Academia.edu no longer supports Internet Explorer.
To browse Academia.edu and the wider internet faster and more securely, please take a few seconds to upgrade your browser.
2007, Journal of Mathematical Inequalities
The eigenvalues of a graph are the eigenvalues of its adjacency matrix. The energy of a graph is the sum of absolute values of its eigenvalues. Recently, the concept of energy of graphs is extended to digraphs. Minimal and maximal energy among n-vertex unicyclic digraphs is known, where n 2. In this paper, we address the problem of finding minimal and maximal energy among n-vertex bicyclic digraphs which contain vertex-disjoint directed cycles, where n 4 .
Asian-European Journal of Mathematics, 2019
The energy of a weighted digraph [Formula: see text] is the sum of absolute values of real part of its eigenvalues. Recently, the minimal and maximal energy of unicyclic weighted digraphs with cycle weight [Formula: see text] is studied. In this paper, we introduce a class [Formula: see text] of those bicyclic weighted digraphs of fixed order which contain vertex-disjoint weighted cycles of weights [Formula: see text] or [Formula: see text] and [Formula: see text] or [Formula: see text], where [Formula: see text]. We find digraphs in [Formula: see text] under certain conditions on [Formula: see text] and [Formula: see text] with extremal energy.
Applied Mathematics and Computation, 2016
If D is a digraph with n vertices then the energy of D is defined as E (D) = n k=1 |Re(z k)|, where Re (z1),. .. , Re(z n) are the real parts of the eigenvalues z 1 ,. .. , z n of D. In this paper we solve a problem proposed in Khan et al. (2015), we find the maximal value of the energy over the set of all bicyclic digraphs B n with n vertices.
Kragujevac Journal of Mathematics, 2016
The eigenvalues of a digraph are the eigenvalues of its adjacency matrix. The sum of the absolute values of the real part of the eigenvalues is called the energy of the digraph. The extremal energy of bicyclic digraphs with vertex-disjoint directed cycles is known. In this paper, we consider a class of bicyclic digraphs with exactly two linear subdigraphs of equal length. We find the minimal and maximal energy among the digraphs in this class.
Applied Mathematics and Computation, 2019
The energy of a digraph (sidigraph) is defined as the sum of absolute values of real parts of its eigenvalues. Monsalve and Rada (2016) determined the bicyclic digraphs with maximal energy among the set of all bicyclic digraphs with fixed order. In this paper, we find the bicyclic sidigraphs with maximal energy over the set of all bicyclic sidigraphs with fixed order. We also construct few families of non-cospectral equienergetic bicyclic sidigraphs.
Applied Mathematics and Computation, 2017
The energy of an n-vertex digraph D is defined by E(D) = n k =1 | Re (z k) | , where z 1 ,. .. , z n are eigenvalues of D and Re(z k) is the real part of eigenvalue z k. Very recently, a new type of energy of digraphs has been introduced, which is known as the iota energy of digraphs. The iota energy of the digraph D is defined by E c (D) = n k =1 | Im (z k) | , where z 1 ,. .. , z n are eigenvalues of D and Im(z k) is the imaginary part of eigenvalue z k. The unicyclic digraphs with extremal iota energy are known. In this paper, we consider a class D n of n-vertex bicyclic digraphs with vertex-disjoint directed cycles and find the digraphs in D n with minimal and maximal iota energy.
Applicable Analysis and Discrete Mathematics, 2011
The energy of a digraph D is defined as E(D) = ?n,i=1 ?Re(zi)?, where z1, z2, ..., zn are the (possibly complex) eigenvalues of D . We show that if D is a strongly connected digraph on n vertices, a arcs, and c2 closed walks of length two, such that Re(z1) ? (a + c2)=(2n) ? 1 , then E(D) ? n(1 + ?n)=2. Equality holds if and only if D is a directed strongly regular graph with parameters (n, n+?n/2, 3n+2?n/8, n+2?n/8, n+2?n/8). This bound extends to digraphs an earlier result [J. H. Koolen, V. Moulton:, Maximal energy graphs. Adv. Appl. Math., 26 (2001), 47-52], obtained for simple graphs.
