679 research outputs found

    Long-time behavior of stochastic model with multi-particle synchronization

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    We consider a basic stochastic particle system consisting of NN identical particles with isotropic kk-particle synchronization, kβ‰₯2k\geq 2. In the limit when both number of particles NN and time t=t(N)t=t(N) grow to infinity we study an asymptotic behavior of a coordinate spread of the particle system. We describe three time stages of t(N)t(N) for which a qualitative behavior of the system is completely different. Moreover, we discuss the case when a spread of the initial configuration depends on NN and increases to infinity as Nβ†’βˆžN\to \infty .Comment: 9 pages, 1 figure; one reference and one figure added, typos corrected, minor improvements of the proof

    Positivity of transition probabilities of infinite-dimensional diffusion processes on ellipsoids

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    We consider diffusion processes in Hilbert spaces with constant non-degenerate diffusion operators and show that, under broad assumptions on the drift, the transition probabilities of the process are positive on ellipsoids associated with the diffusion operator. This is an infinite-dimensional analogue of positivity of densities of transition probabilities. Our results apply to diffusions corresponding to stochastic partial differential equations.Comment: 12 pages; to appear in Theory of Stochastic Processe

    Controlling of clock synchronization in WSNs: structure of optimal solutions

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    Energy-saving optimization is very important for various engineering problems related to modern distributed systems. We consider here a control problem for a wireless sensor network with a single time server node and a large number of client nodes. The problem is to minimize a functional which accumulates clock synchronization errors in the clients nodes and the energy consumption of the server over some time interval [0,T][0,T]. The control function u=u(t)u=u(t), 0≀u(t)≀u10\leq u(t)\leq u_{1}, corresponds to the power of the server node transmitting synchronization signals to the clients. For all possible parameter values we find the structure of optimal trajectories. We show that for sufficiently large u1u_{1} the solutions contain singular arcs.Comment: 14 pages, 6 figure

    Time Scales in Probabilistic Models of Wireless Sensor Networks

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    We consider a stochastic model of clock synchronization in a wireless network consisting of N sensors interacting with one dedicated accurate time server. For large N we find an estimate of the final time sychronization error for global and relative synchronization. Main results concern a behavior of the network on different time scales t=tNβ†’βˆžt=t_N \to \infty, Nβ†’βˆžN \to \infty. We discuss existence of phase transitions and find exact time scales on which an effective clock synchronization of the system takes place.Comment: 31 page

    Intrinsic scales for high-dimensional LEVY-driven models with non-Markovian synchronizing updates

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    We propose stochastic NN-component synchronization models (x1(t),...,xN(t))(x_{1}(t),...,x_{N}(t)), xj∈Rdx_{j}\in\mathbb{R}^{d}, t∈R+t\in\mathbb{R}_{+}, whose dynamics is described by Levy processes and synchronizing jumps. We prove that symmetric models reach synchronization in a stochastic sense: differences between components dkj(N)(t)=xk(t)βˆ’xj(t)d_{kj}^{(N)}(t)=x_{k}(t)-x_{j}(t) have limits in distribution as tβ†’βˆžt\rightarrow\infty. We give conditions of existence of natural (intrinsic) space scales for large synchronized systems, i.e., we are looking for such sequences {bN}\{b_{N}\} that distribution of dkj(N)(∞)/bNd_{kj}^{(N)}(\infty)/b_{N} converges to some limit as Nβ†’βˆžN\rightarrow\infty. It appears that such sequence exists if the Levy process enters a domain of attraction of some stable law. For Markovian synchronization models based on Ξ±\alpha-stable Levy processes this results holds for any finite NN in the precise form with bN=(Nβˆ’1)1/Ξ±b_{N}=(N-1)^{1/\alpha}. For non-Markovian models similar results hold only in the asymptotic sense. The class of limiting laws includes the Linnik distributions. We also discuss generalizations of these theorems to the case of non-uniform matrix-based intrinsic scales. The central point of our proofs is a representation of characteristic functions of dkj(N)(t)d_{kj}^{(N)}(t) via probability distribution of a superposition of NN independent renewal processes.Comment: 50 page

    Optimal chattering solutions for longitudinal vibrations of a nonhomogeneous bar

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    We consider a control problem for longitudinal vibrations of a nonhomogeneous bar with clamped ends. The vibrations of the bar are controlled by an external force which is distributed along the bar. For the minimization problem of mean square deviation of the bar we prove that the optimal control has an infinite number of switchings in a finite time interval, i.e., the optimal control is the chattering control.Comment: 12 page

    Estimates for Kantorovich functionals between solutions to Fokker -- Planck -- Kolmogorov equations with dissipative drifts

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    We obtain estimates for the Kantorovich functionals between solutions to different Fokker -- Planck -- Kolmogorov equations for measures with same diffusion part but different drifts and different initial conditions. We show possible applications of such estimates to the study of the well-posedness for nonlinear equations.Comment: 13 pages; revised, extended to a more general case, minor mistaked correcte

    Asymptotic analysis of a particle system with mean-field interaction

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    We study a system of NN interacting particles on Z\bf{Z}. The stochastic dynamics consists of two components: a free motion of each particle (independent random walks) and a pair-wise interaction between particles. The interaction belongs to the class of mean-field interactions and models a rollback synchronization in asynchronous networks of processors for a distributed simulation. First of all we study an empirical measure generated by the particle configuration on R\bf{R}. We prove that if space, time and a parameter of the interaction are appropriately scaled (hydrodynamical scale), then the empirical measure converges weakly to a deterministic limit as NN goes to infinity. The limit process is defined as a weak solution of some partial differential equation. We also study the long time evolution of the particle system with fixed number of particles. The Markov chain formed by individual positions of the particles is not ergodic. Nevertheless it is possible to introduce relative coordinates and to prove that the new Markov chain is ergodic while the system as a whole moves with an asymptotically constant mean speed which differs from the mean drift of the free particle motion.Comment: 31 pages; added references, section 5 and appendix; corrected typo

    Phase transitions in the time synchronization model

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    We continue the study of the time synchronization model from arXiv:1201.2141 . There are two types i=1,2i=1,2 of particles on the line RR, with NiN_{i} particles of type ii. Each particle of type ii moves with constant velocity viv_{i}. Moreover, any particle of type i=1,2i=1,2 jumps to any particle of type j=1,2j=1,2 with rates Njβˆ’1Ξ±ijN_{j}^{-1}\alpha_{ij}. We find phase transitions in the clusterization (synchronization) behaviour of this system of particles on different time scales t=t(N)t=t(N) relative to N=N1+N2N=N_{1}+N_{2}.Comment: 10 pages; first published in Theory Probab. Appl. 50, pp. 134-141 (2006); small corrections in text of the paper; bibliography update

    Dynamics of Phase Boundary with Particle Annihilation

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    Infinitely many particles of two types ("plus" and "minus") jump randomly along the one-dimensional lattice ZΞ΅=Ξ΅Z\mathbf{Z}_{\varepsilon}=\varepsilon\mathbf{Z}. Annihillations occur when two particles of different time occupy the same site. Assuming that at time t=0t=0 all "minus" particles are placed on the left of the origin and all "plus" particles are on the right of it, we study evolution of Ξ²Ξ΅(t)\beta_\varepsilon(t), the boundary between two types. We prove that in large density limit Ο΅β†’0\epsilon\to 0 the boundary Ξ²Ξ΅(t)\beta_\varepsilon(t) converges to a deterministic limit. This particle system can be interpreted as a microscopic model of price formation on economic markets with large number of players
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