• Tidak ada hasil yang ditemukan

getdoc4bad. 181KB Jun 04 2011 12:04:21 AM

N/A
N/A
Protected

Academic year: 2017

Membagikan "getdoc4bad. 181KB Jun 04 2011 12:04:21 AM"

Copied!
20
0
0

Teks penuh

Loading

Gambar

Figure 1: Three basically different posibilities in coupling continuous and discrete processes: incase (a) the continuous one moves while the discrete one does not change, in case (b) they stayapproximately aligned, and in case (c) the discrete one overtakes the continuous one.
Table 2: Numerical values of wˆnn
Figure 2: The evolution of the distance between two coupled processes

Referensi

Dokumen terkait

We prove that one characterization for the classical orthogonal polynomials sequences (Hermite, Laguerre, Jacobi and Bessel) cannot be extended to the semi-classical ones..

A class of discrete renewal processes with exponentially decaying inter-arrival distributions coincides with the infinite volume limit of general homogeneous pinning models in

Abstract A common technique in the theory of stochastic process is to replace a discrete time coordinate by a continuous randomized time, defined by an independent Poisson or

A construction of processes with one-dimensional martingale marginals, associated with a Lévy process, via its Lévy sheet.. Self-similar processes with independent increments

We also mention that a different connection linking L´evy processes with no negative jumps to continuous state branching processes has recently been pointed out by Le Gall and Le

A Central Limit Theorem for non-commutative random variables is proved using the Lindeberg method.. The theorem is a generalization of the Central Limit Theorem for free random

Roughly speaking, the Krawtchouk process is a system of non-colliding random walks in discrete time and the Charlier process is the continuous-time analogue (but note that they

To change the velocity of the massless charge the energy is necessary which is too large to be observed, while non-accelerated photon-like charge does not generate the