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Gunton, J.D.1
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5
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0042937034
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note
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The exponent 1/3 is probably the result of friction of the fluid with the confining parallel plates which leads to an overdamping of the velocity field.
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13
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0035934131
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F. Qiu, G. Peng, V. V. Ginzburg, A. C. Balazs, H.-Y. Chen, and D. Jasnow, J. Chem. Phys. 115, 3779 (2001).
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14
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0037041806
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D. Suppa, O. Kuksenok, A. C. Balazs, and J. M. Yeomans, J. Chem. Phys. 116, 6305 (2002).
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0001190885
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V. V. Ginzburg, F. Qiu, M. Paniconi, G. Peng, D. Jasnow, and A. C. Balazs, Phys. Rev. Lett. 82, 4026 (1999).
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0035997661
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V. V. Ginzburg, C. Gibbons, F. Qiu, G. Peng, and A. C. Balazs, Macromolecules 33, 6140 (2000).
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21
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A. C. Balazs, V. V. Ginzburg, F. Qiu, G. Pend, and D. Jasnow, J. Phys. Chem. B 104, 3411 (2000).
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26
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0042436346
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note
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Due to the very steep repulsive part of the Lennard-Jones potential, the filler particles are effectively hard particles.
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28
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0001575696
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M. Laradji, O. G. Mouritsen, S. Toxvaerd, and M. J. Zuckermann, Phys. Rev. E 50, 1243 (1994).
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33
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0041433934
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note
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The considered density and temperature assures that the system is safely within in the coexistence region of the A-rich and B-rich fluid phases in the case of a pure binary mixture. The addition of C-particles is expected to change the phase behavior. The phase diagram of the system is currently being evaluated by us.
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34
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0041433933
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note
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The majority of the simulations were performed on Sun Ultra-80 workstations, and the total computer time was about 3360 h.
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35
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0042937030
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note
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B-particle local density was considered for the calculation of the structure factor in order to avoid interference between the average domain size and the next smaller length scale corresponding to the radius of a C-particle.
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39
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0000145947
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0000979359
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M. Laradji, H. Guo, M. Grant, and M. J. Zuckermann, J. Phys. A 24, L629 (1991).
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Laradji, M.1
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43
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0041433932
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(unpublished)
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M. Laradji (unpublished).
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Laradji, M.1
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47
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0000447296
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J. H. Yao, K. R. Elder, H. Guo, and M. Grant, Phys. Rev. B 47, 14110 (1993).
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