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For colloid-polymer mixtures, the presence or absence of the liquid minimum depends on both the size (ξ, relative to a colloidal sphere) and activity of the polymer (ILETT S. M., ORROCK A., POON W. C. K. and PUSEY P. N., Phys. Rev. E, 51 (1995) 1344). Translating the latter into an effective temperature, one finds (for high ξ) a conventional (gas/liquid/solid) phase diagram or (for low ξ) one in which the liquid phase is absent. Reference [8] concerns the latter case, for which the liquid-gas binodal curve is entirely hidden within the gas-solid coexistence region.
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Contrast this with the truly steady motion possible in pure systems with molecular (rather than dissipative) dynamics, where density changes can relax by propagating modes. See OXTOBY D. W. and HARROWELL P. R., J. Chem. Phys., 96 (1992) 3834.
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