ and H ˙ be as in Theorem 2.2.

  1. If H ˙ has no repeated eigenvalues, then

    det ( G ˙ ) = i = 1 n 1 α i j i μ j .

  2. If 0 is an eigenvalue of H ˙ , then

    det ( G ˙ ) = ( r x ) 2 μ j 0 μ j m j , if 0 i s s i m p l e , 0 , otherwise,

    where x is a unit eigenvector associated with 0.

  3. det ( G ˙ ) i = 1 k d m i μ i m i 1 j i μ j m j , where d is the degree of the deleted vertex.

  4. If G ˙ is nonsingular and each of its vertex-deleted subgraph is singular, then det ( G ˙ ) 2 n Δ a n 2 ( G ˙ ) , where Δ is the maximum vertex degree in G ˙ . Equality holds if G ˙ is regular and r is an eigenvector to zero in every vertex-deleted subgraph.

Proof

Item (i) follows by setting m i = 1 , for 1 i k , in equation (2) when we also have k = n 1 .

For (ii), if 0 is a nonsimple eigenvalue of H ˙ , then the right-hand side of equation (2) is 0; this assertion follows from the interlacing theorem as well. If 0 is a simple eigenvalue, the right-hand side of equation (2) reduces to exactly one term given in the formulation of this corollary, and we are done.

Under the notation of Theorem 2.2, we have α i = j = 1 m i ( r x j ) 2 d m i , by the Cauchy-Schwarz inequality, which leads to (iii).

For (iv), by the interlacing theorem, 0 is a simple eigenvalue in every vertex-deleted subgraph. Substituting μ j 0 μ j m j = ( 1 ) n 2 a n 2 ( G ˙ v ) in (ii) of this statement, we arrive at det ( G ˙ ) = ( 1 ) n 1 ( r x ) 2 a n 2 ( G ˙ v ) , giving det ( G ˙ ) d v a n 2 ( G ˙ v ) , by (iii). An other consequence of the latter equality is that the terms a n 2 ( G ˙ v ) have the same sign for every v of G ˙ . Summing over the vertex set V ( G ˙ ) , we obtain

n det ( G ˙ ) Δ v V ( G ˙ ) a n 2 ( G ˙ v ) = Δ v V ( G ˙ ) a n 2 ( G ˙ v ) = 2 Δ a n 2 ( G ˙ ) ,

where the latter equality follows from Φ G ˙ ( x ) = v V ( G ˙ ) Φ G ˙ v ( x ) (cf. [6, Theorem 2.3.1]). The equality holds if Δ is the common vertex degree in G ˙ (i.e., if G ˙ is regular) and the equality is attained in the Cauchy-Schwarz inequality (i.e., if r and x are linearly dependent) which gives the desired assertion.□

We proceed with determinants of two products. Let G ˙ 1 and G ˙ 2 be signed graphs with eigenvalues λ 1 , λ 2 , , λ n 1 and μ 1 , μ 2 , , μ n 2 , respectively. The vertex set of the tensor product G ˙ 1 × G ˙ 2 is the Cartesian product V ( G ˙ 1 ) × V ( G ˙ 2 ) , and two vertices ( u 1 , u 2 ) and ( v 1 , v 2 ) are adjacent if and only if u i is adjacent to v i in G ˙ i , for 1 i 2 ; the edge sign is σ ( u 1 v 1 ) σ ( u 2 v 2 ) . The Cartesian product G ˙ 1 G ˙ 2 has the same vertex set, and the vertices are adjacent if and only if either u 1 = v 1 and u 2 is adjacent to v 2 in G ˙ 2 or u 2 = v 2 and u 1 is adjacent to v 1 in G 1 ; the edge sign is either σ ( u 2 v 2 ) or σ ( u 1 v 1 ) . We know from [6, p. 45] that the eigenvalues of G ˙ 1 × G ˙ 2 (resp. G ˙ 1 G ˙ 2 ) are λ i μ j (resp. λ i + μ j ), for 1 i n 1 , and 1 j n 2 . This leads to the next result.

Theorem 2.4

Let G ˙ 1 and G ˙ 2 be the signed graphs with eigenvalues λ 1 , λ 2 , , λ n 1 and μ 1 , μ 2 , , μ n 2 , respectively.