Journal of Combinatorial Theory, Series B, 1973
We consider directed graphs without loops and multiple edges, where the exclusion of multiple edges means that two vertices cannot be joined by two edges of the same orientation . Let L I , . . ., LQ be given digraphs . What is the maximum number of edges a digraph can have if it does not contain any L i as a subgraph and has given number of vertices? We shall prove the existence of a sequence of asymptotical extremal graphs having fairly simple structure . More exactly : There exist a matrix A = (ai,5)ij * and a sequence {S"} of graphs such that (i) the vertices of S" can be divided into classes Ct , . . ., C, so that, if i =A j, each vertex of Ci is joined to each vertex of C ; by an edge oriented from C i to C; if and only if a,, ; = 2 ; the vertices of Ci are independent if ai ,, = 0 ; and otherwise ai , , = 1 and the digraph determined by C, is a complete acyclic digraph ; (ii) S" contains no L, but any graph having [en 2 ] more edges than S" must contain at least one Li . (Here the word graph is an "abbreviation" for "directed graph or digraph.") The digraphs (= directed graphs) considered in this paper have neither loops nor multiple edges : a vertex cannot be joined to itself and the digraph cannot have two edges joining the vertices x and y and oriented
Discrete Applied Mathematics, 2014
In this paper we extend the concept of energy to signed digraphs and we obtain Coulson's integral formula for energy of signed digraphs. We compute formulae for energies of signed directed cycles and we show that energy of non cycle balanced signed directed cycles increases monotonically with respect to the number of vertices. We extend the concept of non-complete extended p sum (or briefly, NEPS) to signed digraphs. We construct infinite families of noncospectral equienergetic signed digraphs. Moreover, we extend McClelland's inequality to signed digraphs and also obtain a sharp upper bound for the energy of a signed digraph in terms of the number of arcs. Some open problems are also given at the end.
Linear and Multilinear Algebra, 2015
The set of distinct eigenvalues of a signed digraph S together with their multiplicities is called its spectrum. The energy of a signed digraph S with eigenvalues z 1 , z 2 , • • • , z n is defined as E(S) = n j=1 |ℜz j |, where ℜz j denotes real part of complex number z j. In this paper, we show that the characteristic polynomial of a bipartite signed digraph of order n with each cycle of length ≡ 0 (mod 4) negative and each cycle of length ≡ 2 (mod 4) positive is of the form φ S (z) = z n + ⌊ n 2 ⌋ j=1 (−1) j c 2j (S)z n−2j , where c 2j (S) are nonnegative integers. We define a quasi-order relation in this case and show energy is increasing. It is shown that the characteristic polynomial of a bipartite signed digraph of order n with each cycle negative has the form φ S (z) = z n + ⌊ n 2 ⌋ j=1 c 2j (S)z n−2j , where c 2j (S) are nonnegative integers. We study integral, real, Gaussian signed digraphs and quasi-cospectral digraphs and show for each positive integer n ≥ 4 there exists a family of n cospectral, non symmetric, strongly connected, integral, real, Gaussian signed digraphs (non cycle balanced) and quasi-cospectral digraphs of order 4 n. We obtain a new family of pairs of equienergetic strongly connected signed digraphs and answer to open problem (2) posed in Pirzada and Mushtaq, Energy of signed digraphs, Discrete Applied Mathematics 169 (2014) 195-205.
Discrete Applied Mathematics, 2017
Let D be a strong digraph on n ≥ 4 vertices. In [2, J. Graph Theory 22 (2) (1996) 181-187)], J. Bang-Jensen, G. Gutin and H. Li proved the following theorems: If (*) d(x) + d(y) ≥ 2n − 1 and min{d(x), d(y)} ≥ n − 1 for every pair of non-adjacent vertices x, y with a common in-neighbour or (**) min{d + (x) + d − (y), d − (x) + d + (y)} ≥ n for every pair of non-adjacent vertices x, y with a common in-neighbour or a common out-neighbour, then D is hamiltonian. In this paper we show that: (i) if D satisfies the condition (*) and the minimum semi-degree of D at least two or (ii) if D is not directed cycle and satisfies the condition (**), then either D contains a cycle of length n − 1 or n is even and D is isomorphic to complete bipartite digraph or to complete bipartite digraph minus one arc.
