A full study of parity-broken states in the directional solidification of lamellar eutectics is performed within the boundary-integral formulation. Symmetric states cease to exist at a wavelength {λ}, which is approximately twice that corresponding to their minimum undercooling, whereas solutions with a broken parity, drifting transversely to the growth front, appear as a forward bifurcation. Our results suggest that if one effectively doubles the wavelength of the initially symmetric state---a situation that can be achieved via a sudden jump of the velocity V by a factor of about 4, since λ²V{}const---then tilted lamellae should appear as extended states and not as ``solitons.'' We find here that parity-broken states exist for hypereutectic as well as for hypoeutectic and eutectic compositions. We have extended the derivation of the similarity equation derived previously [K. Kassner and C. Misbah, Phys. Rev. Lett. 66, 445 (1991)] to the present situation. This case involves additional subtleties, due to the loss of reflection symmetry about the growth axis. Among other results, we find that the tilt angle {φ} should depend on {σ}=d₀l/λ² and {χ}=l/lT only, where d₀, l, and lT are the capillary, diffusion, and thermal lengths, respectively, and {λ} is the wavelength of the pattern. At large enough growth velocities V, {φ}{}{φ}({σ}), while at small V the dependence on {χ} is strong. These predictions can be tested experimentally.
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Kassner et al. (1991) studied this question.
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