  1. The determinant of G ˙ 1 × G ˙ 2 is ( λ 1 λ 2 λ n 1 ) n 2 ( μ 1 μ 2 μ n 2 ) n 1 .

  2. The determinant of G ˙ 1 G ˙ 2 is

    ( 1 ) n 1 + n 2 i = 1 n 1 Φ G ˙ 2 ( λ i ) = ( 1 ) n 1 + n 2 j = 1 n 2 Φ G ˙ 1 ( μ j ) .

Proof

For (i), since the eigenvalues are λ i μ j , the determinant is computed as det ( G ˙ 1 × G ˙ 2 ) = i , j λ i μ j = ( λ 1 λ 2 λ n 1 ) n 2 ( μ 1 μ 2 μ n 2 ) n 1 .

Item (ii) can be proved by taking into account that the adjacency matrix of G ˙ 1 G ˙ 2 is A G ˙ 1 × I n 2 + I n 1 × A G ˙ 2 . Notwithstanding, we may use the eigenvalues and compute the determinant as follows:

det ( G ˙ 1 G ˙ 2 ) = i , j ( λ i + μ j ) = i , j ( λ i ( μ j ) ) = i = 1 n 1 Φ G ˙ 2 ( λ i ) ,

since the eigenvalues of G ˙ 2 are μ 1 , μ 2 , , μ n 2 . The second product follows by the symmetry.□

Note that if the spectrum of G ˙ 2 is symmetric (with respect to the origin), then Φ G ˙ 2 ( x ) = Φ G ˙ 2 ( x ) , and so, in this case, the determinant is i = 1 n 1 Φ G ˙ 2 ( λ i ) .

3 Applications

In this section, we provide several results based on the previous theorems.

3.1 An algorithm for the determinant of a bicyclic graph

We provide an algorithm for computing the determinant of a signed graph with pendant edges. It is based on the Heilbronner’s Formula: If u is a pendant vertex of G ˙ and v is its neighbor, then Φ G ˙ ( x ) = x Φ G ˙ u ( x ) Φ G ˙ u v ( x ) (see [8] for signed graphs and [6, Theorem 2.3.4] for the particular case of ordinary graphs). It follows that det ( G ˙ ) = det ( G ˙ u v ) .

Algorithm 1. Compute determinant
Require Signed graph G ˙ with n vertices and pendant edges
k = 0
while there is a pendant edge u v do
G ˙ G ˙ u v
if G ˙ has an isolated vertex
return 0
end if
k k + 1
end while
return ( 1 ) k det ( G ˙ )

Observing Algorithm 1, we note that since the search on vertices of degree 0 or 1 is linear, the time complexity depends on the complexity of computing the determinant of a reduced signed graph in the last line. Depending on the approach, it varies around O ( ( n 2 k ) 3 ) . However, one may observe that the previous procedure may reduce the initial signed graph to a comparatively small subgraph. In other words, as k is larger, the computation is simpler. Moreover, during the procedure, an isolated vertex may appear, and then the determinant is 0.

We apply Algorithm 1 to compute the determinant of an ordinary bicyclic graph, i.e., a connected graph with n vertices and n + 1 edges.

Theorem 3.1

Assume that the while loop of Algorithm 1 applied to a bicyclic graph G results in a graph H. Then, det ( G ) = ( 1 ) k det ( H ) , where det ( H ) is computed in the following way:

  1. If H has no vertices, then det ( H ) = 1 (the multiplicative identity).

  2. If H has an isolated vertex, then det ( H ) = 0 .

  3. If H is a cycle with p = n 2 k vertices, then

    det ( H ) = 2 ( ( 1 ) p 2 1 ) , if p i s e v e n , 2 , otherwise .

  4. Let H be a disjoint union of two cycles with p and q vertices, respectively. Then,

    det ( H ) = 4 , p , q odd , 4 ( ( 1 ) ( p + q ) 2 ( 1 ) p 2 ( 1 ) q 2 + 1 ) , p , q even , 4 ( ( 1 ) p 2 1 ) , p even , q odd .

  5. Let H have s vertices and consists of two cycles of length p and q, respectively, along with an internal path between them. Then,

    det ( H ) = ( 1 ) s 2 + 4 ( 1 ) ( s p q ) 2 , s even , p , q odd , 2 ( ( 1 ) s 2 ( 1 ) ( s p ) 2 ) , s , p even , q odd , 4 ( ( 1 ) s 2 ( 1 ) ( s p ) 2 ( 1 ) ( s q ) 2 + ( 1 ) ( s p q ) 2 ) , s , p , q even , 2 ( ( 1 ) ( s p ) 2 + ( 1 ) ( s q ) 2 ) , s , p , q odd , 4 ( ( 1 ) ( s p ) 2 ( 1 ) ( s p q ) 2 ) , s , p odd , q even , 0 , s odd , p , q even .

