scholarly journals Sectoriality and Essential Spectrum of Non Symmetric Graph Laplacians

2018 ◽  
Vol 13 (3) ◽  
pp. 967-983 ◽  
Author(s):  
Colette Anné ◽  
Marwa Balti ◽  
Nabila Torki-Hamza
2020 ◽  
Vol 61 ◽  
pp. C59-C74
Author(s):  
Shev Macnamara ◽  
Sergio Blanes ◽  
Arieh Iserles

An important framework for modelling and simulation of chemical reactions is a Markov process sometimes known as a master equation. Explicit solutions of master equations are rare; in general the explicit solution of the governing master equation for a bimolecular reaction remains an open question. We show that a solution is possible in special cases. One method of solution is diagonalization. The crucial class of matrices that describe this family of models are non-symmetric graph Laplacians. We illustrate how standard numerical algorithms for finding eigenvalues fail for the non-symmetric graph Laplacians that arise in master equations for models of chemical kinetics. We propose a novel way to explore the pseudospectra of the non-symmetric graph Laplacians that arise in this class of applications, and illustrate our proposal by Monte Carlo. Finally, we apply the Magnus expansion, which provides a method of simulation when rates change in time. Again the graph Laplacian structure presents some unique issues: standard numerical methods of more than second-order fail to preserve positivity. We therefore propose a method that achieves fourth-order accuracy, and maintain positivity. References A. Basak, E. Paquette, and O. Zeitouni. Regularization of non-normal matrices by gaussian noise–-the banded toeplitz and twisted toeplitz cases. In Forum of Mathematics, Sigma, volume 7. Cambridge University Press, 2019. doi:10.1017/fms.2018.29. S. Blanes, F. Casas, J. A. Oteo, and J. Ros. The magnus expansion and some of its applications. Phys. Rep., 470(5-6):151–238, 2009. doi:10.1016/j.physrep.2008.11.001. B. A. Earnshaw and J. P. Keener. Invariant manifolds of binomial-like nonautonomous master equations. SIAM J. Appl. Dyn. Sys., 9(2):568–588, 2010. doi10.1137/090759689. J. Gunawardena. A linear framework for time-scale separation in nonlinear biochemical systems. PloS One, 7(5):e36321, 2012. doi:10.1371/journal.pone.0036321. A. Iserles and S. MacNamara. Applications of magnus expansions and pseudospectra to markov processes. Euro. J. Appl. Math., 30(2):400–425, 2019. doi:10.1017/S0956792518000177. S. MacNamara. Cauchy integrals for computational solutions of master equations. ANZIAM Journal, 56:32–51, 2015. doi:10.21914/anziamj.v56i0.9345. S. MacNamara, A. M. Bersani, K. Burrage, and R. B. Sidje. Stochastic chemical kinetics and the total quasi-steady-state assumption: Application to the stochastic simulation algorithm and chemical master equation. J. Chem. Phys., 129:095105, 2008. doi:10.1063/1.2971036. S. MacNamara and K. Burrage. Stochastic modeling of naive T cell homeostasis for competing clonotypes via the master equation. SIAM Multiscale Model. Sim., 8(4):1325–1347, 2010. S. MacNamara, K. Burrage, and R. B. Sidje. Multiscale modeling of chemical kinetics via the master equation. SIAM Multiscale Model. and Sim., 6(4):1146–1168, 2008. doi:10.1137/060678154. S. MacNamara, Wi. McLean, and K. Burrage. Wider contours and adaptive contours, pages 79–98. Springer International Publishing, 2019. doi:10.1007/978-3-030-04161-8_7. M. J. Shon. Trapping and manipulating single molecules of DNA. PhD thesis, Harvard University, 2014. http://nrs.harvard.edu/urn-3:HUL.InstRepos:11744428. M. J. Shon and A. E. Cohen. Mass action at the single-molecule level. J. Am. Chem. Soc., 134(35):14618–14623, 2012. doi:10.1021/ja3062425. C. Timm. Random transition-rate matrices for the master equation. Phys. Rev. E, 80(2):021140, 2009. doi:10.1103/PhysRevE.80.021140. L. N. Trefethen and M. Embree. Spectra and pseudospectra: The behavior of nonnormal matrices and operators. Princeton University Press, 2005. https://press.princeton.edu/books/hardcover/9780691119465/spectra-and-pseudospectra.


2008 ◽  
Vol 15 (03) ◽  
pp. 379-390 ◽  
Author(s):  
Xuesong Ma ◽  
Ruji Wang

Let X be a simple undirected connected trivalent graph. Then X is said to be a trivalent non-symmetric graph of type (II) if its automorphism group A = Aut (X) acts transitively on the vertices and the vertex-stabilizer Av of any vertex v has two orbits on the neighborhood of v. In this paper, such graphs of order at most 150 with the basic cycles of prime length are investigated, and a classification is given for such graphs which are non-Cayley graphs, whose block graphs induced by the basic cycles are non-bipartite graphs.


2008 ◽  
Vol 18 (01) ◽  
pp. 219-225 ◽  
Author(s):  
DANIEL TURZÍK ◽  
MIROSLAVA DUBCOVÁ

We determine the essential spectrum of certain types of linear operators which arise in the study of the stability of steady state or traveling wave solutions in coupled map lattices. The basic tool is the Gelfand transformation which enables us to determine the essential spectrum completely.


2004 ◽  
Vol 2004 (1) ◽  
pp. 25-44 ◽  
Author(s):  
Fu-Zhou Gong ◽  
Feng-Yu Wang

Using a functional inequality, the essential spectrum and eigenvalues are estimated for Laplace-type operators on Riemannian vector bundles. Consequently, explicit upper bounds are obtained for the dimension of the correspondingL 2-harmonic sections. In particular, some known results concerning Gromov's theorem and theL 2-Hodge decomposition are considerably improved.


2003 ◽  
Vol 475 ◽  
pp. 377-408 ◽  
Author(s):  
SERAFIM KALLIADASIS ◽  
ALLA KIYASHKO ◽  
E. A. DEMEKHIN

We consider the motion of a liquid film falling down a heated planar substrate. Using the integral-boundary-layer approximation of the Navier–Stokes/energy equations and free-surface boundary conditions, it is shown that the problem is governed by two coupled nonlinear partial differential equations for the evolution of the local film height and temperature distribution in time and space. Two-dimensional steady-state solutions of these equations are reported for different values of the governing dimensionless groups. Our computations demonstrate that the free surface develops a bump in the region where the wall temperature gradient is positive. We analyse the linear stability of this bump with respect to disturbances in the spanwise direction. We show that the operator of the linearized system has both a discrete and an essential spectrum. The discrete spectrum bifurcates from resonance poles at certain values of the wavenumber for the disturbances in the transverse direction. The essential spectrum is always stable while part of the discrete spectrum becomes unstable for values of the Marangoni number larger than a critical value. Above this critical Marangoni number the growth rate curve as a function of wavenumber has a finite band of unstable modes which increases as the Marangoni number increases.


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