2012
DOI: 10.1007/12_2011_165
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Liquid Crystal Elastomers and Light

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Cited by 20 publications
(18 citation statements)
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“…[11][12][13][14] If a CLC is polymerized into an elastomer (CLCE), a very interesting material arises, combining the striking optical properties of a cholesteric phase with the viscoelasticity of a rubber. [15,16] Because of the coupling between the cholesteric helix and the elastomeric network, a mechanical deformation changes the reflection color and often also the polarization. [17] A striking demonstration was the continuous and reversi ble tuning toward shorter wavelengths of a CLCE film with vertical helix by stretching biaxially in the film plane, equivalent to a uniaxial compression along the helix.…”
Section: Introductionmentioning
confidence: 99%
“…[11][12][13][14] If a CLC is polymerized into an elastomer (CLCE), a very interesting material arises, combining the striking optical properties of a cholesteric phase with the viscoelasticity of a rubber. [15,16] Because of the coupling between the cholesteric helix and the elastomeric network, a mechanical deformation changes the reflection color and often also the polarization. [17] A striking demonstration was the continuous and reversi ble tuning toward shorter wavelengths of a CLCE film with vertical helix by stretching biaxially in the film plane, equivalent to a uniaxial compression along the helix.…”
Section: Introductionmentioning
confidence: 99%
“…[18][19][20][21] Since then, much effort has been made to improve the performance of photomobile polymer materials. [22][23][24][25][26][27][28][29][30][31][32] In this Minireview, we focus on CLCPs that macroscopically deform upon irradiation with actinic light. First, we introduce typical examples of photomobile polymer materials and their working mechanisms.…”
Section: Introductionmentioning
confidence: 99%
“…f B is as in (17) and ǫ > 0 is a small positive parameter. We can obtain an explicit upper bound for the norm of a global energy minimizer using a maximum principle approach as shown below.…”
Section: Discussionmentioning
confidence: 99%
“…Let Q * be a global minimizer of F ǫ in the admissible space A in (14). Then |Q * | ≤ max 1 √ 6 , bǫ 2 √ 6(8 + 2ǫ 2 c) + 64 + 16ǫ 2 (c − 6a) + ǫ 4 (b 2 − 24ac) √ 6(8 + 2ǫ 2 c) , max r∈∂Ω |Q 0 | onΩ (87) where a, b, c are the bulk constants in f B in (17).…”
Section: Discussionmentioning
confidence: 99%