  6. Let H consists of two cycles of length p and q, sharing a common vertex. Then,

    det ( H ) = 2 ( ( 1 ) ( p + q 1 ) 2 ( 1 ) ( q 1 ) 2 ) , p even , q odd , 2 ( ( 1 ) ( p 1 ) 2 + ( 1 ) ( q 1 ) 2 ) , p , q odd , 0 , p , q even .

  7. Let H consists of two vertices and three internal paths between them having p, q, and r vertices, respectively. Then,

    det ( H ) = 2 ( ( 1 ) ( p + q + r + 2 ) 2 ( 1 ) p 2 ) , p even , q , r odd , 3 ( 1 ) ( p + q + r + 2 ) 2 2 ( ( 1 ) p 2 + ( 1 ) q 2 + ( 1 ) r 2 ) , p , q , r even , 2 ( ( 1 ) p 2 + ( 1 ) q 2 ) , p , q even , r odd , 0 , p , q , r odd .

Proof

Observe that G contains as an induced subgraph either two cycles joined by a path, two cycles with a common vertex, or three paths sharing the same endvertices. Accordingly, Algorithm 1 results in either a graph without vertices, a graph with an isolated vertex, a cycle, two disjoint cycles, or one of the aforementioned induced subgraphs. In other words, items (i)–(vii) cover all the possibilities.

It remains to compute the determinant of H . Items (i) and (ii) are obvious. The remaining ones are based on equation (1) (where i is the number of vertices in H ), and the fact that det ( H ) = ( 1 ) i a i . Now, items (iii) and (iv) follow by a direct algebraic computation. For (v)–(vii), we demonstrate the proofs of certain representative cases, while the remaining ones are considered analogously.

For (v), with p , q , and s even, there are exactly four perfect matchings in H , which gives the term 4 ( 1 ) s 2 . Removing the first (resp. second) cycle, we obtain a graph with two perfect matchings, which by equation (1) gives 4 ( 1 ) ( s p ) 2 ( 4 ( 1 ) ( s q ) 2 ). Finally, exactly one basic figure contains both cycles, giving 4 ( 1 ) ( s p q ) 2 . Summing up, we arrive at the desired result.

For (vi), with p and q odd, H has p + q 1 vertices, which is an odd number, and so H has no perfect matching. Removing any cycle, we obtain exactly one perfect matching, which by equation (1) leads to a i = 2 ( ( 1 ) ( p 1 ) 2 + ( 1 ) ( q 1 ) 2 ) = det ( H ) .

For (vii), with p even, q and r odd, two perfect matchings give the first term, and the remaining basic figure (the cycle of length q + r + 2 with the set of independent edges) gives the second one.

At the end, note that if the number of vertices in H is odd and all cycles are even, then there is no required basic figure, and det ( H ) = 0 (this occurs in (v)–(vii)).□

3.2 The determinant of a chain graph and a contribution to the polynomial reconstruction problem

A chain graph is a { 2 K 2 , C 4 , C 5 } -free graph (i.e., it does not contain the pair of nonadjacent edges, the triangle, or the pentagon as an induced subgraph). It follows that it is a bipartite graph whose color classes are partitioned into h nonempty cells, i.e., i = 1 h U i and i = 1 h V i , respectively. All vertices in U s are joined to all vertices in k = 1 h + 1 s V k for 1 s h . We know from [9,10] that the determinant of a chain graph is zero if and only if at least one cell contains at least two vertices. To compute the determinant in general case, it remains to consider the situation in which every cell contains a single vertex. This is performed in the next theorem.

Theorem 3.2

Let H be a vertex-deleted subgraph of a nonsingular chain graph G. Then,

det ( G ) = μ j 0 μ j m j , if H h a s a n i s o l a t e d v e r t e x , 1 2 μ j 0 μ j m j , otherwise,

where μ j is an eigenvalue of H.

