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8
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85036248903
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D. R. Nelson, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, New York, 1983), Vol. 7
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D. R. Nelson, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, New York, 1983), Vol. 7.
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14
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0013262654
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Zh. Éksp. Teor. Fiz. 64, 672 (1973) [, SPHJAR
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V. N. Popov, Zh. Éksp. Teor. Fiz. 64, 672 (1973) [Sov. Phys. JETP 37, 341 (1973)].SPHJAR
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(1973)
Sov. Phys. JETP
, vol.37
, pp. 341
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Popov, V.N.1
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17
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36449006950
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The system of PHCs has been used recently as a model for the study of demixing in fluid mixtures. See , JCPSA6
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The system of PHCs has been used recently as a model for the study of demixing in fluid mixtures. See M. Dijkstra, D. Frenkel, and J. P. Hansen, J. Chem. Phys. 101, 3179 (1994); JCPSA6
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(1994)
J. Chem. Phys.
, vol.101
, pp. 3179
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Dijkstra, M.1
Frenkel, D.2
Hansen, J.P.3
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21
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85036341695
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the system of PHCs, molecular-orientational order, i.e., order in the orientation of the individual particles, always exists since all particles are parallel to each other by definition. Bond-orientational order refers to long-range correlations in the orientations of the segments joining the centers of neighbor particles. This is what is tested with the parameter [formula presented] (see the text). I will use simply “orientational order” to refer to “bond-orientational order.”
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In the system of PHCs, molecular-orientational order, i.e., order in the orientation of the individual particles, always exists since all particles are parallel to each other by definition. Bond-orientational order refers to long-range correlations in the orientations of the segments joining the centers of neighbor particles. This is what is tested with the parameter B2 (see the text). I will use simply “orientational order” to refer to “bond-orientational order.”
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22
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85036172777
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Simulations were also performed by fixing the volume of the system and calculating the equilibrium pressure (and thus [formula presented] along the simulations (the [formula presented] ensemble). The results are completely consistent with the ones presented here
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Simulations were also performed by fixing the volume of the system and calculating the equilibrium pressure (and thus T*) along the simulations (the NVT ensemble). The results are completely consistent with the ones presented here.
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23
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85036213688
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fact, the simple cubic structure of hard cubes has at low temperatures a shear modulus proportional to [formula presented] along the main crystalline directions [E. A. Jagla (unpublished)]
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In fact, the simple cubic structure of hard cubes has at low temperatures a shear modulus proportional to T* along the main crystalline directions [E. A. Jagla (unpublished)].
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24
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85036362808
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Strictly speaking, long-range orientational order alone generates values of [formula presented] that are different from zero. However, these values are much smaller than in the presence of long-range positional order. This justifies the use of [formula presented] as an indicator of long-range positional order
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Strictly speaking, long-range orientational order alone generates values of Bc that are different from zero. However, these values are much smaller than in the presence of long-range positional order. This justifies the use of Bc as an indicator of long-range positional order.
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28
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0004072342
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Cambridge University Press, Cambridge
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S. Chandrasekhar, Liquid Crystals (Cambridge University Press, Cambridge, 1977).
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(1977)
Liquid Crystals
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Chandrasekhar, S.1
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