Abstract
We study theoretically the smectic- to - phase transition in isotropic disordered environments. Surprisingly, we find that, as in the clean smectic- to - phase transition, smectic layer fluctuations do not affect the nature of the transition, in spite of the fact that they are much stronger in the presence of the disorder. As a result, we find that the universality class of the transition is that of the “random field model” ().
- Received 12 June 2012
DOI:https://doi.org/10.1103/PhysRevE.87.042501
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