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2
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4143082557
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A. P. Y. Wong, Ph.D. dissertation, Penn State University, 1990
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A. P. Y. Wong, S. B. Kim, W. I. Goldburg and M. H. W. Chan, Phys. Rev. Lett. 70, 954 (1993); A. P. Y. Wong, Ph.D. dissertation, Penn State University, 1990.
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4
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A. Maritan, M. R. Swift, M. Cieplak, M. H. W. Chan, M. W. Cole and J. R. Banavar, Phys. Rev. Lett. 67, 1821 (1991).
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5
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3543149184
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E. Pitard, M. L. Rosinberg, G. Stell and G. Tarjus, Phys. Rev. Lett. 74, 4361 (1995).
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Rosinberg, M.L.2
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9
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6944223628
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Falicov and Berker studied (Formula presented)He mixtures numerically in both fractal and periodic networks and found that the superfluid transition becomes detached from the phase-separation transition in both cases, in accord with experiments 10. Al-though the systems are different, their results support our use of a periodic gel network. See A. Falicov and A. N. Berker, Phys. Rev. Lett. 74, 426 (1995).
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Falicov, A.1
Berker, A.N.2
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11
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0343673900
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By replacing the hexagonal unit cell with a circular one, we have eliminated the possibility of ``bridging transitions, '' where bridges of high magnetization develop to connect strands. See W. R. Osborn and J. M. Yeomans, Phys. Rev. E 51, 2053 (1995).
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Phys. Rev. E
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Yeomans, J.M.2
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13
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85037207548
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This is a manifestation of capillary condensation, where the phase transition is shifted to a value of the bulk field (or chemical potential in the fluid case) that favors the nonwetting phase
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This is a manifestation of capillary condensation, where the phase transition is shifted to a value of the bulk field (or chemical potential in the fluid case) that favors the nonwetting phase.
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21
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4244062729
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for numerical estimates, see K. K. Mon, Phys. Rev. Lett. 60, 2749 (1988);
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24
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85037229783
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Note that both critical points have exponents Β=1/2 because our approximation only builds in nonclassical exponents at the bulk critical point
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Note that both critical points have exponents Β=1/2 because our approximation only builds in nonclassical exponents at the bulk critical point.
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25
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85037183104
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P. J. Upton, S.-Y. Zinn, and M. E. Fisher (private communication)
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P. J. Upton, S.-Y. Zinn, and M. E. Fisher (private communication).
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26
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85037206360
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(private communication)
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M. H. W. Chan (private communication).
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Chan, M.H.W.1
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27
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0000154360
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The disappearance of the double hump below a threshold value of the surface field is reminiscent of the behavior of the wetting transition on a single planar surface. See H. Nakanishi and M. E. Fisher, Phys. Rev. Lett. 49, 1565 (1982).
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Phys. Rev. Lett.
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Nakanishi, H.1
Fisher, M.E.2
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