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Volumn 38, Issue 8, 1997, Pages 595-600

Role of metastable states in phase ordering dynamics

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EID: 0031161068     PISSN: 02955075     EISSN: None     Source Type: Journal    
DOI: 10.1209/epl/i1997-00289-y     Document Type: Article
Times cited : (60)

References (23)
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    • For colloids and similar soft condensed systems, heat diffusion can be neglected since the entropy is dominated by solvent degrees of freedom. See LÖWEN H., Phys. Rep., 237 (1994) 249.
    • (1994) Phys. Rep. , vol.237 , pp. 249
    • Löwen, H.1
  • 10
    • 0005368652 scopus 로고
    • BECHHOEFER J., LÖWEN H. and TUCKERMAN L. S., Phys. Rev. Lett., 67 (1991) 1266; CELESTINI F. and TEN BOSCH A., Phys. Rev. E, 50 (1994) 1836; TUCKERMAN L. S. and BECHHOEFER J., Phys. Rev. A, 46 (1992) 3178.
    • (1991) Phys. Rev. Lett. , vol.67 , pp. 1266
    • Bechhoefer, J.1    Löwen, H.2    Tuckerman, L.S.3
  • 11
    • 0004712051 scopus 로고
    • BECHHOEFER J., LÖWEN H. and TUCKERMAN L. S., Phys. Rev. Lett., 67 (1991) 1266; CELESTINI F. and TEN BOSCH A., Phys. Rev. E, 50 (1994) 1836; TUCKERMAN L. S. and BECHHOEFER J., Phys. Rev. A, 46 (1992) 3178.
    • (1994) Phys. Rev. E , vol.50 , pp. 1836
    • Celestini, F.1    Ten Bosch, A.2
  • 12
    • 0040101420 scopus 로고
    • BECHHOEFER J., LÖWEN H. and TUCKERMAN L. S., Phys. Rev. Lett., 67 (1991) 1266; CELESTINI F. and TEN BOSCH A., Phys. Rev. E, 50 (1994) 1836; TUCKERMAN L. S. and BECHHOEFER J., Phys. Rev. A, 46 (1992) 3178.
    • (1992) Phys. Rev. A , vol.46 , pp. 3178
    • Tuckerman, L.S.1    Bechhoefer, J.2
  • 13
    • 33646068673 scopus 로고
    • 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.
    • (1995) Phys. Rev. E , vol.51 , pp. 1344
    • Ilett, S.M.1    Orrock, A.2    Poon, W.C.K.3    Pusey, P.N.4
  • 14
    • 0040101418 scopus 로고    scopus 로고
    • 2 (both isotropic) and N (nematic)
    • 2 (both isotropic) and N (nematic).
  • 15
    • 0038917060 scopus 로고    scopus 로고
    • cond-mat/9701138 preprint
    • EVANS R. M. L. and CATES M. E., cond-mat/9701138 preprint (1997).
    • (1997)
    • Evans, R.M.L.1    Cates, M.E.2
  • 16
    • 0040101419 scopus 로고    scopus 로고
    • cond-mat/9701139 preprint
    • EVANS R. M. L. and POON W. C. K., cond-mat/9701139 preprint (1997).
    • (1997)
    • Evans, R.M.L.1    Poon, W.C.K.2
  • 17
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    • edited by C. GODRÈCHE (Cambridge University Press) Chapt. 3
    • LANGER J. S., in Solids Far from Equilibrium, edited by C. GODRÈCHE (Cambridge University Press) 1995, Chapt. 3.
    • (1995) Solids Far from Equilibrium
    • Langer, J.S.1
  • 21
    • 36449004757 scopus 로고
    • 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.
    • (1992) J. Chem. Phys. , vol.96 , pp. 3834
    • Oxtoby, D.W.1    Harrowell, P.R.2
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    • A
    • A.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.