Proof

Let u 1 , u 2 , , u h and v 1 , v 2 , , v h be the vertices of G , and assume that they correspond to the cells shown in Figure 1 (since G is nonsingular, every cell has exactly one vertex). Observe that H has an isolated vertex if and only if either H G u 1 or H G v 1 . In this case, the unit eigenvector to 0 in H takes 1 on the isolated vertex and 0 on the remaining vertices, and then the result follows from Corollary 2.3(ii).

If H G w , where w { u 1 , v 1 } , then H has a pair of nonadjacent vertices sharing the same neighborhood, and a unit eigenvector associated with zero in H takes 2 2 on one of these vertices, 2 2 on the other one, and 0 on the remaining vertices. Observing that w is adjacent to exactly one vertex of the mentioned pair, we arrive at the desired result by employing the same corollary.□

An interesting consequence of the previous result is that the product of eigenvalues of every vertex-deleted subgraph of G (defined in the theorem) is constant whenever this subgraph has no isolated vertices. Of course, the same holds for two subgraphs with an isolated vertex, even more they share the same spectrum. In what follows, we use the latter observation. Before this, we mention another detail.

Figure 1 
                  A sketch of a chain graph.
Figure 1

A sketch of a chain graph.

Remark 3.3

If H of Theorem 3.2 has an isolated vertex, then the result holds in general, so for any nonsingular graph along with unchanged proof.

The polynomial reconstruction problem, posed by Cvetković in 1973, asks whether the characteristic polynomial of a graph G with at least three vertices is uniquely determined by the collection of characteristic polynomials of its vertex-deleted subgraphs. An experienced reader will recognize this problem as a spectral counterpart to the famous Ulam’s reconstruction conjecture. Many details on the polynomial reconstruction problem, and its generalizations and relations with other problems can be found in the recent survey [4]. In particular, no counterexamples are known, the reconstruction is unique for graphs with at most 10 vertices, and the characteristic polynomial of G is determined up to the constant term ( 1 ) n det ( G ) , where n is the order of G . The conjecture has been confirmed for many graph classes, and here we contribute by proving that the polynomial reconstruction is unique for chain graphs.

Theorem 3.4

The polynomial reconstruction of chain graphs is unique.

Proof

It is sufficient to show that we are able to compute the determinant of a graph from the collection of characteristic polynomials of vertex-deleted subgraphs (the so-called polynomial deck).

First, if at least one cell of a chain graph G has more than one vertex, then there exists a vertex outside this particular cell whose removal leaves a graph in which the multiplicity of 0 is at least 2, which by the interlacing argument implies that the determinant of every graph with the same polynomial deck is 0.

If every cell contains a single vertex, then G is nonsingular. Let H be a graph that together with G , form a counterexample pair for the polynomial reconstruction problem. We have the following setting: H is bipartite, it has the same vertex degrees as G , and vertex-deleted subgraphs sharing the same characteristic polynomial are obtained by removing vertices of the same degree [4].

The color classes of a graph H are equal in size; otherwise, 0 with multiplicity at least 2 would appear in the spectrum of a vertex-deleted subgraph, which is impossible by an interlacing argument since G is nonsingular. The vertex of maximum degree (equal to the class size) in H is adjacent to a vertex of degree 1; otherwise, two vertices of maximum degree belong to the same color class of H , and then, we would arrive at a vertex-deleted subgraph with 0 of multiplicity at least 2, which is impossible.

Let w and w be vertices of maximum degree in G and H , respectively, such that G w and H w share the same characteristic polynomial. By Theorem 3.2 and Remark 3.3, G and H share the same determinant, and we are done.□

Some other unusual applications of determinants for particular classes of signed graphs can be found in [11]. In addition, we point out that walks in a signed graph are related particular products of eigenvalues, i.e., the determinant [12] (see also [13]).

  1. Funding information: None declared.

  2. Conflict of interest: Authors state no conflict of interest.

  3. Data availability statement: Data sharing is not applicable to this article as no datasets were generated or analyzed during the current study.

