Defect kinetics and dynamics of pattern coarsening in a two-dimensional smectic-A system

Two-dimensional simulations of the coarsening process of the isotropic/smectic-A phase transition are presented using a high-order Landau–de Gennes-type free energy model. Defect annihilation laws for smectic disclinations, elementary dislocations and total dislocation content are determined. The computed evolution of the orientational correlation length and disclination density is found to be in agreement with previous experimental observations showing that disclination interactions dominate the coarsening process. The mechanism of smectic disclination movement, limited by the absorption and emission of elementary dislocations, is found to be facilitated by curvature walls connecting interacting disclinations. At intermediate times in the coarsening process, split-core dislocation formation and interactions displaying an effective disclination quadrupole configuration are observed. This work provides the framework for further understanding of the formation and dynamics of the diverse set of curvature defects observed in smectic liquid crystals and other layered material systems.

[1]  H. Coles,et al.  The Order-Disorder Phase Transition in Liquid Crystals as a Function of Molecular Structure. I. The Alkyl Cyanobiphenyls , 1979 .

[2]  Oleg D. Lavrentovich,et al.  Soft Matter Physics: An Introduction , 2002 .

[3]  M. Calderer,et al.  Landau-de Gennes theory of isotropic-nematic-smectic liquid crystal transitions. , 2007, Physical review. E, Statistical, nonlinear, and soft matter physics.

[4]  E. Lacaze,et al.  Structure of smectic defect cores: x-ray study of 8CB liquid crystal ultrathin films. , 2005, Physical review letters.

[5]  H. Jagodzinski Points, lines and walls in liquid crystals, magnetic systems and various ordered media by M. Kléman , 1984 .

[6]  Jean-Claude Tolédano,et al.  The Landau theory of phase transitions : application to structural, incommensurate, magnetic, and liquid crystal systems , 1987 .

[7]  N. David Mermin,et al.  Points, Lines and Walls: In Liquid Crystals, Magnetic Systems and Various Ordered Media. , 1982 .

[8]  Wolfe,et al.  Evolution of disorder in two-dimensional stripe patterns: "Smectic" instabilities and disclination unbinding. , 1992, Physical review letters.

[9]  P. Mukherjee,et al.  Simple Landau model of the smectic- A-isotropic phase transition , 2001 .

[10]  W. H. Jeu,et al.  Shear-Induced Smectic Ordering as a Precursor of Crystallization in Isotactic Polypropylene , 2003 .

[11]  Interfacial nematodynamics of heterogeneous curved isotropic-nematic moving fronts. , 2006, The Journal of chemical physics.

[12]  L. Lejček Wedge disclinations as models of curvature walls in smectic A liquid crystals , 1990 .

[13]  P. Mather,et al.  Responsive materials: soft answers for hard problems. , 2007, Nature materials.

[14]  Entropy-induced smectic phases in rod-coil copolymers , 2002, cond-mat/0205569.

[15]  J. Friedel,et al.  Disclinations, dislocations and continuous defects: a reappraisal , 2007, 0704.3055.

[16]  C. Blanc,et al.  Dynamics of nematic liquid crystal disclinations: the role of the backflow. , 2005, Physical review letters.

[17]  Noel A. Clark,et al.  End-to-End Stacking and Liquid Crystal Condensation of 6– to 20–Base Pair DNA Duplexes , 2007, Science.

[18]  Hudson,et al.  Disclination interaction in an applied field: Stabilization of the Lehmann cluster. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[19]  A. Rey,et al.  Growth and structure of nematic spherulites under shallow thermal quenches , 2007 .

[20]  E. Thomas,et al.  Are domains in liquid crystalline polymers arrays of disclinations? , 1986, Nature.

[21]  D. Huse,et al.  Mechanisms of ordering in striped patterns. , 2000, Science.

[22]  C. Black Polymer self-assembly as a novel extension to optical lithography. , 2007, ACS nano.

[23]  L. M. Pismen Patterns and Interfaces in Dissipative Dynamics , 2009, Encyclopedia of Complexity and Systems Science.

[24]  Marcus Müller,et al.  Directed self-assembly of block copolymers for nanolithography: fabrication of isolated features and essential integrated circuit geometries. , 2007, ACS nano.

[25]  C. Blanc,et al.  The Curvature Walls in Lyotropic Lamellar Phases , 2000 .

[26]  Macroscopic dynamics near the isotropic-smectic-A phase transition. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.

[27]  D. A. Vega,et al.  Dynamics of pattern coarsening in a two-dimensional smectic system. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[28]  Denis Boyer,et al.  Grain boundary pinning and glassy dynamics in stripe phases. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[29]  Wolfe,et al.  Evolution of disorder in magnetic stripe domains. I. Transverse instabilities and disclination unbinding in lamellar patterns. , 1992, Physical review. A, Atomic, molecular, and optical physics.

[30]  Ricardo Ruiz,et al.  Induced Orientational Order in Symmetric Diblock Copolymer Thin Films , 2007 .

[31]  T. Kibble Phase-transition dynamics in the lab and the universe , 2007 .

[32]  Alan C. Newell,et al.  Natural patterns and wavelets , 1998 .

[33]  Luiz Roberto Evangelista,et al.  An Elementary Course on the Continuum Theory for Nematic Liquid Crystals , 2000 .

[34]  P. Pershan,et al.  Dislocation and impurity effects in smectic‐A liquid crystals , 1975 .

[35]  J. Rigden Eisenhower, scientists, and Sputnik , 2006 .

[36]  Phase ordering in nematic liquid crystals. , 2001, Physical review. E, Statistical, nonlinear, and soft matter physics.