Asian-European Journal of Mathematics
Iota energy of signed digraphs is defined as sum of absolute values of imaginary parts of its eigenvalues. Extremal energy and iota energy of unicyclic signed digraphs is known. In this paper, we address the problem of finding signed digraphs with extremal iota energy among vertex-disjoint bicyclic signed digraphs of fixed order.
Linear and Multilinear Algebra, 2016
The eigenvalues of a digraph are the eigenvalues of its adjacency matrix. If D is a digraph of order n with eigenvalues z 1 , z 2 ,. .. , z n , then its energy is defined by E(D) = n k=1 Re(z k). We give a new notion of energy of digraphs defined by E c (D) = n k=1 Im(z k) and call it the iota energy of the digraph D. It is shown that the Coulson's integral formula remains valid for iota energy. We also find the unicyclic digraphs with extremal iota energies among the class of unicyclic digraphs with a fixed order. Furthermore, it is shown that the iota energy is increasing over the set D n,h of n-vertex digraphs with cycles of length h, with respect to a quasi-order relation. We also generalize the increasing property of the energy over the set D n,h with respect to quasi-order relation.
Asian-European Journal of Mathematics, 2019
The energy of a weighted digraph [Formula: see text] is the sum of absolute values of real part of its eigenvalues. Recently, the minimal and maximal energy of unicyclic weighted digraphs with cycle weight [Formula: see text] is studied. In this paper, we introduce a class [Formula: see text] of those bicyclic weighted digraphs of fixed order which contain vertex-disjoint weighted cycles of weights [Formula: see text] or [Formula: see text] and [Formula: see text] or [Formula: see text], where [Formula: see text]. We find digraphs in [Formula: see text] under certain conditions on [Formula: see text] and [Formula: see text] with extremal energy.
Linear and Multilinear Algebra, 2018
The eigenvalues of a signed digraph are the eigenvalues of its adjacency matrix. If S is an n-vertex signed digraph with eigenvalues z 1 ,. .. , z n then the energy of S is defined by E(S) = n k=1 |Re(z k)|, where Re(z k) is the real part of z k. Recently, the concept of iota energy of digraphs is introduced. In this paper, we extend notion of iota energy to signed digraphs. We compute iota energy formulas for the signed directed cycles. We find the unicyclic signed digraphs with extremal iota energies among the class of unicyclic signed digraphs with fixed order. Moreover, it is shown that the Coulson's integral formula remains valid for signed digraphs. We also discuss the increasing property of iota energy over some specific subclasses of the set S n,h , where the set S n,h contains n-vertex signed digraphs with cycles each of length h.
Applied Mathematics and Computation, 2019
Graph energy can be extended to digraphs via the trace norm. The trace norm of a digraph is the trace norm of its adjacency matrix, i.e. the sum of its singular values. In this work we find the oriented graphs that attain minimal and maximal trace norm over the set of oriented bicyclic graphs.
Proyecciones, 2016
The energy of a digraph is defined as E (D) = n P k=1 |Re (z k)|, where This expression for the energy has many applications in the study of extremal values of the energy in special classes of digraphs. In this paper we consider the set D * (C n) of all strongly connected digraphs whose underlying graph is the cycle C n , and characterize those whose characteristic polynomial is of the form (0.1). As a consequence, we find the extremal values of the energy based on (0.2).
Iranian journal of mathematical chemistry, 2021
The eigenvalues of a digraph are the eigenvalues of its adjacency matrix. Let $z_1,ldots,z_n$ be the eigenvalues of an $n$-vertex digraph $D$. Then we give a new notion of energy of digraphs defined by $E_p(D)=sum_{k=1}^{n}|{Re}(z_k) {Im}(z_k)|$, where ${Re}(z_k)$ (respectively, ${Im}(z_k)$) is real (respectively, imaginary) part of $z_k$. We call it $p$-energy of the digraph $D$. We compute $p$-energy formulas for directed cycles. For $ngeq 12$, we show that $p$-energy of directed cycles increases monotonically with respect to their order. We find unicyclic digraphs with smallest and largest $p$-energy. We give counter examples to show that the $p$-energy of digraph does not possess increasing--property with respect to quasi-order relation over the set $mathcal{D}_{n,h}$, where $mathcal{D}_{n,h}$ is the set of $n$-vertex digraphs with cycles of length $h$. We find the upper bound for $p$-energy and give all those digraphs which attain this bound. Moreover, we construct few families...