References

[1] F. Belardo and S. K. Simić, On the Laplacian coefficients of signed graphs, Linear Algebra Appl. 475 (2015), 94–113, DOI: https://doi.org/10.1016/j.laa.2015.02.007. 10.1016/j.laa.2015.02.007Search in Google Scholar

[2] T. Zaslavsky, Matrices in the theory of signed simple graphs, in: B. D. Acharya, G. O. H. Katona, J. Nešetřil, (Eds.), Advances in Discrete Mathematics and Applications: Mysore 2008, Ramanujan Math. Soc., Mysore, 2010, pp. 207–229.Search in Google Scholar

[3] S. K. Simić and Z. Stanić, The polynomial reconstruction of unicyclic graphs is unique, Linear Multilinear Algebra 55 (2007), no. 1, 35–43, DOI: https://doi.org/10.1080/03081080500426133. 10.1080/03081080500426133Search in Google Scholar

[4] I. Sciriha and Z. Stanić, The polynomial reconstruction problem: The first 50 years, Discrete Math. 346 (2023), no. 6, 113349, DOI: https://doi.org/10.1016/j.disc.2023.113349. 10.1016/j.disc.2023.113349Search in Google Scholar

[5] J. Liu and L. You, Further results on the nullity of signed graphs, J. Appl. Math. 2014 (2014), 483735, DOI: https://doi.org/10.1155/2014/483735. 10.1155/2014/483735Search in Google Scholar

[6] D. Cvetković, P. Rowlinson, and S. Simić, An Introduction to the Theory of Graph Spectra, Cambridge University Press, Cambridge, 2010. 10.1017/CBO9780511801518Search in Google Scholar

[7] F. Ramezani, P. Rowlinson, and Z. Stanić, More on signed graphs with at most three eigenvalues, Discuss. Math. Graph Theory 42 (2022), no. 4, 1313–1331, DOI: https://doi.org/10.7151/dmgt.2393. 10.7151/dmgt.2393Search in Google Scholar

[8] F. Belardo, E. M. Li Marzi, and S. K. Simić, Combinatorial approach for computing the characteristic polynomial of a matrix, Linear Algebra Appl. 433 (2010), no. 8–10, 1513–1523, DOI: https://doi.org/10.1016/j.laa.2010.05.010. 10.1016/j.laa.2010.05.010Search in Google Scholar

[9] C. M. da Fonseca, On the eigenvalues of some tridiagonal matrices, J. Comput. Appl. Math. 200 (2007), no. 1, 283–286, DOI: https://doi.org/10.1016/j.cam.2005.08.047. 10.1016/j.cam.2005.08.047Search in Google Scholar

[10] W. F. Trench, Eigenvalues and eigenvectors of two symmetric matrices, IMAGE Bull. Int. Linear Algebra Soc. 22 (1999), 28–29. Search in Google Scholar

[11] M. Andjelić, T. Koledin, and Z. Stanić, A note on the eigenvalue free intervals of some classes of signed threshold graphs, Spec Matrices 7 (2019), 218–225, DOI: https://doi.org/110.1515/spma-2019-0014. 10.1515/spma-2019-0014Search in Google Scholar

[12] Z. Stanić, Walks and eigenvalues of signed graphs, Spec. Matrices 11 (2023), 20230104, DOI: https://doi.org/10.1515/spma-2023-0104. 10.1515/spma-2023-0104Search in Google Scholar

[13] Z. Stanić, A note on a walk-based inequality for the index of a signed graph, Spec. Matrices 9 (2021), 19–21, DOI: https://doi.org/10.1515/spma-2020-0120. 10.1515/spma-2020-0120Search in Google Scholar

Received: 2023-12-01
Revised: 2024-02-18
Accepted: 2024-02-22
Published Online: 2024-03-25

