On Phase Ordering Behind the Propagating Front of a Second-Order Transition

Details On Phase Ordering Behind the Propagating Front of a Second-Order Transition On Phase Ordering Behind the Propagating Front of a Second-Order Transition

1996-12-09

arxiv.org/abs/cond-mat/9612075v1

JETP Lett. 65 (1997) 102-107; Pisma Zh.Eksp.Teor.Fiz. 65 (1997) 96-101

Physics

Condensed Matter

LaTeX file, 9 pages, no figures, submitted to JETP Lett

Scientific paper

10.1134/1.567332

In a real system the heating is nonuniform and a second-order phase transition into a broken symmetry phase occurs by propagation of the temperature front. Two parameters, the cooling rate $\tau_Q$ and the velocity $v_T$ of the transition front, determine the nucleation of topological defects. Depending on the relation of these parameters two regimes are found: in the regime of fast propagation defects are created according to the Zurek scenario for the homogeneous case, while in the slow propagation regime vortex formation is suppressed.

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