Transport coefficients from computer experiments: A stochastic Ising model

1974 ◽  
Vol 9 (5) ◽  
pp. 2299-2310 ◽  
Author(s):  
Abdullah Sadiq
1997 ◽  
Vol 40 (8) ◽  
pp. 832-842 ◽  
Author(s):  
Dayue Chen ◽  
Jianfeng Feng ◽  
Minping Qian

1997 ◽  
Vol 40 (11) ◽  
pp. 1129-1135 ◽  
Author(s):  
Dayue Chen ◽  
Jianfeng Feng ◽  
Minping Qian

1976 ◽  
Vol 48 (3) ◽  
pp. 249-265 ◽  
Author(s):  
Richard A. Holley ◽  
Daniel W. Stroock

Fractals ◽  
1998 ◽  
Vol 06 (01) ◽  
pp. 81-86 ◽  
Author(s):  
Makoto Katori ◽  
Shinya Kizaki ◽  
Youichi Terui ◽  
Takuya Kubo

Importance of the influence of neighboring canopy gaps upon new gap creation has been clarified by the ecological study of a neotropical forest on Barro Colorado Island (BCI), Panama. A stochastic lattice model for the forest dynamics with interacting canopy gap expansion was introduced by Kubo et al. We give a theorem showing a condition that this model can be regarded as a stochastic Ising model, and that its stationary state is exactly given by a Gibbs state. Using this theorem, we obtain a Gibbs state which remarkably well approximates the real gap-size distribution in BCI.


2007 ◽  
Vol 129 (1) ◽  
pp. 121-149 ◽  
Author(s):  
Yu. Kondratiev ◽  
E. Zhizhina

2013 ◽  
Vol 15 (2) ◽  
pp. 339-386 ◽  
Author(s):  
Eyal Lubetzky ◽  
Fabio Martinelli ◽  
Allan Sly ◽  
Fabio-Lucio Toninelli

1998 ◽  
Vol 16 (1) ◽  
pp. 71-81 ◽  
Author(s):  
N. H. March ◽  
M. P. Tosi

Recent computer experiments on liquid Mg and Bi (and also on dense hydrogen) have focussed anew on issues involving static and dynamical structure in plasmas. In Mg and Bi, under normal liquid metal conditions, separation of core and valence electrons is valuable both for thermodynamics and in interpreting diffraction experiments. Mg is considered in some detail as a specific example where there is weak electron–ion interaction. Finally, dynamical structure is considered. After a brief summary relating back to the electron–electron pair correlation contribution in X-ray scattering, attention is next focussed on the (longitudinal) viscosity of alkali metals via the Kubo formula. This viscosity is shown to be dominated by ion–ion interactions. Nevertheless, an intimate relation at the melting point is exposed between shear viscosity, thermal conductivity, and electrical resistivity, the latter two transport coefficients being dominated by electrons.


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