© 2024 the author(s), published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Special Issue on Contemporary Developments in Graph Topological Indices
  2. On the maximum atom-bond sum-connectivity index of graphs
  3. Upper bounds for the global cyclicity index
  4. Zagreb connection indices on polyomino chains and random polyomino chains
  5. On the multiplicative sum Zagreb index of molecular graphs
  6. The minimum matching energy of unicyclic graphs with fixed number of vertices of degree two
  7. Special Issue on Convex Analysis and Applications - Part I
  8. Weighted Hermite-Hadamard-type inequalities without any symmetry condition on the weight function
  9. Scattering threshold for the focusing energy-critical generalized Hartree equation
  10. (pq)-Compactness in spaces of holomorphic mappings
  11. Characterizations of minimal elements of upper support with applications in minimizing DC functions
  12. Some new Hermite-Hadamard-type inequalities for strongly h-convex functions on co-ordinates
  13. Global existence and extinction for a fast diffusion p-Laplace equation with logarithmic nonlinearity and special medium void
  14. Extension of Fejér's inequality to the class of sub-biharmonic functions
  15. On sup- and inf-attaining functionals
  16. Regularization method and a posteriori error estimates for the two membranes problem
  17. Rapid Communication
  18. Note on quasivarieties generated by finite pointed abelian groups
  19. Review Articles
  20. Amitsur's theorem, semicentral idempotents, and additively idempotent semirings
  21. A comprehensive review of the recent numerical methods for solving FPDEs
  22. On an Oberbeck-Boussinesq model relating to the motion of a viscous fluid subject to heating
  23. Pullback and uniform exponential attractors for non-autonomous Oregonator systems
  24. Regular Articles
  25. On certain functional equation related to derivations
  26. The product of a quartic and a sextic number cannot be octic
  27. Combined system of additive functional equations in Banach algebras
  28. Enhanced Young-type inequalities utilizing Kantorovich approach for semidefinite matrices
  29. Local and global solvability for the Boussinesq system in Besov spaces
  30. Construction of 4 x 4 symmetric stochastic matrices with given spectra
  31. A conjecture of Mallows and Sloane with the universal denominator of Hilbert series
  32. The uniqueness of expression for generalized quadratic matrices
  33. On the generalized exponential sums and their fourth power mean
  34. Infinitely many solutions for Schrödinger equations with Hardy potential and Berestycki-Lions conditions
  35. Computing the determinant of a signed graph
  36. Two results on the value distribution of meromorphic functions
  37. Zariski topology on the secondary-like spectrum of a module
  38. On deferred f-statistical convergence for double sequences
  39. About j-Noetherian rings
  40. Strong convergence for weighted sums of (α, β)-mixing random variables and application to simple linear EV regression model
  41. On the distribution of powered numbers
  42. Almost periodic dynamics for a delayed differential neoclassical growth model with discontinuous control strategy
  43. A new distributionally robust reward-risk model for portfolio optimization
  44. Asymptotic behavior of solutions of a viscoelastic Shear beam model with no rotary inertia: General and optimal decay results
  45. Silting modules over a class of Morita rings
  46. Non-oscillation of linear differential equations with coefficients containing powers of natural logarithm
  47. Mutually unbiased bases via complex projective trigonometry
  48. Hyers-Ulam stability of a nonlinear partial integro-differential equation of order three
  49. On second-order linear Stieltjes differential equations with non-constant coefficients
  50. Complex dynamics of a nonlinear discrete predator-prey system with Allee effect
  51. The fibering method approach for a Schrödinger-Poisson system with p-Laplacian in bounded domains
  52. On discrete inequalities for some classes of sequences
  53. Boundary value problems for integro-differential and singular higher-order differential equations
  54. Existence and properties of soliton solution for the quasilinear Schrödinger system
  55. Hermite-Hadamard-type inequalities for generalized trigonometrically and hyperbolic ρ-convex functions in two dimension
  56. Endpoint boundedness of toroidal pseudo-differential operators
  57. Matrix stretching
  58. A singular perturbation result for a class of periodic-parabolic BVPs
  59. On Laguerre-Sobolev matrix orthogonal polynomials
  60. Pullback attractors for fractional lattice systems with delays in weighted space
  61. Singularities of spherical surface in R4
  62. Variational approach to Kirchhoff-type second-order impulsive differential systems
  63. Convergence rate of the truncated Euler-Maruyama method for highly nonlinear neutral stochastic differential equations with time-dependent delay
  64. On the energy decay of a coupled nonlinear suspension bridge problem with nonlinear feedback
  65. The limit theorems on extreme order statistics and partial sums of i.i.d. random variables
  66. Hardy-type inequalities for a class of iterated operators and their application to Morrey-type spaces
  67. Solving multi-point problem for Volterra-Fredholm integro-differential equations using Dzhumabaev parameterization method
