5 [15] P. Laguna and W. H. Zurek, Phys. Rev. Lett. 78 , 25 19 (1997); Phys. Rev. D 58 , 5021 (1998). [16] A. Yates and W. H. Zurek, Phys. Rev. Lett. 80 , 5477 (1998). [17] N. D. Antunes, L. M. A. Bettencourt, W. H. Zurek, Phys. Rev. Lett. 82 , 2824 (1999). [18] G. J. Stephens, E. A. Calzetta, B. L. Hu, and S. A. Ram- sey, Phys. Rev. D 59 , 045009 (1999). [19] S. Suzuki, Cooling dynamics of pure and random Ising chains , arXiv:0807.2933. [20] M. E. Dodd, P. C. Henrym N. S. Lawson, P. V. E. Mc- Clintock, and C. D. H. Williams, Phys. Rev. Lett. 81 , 3703 (1998). [21] V. M. H. Ruutu, V. B. Eltsov, A. J. Gill, T. W. B. Kibble, M. Krusius, Y. G. Makhlin, B. Placais, G. E. Volovik, W. Xu, Nature 382 , 334 (1996). C. B¨ auerle, Y. M. Bunkov, S. N. Fisher, H. Godfrin, G. R. Pickett, Nature 382 , 332 (1996). The Grenoble cosmological experiment: the Kibble-Zurek scenario in superfluid $^{3}$He , C. Bauerle, Yu. M. Bunkov, S. Fisher, and H. Godfrin, in Topological defects and the non-equilibrium dynamcis of symmetry breaking phase transitions, Vol 549, Y. M. Bunkov and H. Godfrin eds. (Kluwer Academic Publishers, 1999). [22] T. Kibble, Physics Today, 60 , No. 9, 47 (2007). [23] J. R. Kirtley and F. Tafuri, Physics 2 , 92 (2009). [24] R. Monaco, J. Mygind, R. J. Rivers and V. P. Koshelets, Phys. Rev. B, 80 , 180501 (2009). [25] Some cases in which the dynamic scaling hypothesis fails due to more than one growing length exist [1]. [26] H. K. Janssen, B. Schaub, and B. Schmittmann, Z. Phys. B 73 , 539 (1989). B. Schmittmann and R. K. P. Zia in Phase transitions and critical phenomena C. Domb and J. L. Lebowitz Vol. 17 (Academic Press, N. Y.) 1995. [27] P. Calabrese and A. Gambassi, J. Phys. A 38 , R133 (2005). U. C. Tauber Lecture Notes in Physics 716 , 295 (2007). [28] A. Sicilia, J. J. Arenzon, A. J. Bray, and L. F. Cuglan- dolo, Phys. Rev. E 76 , 061116 (2007). [29] H.-C. Chu and G. A. Williams Phys. Rev. Lett. 86 , 2585 (2001). [30] P. Krapivsky, arXiv:cond-mat (2010).