sigma05-025. 250KB Jun 04 2011 12:09:47 AM
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Figure 1: Three basically different posibilities in coupling continuous and discrete processes: in case ( a ) the continuous one moves while the discrete one does not change, in case
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
The accuracy of our results depends primarily upon an inequality pertaining to the number of event recurrences, as given in Klass and Nowicki (2003), a corollary of which extends
(Ordinary differential equations constitute a special case; we will mention those later.) We define the partial derivatives of the dependent variables as new variables (prolongation)
It is not surprising, because the equation can be integrated by the inverse scattering method or, in other words, it is S-integrable, it is well known in the case of
This method, which does not use Noether’s Theorem, has been used to calculate some low-order conservation laws of various integrable difference equations that are defined on
The fermion- antifermion operators generate a unitary Lie algebra, whose representations are fixed by a first order Casimir operator (corresponding to baryon number or
Key words: antisymmetric orbit functions; signed orbits; products of orbits; orbit function transform; finite orbit function transform; finite Fourier transforms; finite