  68. Finite groups with gcd(χ(1), χc (1)) a prime
  69. Small values and functional laws of the iterated logarithm for operator fractional Brownian motion
  70. The hull-kernel topology on prime ideals in ordered semigroups
  71. ℐ-sn-metrizable spaces and the images of semi-metric spaces
  72. Strong laws for weighted sums of widely orthant dependent random variables and applications
  73. An extension of Schweitzer's inequality to Riemann-Liouville fractional integral
  74. Construction of a class of half-discrete Hilbert-type inequalities in the whole plane
  75. Analysis of two-grid method for second-order hyperbolic equation by expanded mixed finite element methods
  76. Note on stability estimation of stochastic difference equations
  77. Trigonometric integrals evaluated in terms of Riemann zeta and Dirichlet beta functions
  78. Purity and hybridness of two tensors on a real hypersurface in complex projective space
  79. Classification of positive solutions for a weighted integral system on the half-space
  80. A quasi-reversibility method for solving nonhomogeneous sideways heat equation
  81. Higher-order nonlocal multipoint q-integral boundary value problems for fractional q-difference equations with dual hybrid terms
  82. Noetherian rings of composite generalized power series
  83. On generalized shifts of the Mellin transform of the Riemann zeta-function
  84. Further results on enumeration of perfect matchings of Cartesian product graphs
  85. A new extended Mulholland's inequality involving one partial sum
  86. Power vector inequalities for operator pairs in Hilbert spaces and their applications
  87. On the common zeros of quasi-modular forms for Γ+0(N) of level N = 1, 2, 3
  88. One special kind of Kloosterman sum and its fourth-power mean
  89. The stability of high ring homomorphisms and derivations on fuzzy Banach algebras
  90. Integral mean estimates of Turán-type inequalities for the polar derivative of a polynomial with restricted zeros
  91. Commutators of multilinear fractional maximal operators with Lipschitz functions on Morrey spaces
  92. Vector optimization problems with weakened convex and weakened affine constraints in linear topological spaces
  93. The curvature entropy inequalities of convex bodies
  94. Brouwer's conjecture for the sum of the k largest Laplacian eigenvalues of some graphs
  95. High-order finite-difference ghost-point methods for elliptic problems in domains with curved boundaries
  96. Riemannian invariants for warped product submanifolds in Q ε m × R and their applications
  97. Generalized quadratic Gauss sums and their 2mth power mean
  98. Euler-α equations in a three-dimensional bounded domain with Dirichlet boundary conditions
  99. Enochs conjecture for cotorsion pairs over recollements of exact categories
  100. Zeros distribution and interlacing property for certain polynomial sequences
  101. Random attractors of Kirchhoff-type reaction–diffusion equations without uniqueness driven by nonlinear colored noise
  102. Study on solutions of the systems of complex product-type PDEs with more general forms in ℂ2
  103. Dynamics in a predator-prey model with predation-driven Allee effect and memory effect
  104. A note on orthogonal decomposition of 𝔰𝔩n over commutative rings
  105. On the δ-chromatic numbers of the Cartesian products of graphs
  106. Binomial convolution sum of divisor functions associated with Dirichlet character modulo 8
  107. Commutator of fractional integral with Lipschitz functions related to Schrödinger operator on local generalized mixed Morrey spaces
  108. System of degenerate parabolic p-Laplacian
  109. Stochastic stability and instability of rumor model
  110. Certain properties and characterizations of a novel family of bivariate 2D-q Hermite polynomials
  111. Stability of an additive-quadratic functional equation in modular spaces
  112. Monotonicity, convexity, and Maclaurin series expansion of Qi's normalized remainder of Maclaurin series expansion with relation to cosine
  113. On k-prime graphs
  114. On the existence of tripartite graphs and n-partite graphs
  115. Classifying pentavalent symmetric graphs of order 12pq
  116. Almost periodic functions on time scales and their properties
  117. Some results on uniqueness and higher order difference equations
  118. Coding of hypersurfaces in Euclidean spaces by a constant vector
  119. Cycle integrals and rational period functions for Γ0+(2) and Γ0+(3)
  120. Degrees of (L, M)-fuzzy bornologies
  121. A matrix approach to determine optimal predictors in a constrained linear mixed model
  122. On ideals of affine semigroups and affine semigroups with maximal embedding dimension
  123. Solutions of linear control systems on Lie groups
  124. A uniqueness result for the fractional Schrödinger-Poisson system with strong singularity
  125. On prime spaces of neutrosophic extended triplet groups
  126. On a generalized Krasnoselskii fixed point theorem
  127. On the relation between one-sided duoness and commutators
  128. Non-homogeneous BVPs for second-order symmetric Hamiltonian systems
  129. Erratum
  130. Erratum to “Infinitesimals via Cauchy sequences: Refining the classical equivalence”
  131. Corrigendum
  132. Corrigendum to “Matrix stretching”
  133. Corrigendum to “A comprehensive review of the recent numerical methods for solving FPDEs”
Downloaded on 20.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2023-0188/html
Scroll to top button