Results 111 to 120 of about 302,460 (378)
Constructing graphs having Laplacian pair state transfer by an edge perturbation [PDF]
In this paper, we give some sufficient conditions for graphs with an edge perturbation between twin vertices to have Laplacian perfect pair state transfer as well as Laplacian pretty good pair state transfer. By those sufficient conditions, we also construct many new graphs having Laplacian perfect pair state transfer as well as Laplacian pretty good ...
arxiv
AbstractWe present a simple geometric interpretation of the Laplacian of a graph including the interpretation of the Laplacian eigenvectors.
openaire +2 more sources
Localized and Extended Phases in Square Moiré Patterns
Rotated superimposed lattices in two dimensions, the termed moiré patterns, represent a clear example of how the structure affects the physical properties of a particle moving on it. A robust numerical treatment of continuous and discrete models leads to confirm that while localized states result from angles that produce non‐commensurable lattices ...
C. Madroñero+2 more
wiley +1 more source
Laplacian state transfer in vertex complemented coronas [PDF]
In this paper, we investigate the existence of Laplacian perfect state transfer and Laplacian pretty good state transfer in vertex complemented coronas. We prove that there is no Laplacian perfect state transfer in vertex complemented coronas. In contrast, we give a sufficient condition for vertex complemented coronas to have Laplacian pretty good ...
arxiv
A Generalized Fractional Laplacian
In this article we show that the fractional Laplacian in $R^{2}$ can be factored into a product of the divergence operator, a Riesz potential operator, and the gradient operator. Using this factored form we introduce a generalization of the fractional Laplacian, involving a matrix $K(x)$, suitable when the fractional Laplacian is applied in a non ...
Zheng, Xiangcheng+2 more
openaire +2 more sources
Signless Laplacian energy of a first KCD matrix
The concept of first KCD signless Laplacian energy is initiated in this article. Moreover, we determine first KCD signless Laplacian spectrum and first KCD signless Laplacian energy for some class of graphs and their complement.
Mirajkar Keerthi G., Morajkar Akshata
doaj +1 more source
This article focuses on the fully distributed leader‐following consensus problem of nonlinear fractional multi‐agent systems via event‐triggered control technique. The main intention of this article is to design a novel event‐triggered mechanism, which not only takes into account both the relative error and the absolute error of the samples but also ...
Qiaoping Li, Chao Yue
wiley +1 more source
On the construction of L-equienergetic graphs
For a graph G with n vertices and m edges, and having Laplacian spectrum μ1,μ2,…,μn and signless Laplacian spectrum μ1+,μ2+,…,μn+, the Laplacian energy and signless Laplacian energy of G are respectively, defined as LE(G)=∑i=1n|μi−2mn| and LE+(G)=∑i=1n ...
S. Pirzada, Hilal A. Ganie
doaj +1 more source
The multiplicity of the zero Laplacian eigenvalue of uniform hypertrees [PDF]
In this paper, the Laplacian characteristic polynomial of uniform hypergraphs with cut vertices or pendant edges and the Laplacian matching polynomial of uniform hypergraphs are characterized.The multiplicity of the zero Laplacian eigenvalue of uniform hypertrees is given, which proves the conjecture in \cite{zheng2023zero} (The zero eigenvalue of the ...
arxiv
AbstractWe give complete descriptions of the various spectra of the minimal and maximal operators of the Laplacian on the upper half space and the unit ball. The results are in sharp contrast with the corresponding ones on the whole space. An application to the existence or nonexistence of nontrivial solutions of the Helmholtz equation is given.
openaire +2 more sources