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J. Chem. Phys. 127, 074709 (2007); http://dx.doi.org/10.1063/1.2752505 (11 pages)

Phase field theory of interfaces and crystal nucleation in a eutectic system of fcc structure: I. Transitions in the one-phase liquid region

Gyula I. Tóth1 and László Gránásy2

1Research Institute for Solid State Physics and Optics, P.O. Box 49, H-1525 Budapest, Hungary
2Brunel Centre for Advanced Solidification Technology, Brunel University, Uxbridge, Middlesex UB8 3PH, United Kingdom and Research Institute for Solid State Physics and Optics, P.O. Box 49, H-1525 Budapest, Hungary

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(Received 8 September 2006; accepted 1 June 2007; published online 21 August 2007)

The phase field theory (PFT) has been applied to predict equilibrium interfacial properties and nucleation barrier in the binary eutectic system Ag–Cu using double well and interpolation functions deduced from a Ginzburg-Landau expansion that considers fcc (face centered cubic) crystal symmetries. The temperature and composition dependent free energies of the liquid and solid phases are taken from CALculation of PHAse Diagrams-type calculations. The model parameters of PFT are fixed so as to recover an interface thickness of ∼ 1 nm from molecular dynamics simulations and the interfacial free energies from the experimental dihedral angles available for the pure components. A nontrivial temperature and composition dependence for the equilibrium interfacial free energy is observed. Mapping the possible nucleation pathways, we find that the Ag and Cu rich critical fluctuations compete against each other in the neighborhood of the eutectic composition. The Tolman length is positive and shows a maximum as a function of undercooling. The PFT predictions for the critical undercooling are found to be consistent with experimental results. These results support the view that heterogeneous nucleation took place in the undercooling experiments available at present. We also present calculations using the classical droplet model [classical nucleation theory (CNT)] and a phenomenological diffuse interface theory (DIT). While the predictions of the CNT with a purely entropic interfacial free energy underestimate the critical undercooling, the DIT results appear to be in a reasonable agreement with the PFT predictions.

© 2007 American Institute of Physics

Article Outline

  1. INTRODUCTION
  2. APPLIED MODELS
    1. Phase field theory (PFT)
      1. Specific double well and interpolation functions
        1. The “standard” set (PFT/S)
        2. Ginzburg-Landau form for fcc structure (PFT/GL)
      2. Equilibrium interfaces
        1. Solid-liquid interfaces
        2. Solid-solid interfaces
      3. Barrier for crystal nucleation
      4. Tolman length
    2. Classical nucleation theory (CNT)
    3. Diffuse interface theory (DIT)
    4. Steady state nucleation rate
  3. PHYSICAL PROPERTIES
  4. RESULTS AND DISCUSSION
    1. Equilibrium interfaces
      1. Solid-liquid interfaces
      2. Solid-solid interfaces
    2. Crystal nuclei
      1. Nucleation in PFT with GL free energy
      2. Comparison with other models
  5. SUMMARY

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KEYWORDS and PACS

PACS

  • 64.60.Q-

    Nucleation

  • 64.70.D-

    Solid-liquid transitions

  • 68.08.-p

    Liquid-solid interfaces

  • 68.35.Md

    Surface thermodynamics, surface energies

  • 61.50.Ah

    Theory of crystal structure, crystal symmetry; calculations and modeling

ARTICLE DATA

PUBLICATION DATA

ISSN

0021-9606 (print)  
1089-7690 (online)

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    References

    (a) P. Harrowell and D. W. Oxtoby, J. Chem. Phys. 80, 1639 (1984)JCPSA6000080000004001639000001;, (b) Y. C. Shen and D. W. Oxtoby, ibid. 105, 6517 (1996)JCPSA6000105000015006517000001;, (c) L. Gránásy and T. Pusztai, ibid. 117, 10121 (2002)JCPSA6000117000022010121000001.

    For example, see D. W. Oxtoby and A. D. J. Haymet, J. Chem. Phys. 76, 6262 (1982)JCPSA6000076000012006262000001;, W. E. McMullen and D. W. Oxtoby, ibid. 88, 1967 (1988)JCPSA6000088000003001967000001;, W. A. Curtin, Phys. Rev. Lett. 59, 1228 (1987)
    Phys. Rev. B 39, 6775 (1989)
    N. Choudry and S. K. Gosh, Phys. Rev. E 57, 1939 (1998).

    J. Bechhoefer, H. Löwen, and L. S. Tuckerman, Phys. Rev. Lett. 67, 1266 (1991)
    L. Gránásy and D. W. Oxtoby, J. Chem. Phys. 112, 2410 (2000)JCPSA6000112000005002410000001.

    M. Asta, J. J. Hoyt, and A. Karma, Phys. Rev. B 66, 100101(R) (2002).

    J. W. Cahn and J. E. Hilliard, J. Chem. Phys. 28, 258 (1958)JCPSA6000028000002000258000001.

    B. B. Laird, J. Chem. Phys. 115, 2887 (2001)JCPSA6000115000007002887000001.

    J. W. Cahn and J. E. Hilliard, J. Chem. Phys. 31, 688 (1959)JCPSA6000031000003000688000001.

    R. C. Tolman, J. Chem. Phys. 17, 333 (1949)JCPSA6000017000003000333000001.

    L. Gránásy, J. Chem. Phys. 104, 5188 (1996)JCPSA6000104000013005188000001;, R. McGraw and A. Laaksonen, Phys. Rev. Lett. 76, 2754 (1996).

    R. S. Aga, J. R. Morris, J. J. Hoyt, and M. Mendelev, Phys. Rev. Lett. 96, 245701 (2006).

    P. R. ten Wolde, M. J. Kuiz-Montero, and D. Frenkel, J. Chem. Phys. 104, 9932 (1996)JCPSA6000104000024009932000001.

    D. Y. Sun, M. Asta, and J. J. Hoyt, Phys. Rev. B 69, 174103 (2004).

    Y. C. Shen and D. W. Oxtoby, J. Chem. Phys. 104, 4233 (1996)JCPSA6000104000011004233000001;, 105, 2130 (1996)JCPSA6000105000005002130000001.

    S. Walder and P. L. Ryder, J. Appl. Phys. 74, 6100 (1993)JAPIAU000074000010006100000001.

    G. I. Tóth and L. Gránásy, J. Chem. Phys. 127, 074710 (2007)JCPSA6000127000007074710000001.


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