Asian-European Journal of Mathematics, 2018
Iota energy of signed digraphs is defined as sum of absolute values of imaginary parts of its eigenvalues. Extremal energy and iota energy of unicyclic signed digraphs is known. In this paper, we address the problem of finding signed digraphs with extremal iota energy among vertex-disjoint bicyclic signed digraphs of fixed order.
2021
The energy of a sidigraph is defined as the sum of absolute values of real parts of its eigenvalues. The iota energy of a sidigraph is defined as the sum of absolute values of imaginary parts of its eigenvalues. Recently a new notion of energy of digraphs is introduced which is called the total energy of digraphs. In this paper, we extend this concept of total energy to sidigraphs. We compute total energy formulas for negative directed cycles and show that the total energy of negative directed cycles with fixed order increases monotonically. We introduce complex adjacency matrix to give the integral representation for total energy of sidigraphs. We discuss the increasing property of total energy over some particular subfamilies of Sn,h, where Sn,h contains n-vertex sidigraphs with each cycle having length h. Using the CauchySchwarz inequality, we find upper bound for the total energy of sidigraphs. Finally, we find the class of noncospectral equienergetic sidigraphs.
The energy of a digraph D with eigenvalues z 1 , z 2 ,. .. , zn is defined as E(D) = n ∑ j=1 |ℜz j |, where ℜz j is the real part of the complex number z j. In this paper, we characterize some positive reals that cannot be the energy of a digraph. We also obtain a sharp lower bound for the energy of strongly connected digraphs.
Linear Algebra and its Applications, 2012
Let D be a digraph with vertex set V (D) and A be the adjacency matrix of D. In this paper, we characterize the extremal digraphs which achieve the maximum and minimum spectral radius among strongly connected bicyclic digraphs. Furthermore, we show that any strongly connected bicyclic digraph is determined by the spectrum.
Acta Universitatis Sapientiae, Informatica, 2021
Let S = (G, σ) be a signed graph of order n and size m and let x1, x2, ..., xn be the eigenvalues of S. The energy of S is defined as ɛ ( S ) = ∑ j = 1 n | x j | \varepsilon \left( S \right) = \sum\limits_{j = 1}^n {\left| {{x_j}} \right|} . A connected signed graph is said to be bicyclic if m=n + 1. In this paper, we determine the bicyclic signed graphs with first 20 minimal energies for all n ≥ 30 and with first 16 minimal energies for all 17 ≤ n ≤ 29.
Linear and Multilinear Algebra, 2016
The eigenvalues of a digraph are the eigenvalues of its adjacency matrix. If D is a digraph of order n with eigenvalues z 1 , z 2 ,. .. , z n , then its energy is defined by E(D) = n k=1 Re(z k). We give a new notion of energy of digraphs defined by E c (D) = n k=1 Im(z k) and call it the iota energy of the digraph D. It is shown that the Coulson's integral formula remains valid for iota energy. We also find the unicyclic digraphs with extremal iota energies among the class of unicyclic digraphs with a fixed order. Furthermore, it is shown that the iota energy is increasing over the set D n,h of n-vertex digraphs with cycles of length h, with respect to a quasi-order relation. We also generalize the increasing property of the energy over the set D n,h with respect to quasi-order relation.
Matrix Science Mathematic, 2018
The iota energy of an n-vertex digraph D is defined by Ec () = ∑ |Im(k)| =1 , where z1,. . ., zn are eigenvalues of D and Im(zk) is the imaginary part of eigenvalue zk. The iota energy of an n-vertex sidigraph can be defined analogously. In this paper, we define a class Fn of n-vertex tricyclic digraphs containing five linear subdigraphs such that one of the directed cycles does not share any vertex with the other two directed cycles and the remaining two directed cycles are of same length sharing at least one vertex. We find the digraphs in Fn with minimal and maximal iota energy. We also consider a similar class of tricyclic sidigraphs and find extremal values of iota energy among the sidigraphs in this class.
Loading Preview
Sorry, preview is currently unavailable. You can download the paper by clicking the button above.