Pursuing faster convergence rates and smaller input magnitudes seem to be two conflicting goals in studying multi-agent systems. To give a trade-off between the two, this paper focuses on the bipartite synchronization...
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Within the cubic nonlinear approximation framework we performed the analysis of space charge waves (SCWs) with broad frequency spectrum amplification in superheterodyne free electron laser (FEL) with longitudinal elec...
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The global-in-time energy estimate is derived for the second-order accurate exponential time differencing Runge–Kutta (ETDRK2) numerical scheme to the phase field crystal (PFC) equation, a sixth-order parabolic equat...
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In many practical situations, practitioners use easier-to-compute fuzzy control to approximate the more-difficult-to-compute optimal control. As expected, for many characteristics, this approximate control is slightly...
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Nanoscale multilayer TiSiN/NbN coatings with a modulation period ranging from 75 to 50 nm were deposited onto steel using the cathodic arc physical vapor deposition technique. The microstructure of multilayer TiSiN/Nb...
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The distribution of the volcanoes in indonesia gives positive impacts in the form of fertile land where many residents live to grow crops. Besides having positive impacts, there are also negative impacts in the form o...
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In a quantum communication network, links represent entanglement between qubits located at different nodes. Even if two nodes are not directly linked by shared entanglement, they can still communicate via routing prot...
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In a quantum communication network, links represent entanglement between qubits located at different nodes. Even if two nodes are not directly linked by shared entanglement, they can still communicate via routing protocols. However, in contrast to classical communication, each quantum communication event removes all participating links along the routed path, disrupting the quantum communication network. Here, we propose a simple model, where randomly selected pairs of nodes communicate through the shortest paths. Each time such a path is used, all participating links are eliminated, leading to a correlated percolation process that we call “path percolation.” We study path percolation both numerically and analytically and present the phase diagram of the steady states as a function of the rate at which new links are being added to the network. As a key result, the steady state is found to be independent of the initial network topologies when new links are added randomly between disconnected components. We close by discussing extensions of path percolation and link replenishment, along with their potential applications.
Continuous-time algebraic Riccati equations can be found in many disciplines in different forms. In the case of small-scale dense coefficient matrices, stabilizing solutions can be computed to all possible formulation...
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Demonstrating new asymptotic behavior u − u1 = o(1) at infinity, we employ the Perron method to establish the existence of ancient solutions to exterior Dirichlet problems associated with the parabolic Monge–Amp`ere ...
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In this work, we consider the H2 optimal model reduction of dynamical systems that are linear in the state equation and up to quadratic nonlinearity in the output equation. As our primary theoretical contributions, we...
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