Soft elasticity in biaxial smectic and smectic-C elastomers
Olaf Stenull, T. C. Lubensky

TL;DR
This paper investigates the elastic properties of biaxial smectic elastomers and smectic-C elastomers, revealing their soft elasticity due to spontaneous symmetry breaking through theoretical models.
Contribution
It introduces three related models to analyze the elasticity and phase transitions of biaxial and smectic-C elastomers, highlighting the origin of soft elasticity.
Findings
Emergent phases exhibit soft elasticity with vanishing elastic moduli.
Spontaneous symmetry breaking is key to the softness phenomena.
Different manifestations include absence of restoring forces under specific strains.
Abstract
Ideal (monodomain) smectic- elastomers crosslinked in the smectic- phase are simply uniaxial rubbers, provided deformations are small. From these materials smectic- elastomers are produced by a cooling through the smectic- to smectic- phase transition. At least in principle, biaxial smectic elastomers could also be produced via cooling from the smectic- to a biaxial smectic phase. These phase transitions, respectively from to and from to symmetry, spontaneously break the rotational symmetry in the smectic planes. We study the above transitions and the elasticity of the smectic- and biaxial phases in three different but related models: Landau-like phenomenological models as functions of the Cauchy--Saint-Laurent strain tensor for both the biaxial and the smectic- phases and a detailed model, including contributions…
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