Dynamics of a faceted nematic-smectic B front in thin-sample directional solidification

Details Dynamics of a faceted nematic-smectic B front in thin-sample directional solidification Dynamics of a faceted nematic-smectic B front in thin-sample directional solidification

2001-09-07

arxiv.org/abs/cond-mat/0109148v1

Physics

Condensed Matter

Soft Condensed Matter

12 pages, 19 figures, submitted to Phys. Rev. E

Scientific paper

We present an experimental study of the directional-solidification patterns of a nematic - smectic B front. The chosen system is C_4H_9-(C_6H_{10})_2CN (in short, CCH4) in 12 \mu m-thick samples, and in the planar configuration (director parallel to the plane of the sample). The nematic - smectic B interface presents a facet in one direction -- the direction parallel to the smectic layers -- and is otherwise rough, and devoid of forbidden directions. We measure the Mullins-Sekerka instability threshold and establish the morphology diagram of the system as a function of the solidification rate V and the angle theta_{0} between the facet and the isotherms. We focus on the phenomena occurring immediately above the instability threshold when theta_{0} is neither very small nor close to 90^{o}. Under these conditions we observe drifting shallow cells and a new type of solitary wave, called "faceton", which consists essentially of an isolated macroscopic facet traveling laterally at such a velocity that its growth rate with respect to the liquid is small. Facetons may propagate either in a stationary, or an oscillatory way. The detailed study of their dynamics casts light on the microscopic growth mechanisms of the facets in this system.

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