getdoc3797. 222KB Jun 04 2011 12:04:15 AM
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First we note that the construction of the A -process for all time is trivial, since the A -particles by themselves merely perform independent continuous time simple random walks..
Let G = (V, E) be a finite graph 3. We wish to sample from π by running a reversible MC on S , but allow only transitions that change the state of one node at a time, i.e. We
We give a characterization of stochastic order between different interacting particle systems in a large class of processes with births, deaths and jumps of many particles per
Although the exact convergence rate remains unknown for Wigner matrices, Bai and Yao [ 6 ] proved that the spectral empirical process of Wigner matrices indexed by a set of
We prove that if the particle hopping rates of this process are in a particular relation with the densities of the initial measure then the distribution of this process at any time t
the time reversed process is a drifted fractional Brownian motion, which continuously extends the one obtained in the theory of time reversal of Brownian diffusions when H = 1/2..
We prove that a stochastic flow of reflected Brownian motions in a smooth multidimensional domain is differentiable with respect to its initial position.. The derivative is a linear
Given a remarkable representation of the generalized Pauli operators of two- qubits in terms of the points of the generalized quadrangle of order two, W (2), it is shown that
