(S1) Rotation equation: 𝛾#-4(2)-2+𝛽(𝜓(𝑡))-.$(0,2)-0=𝑃𝐸(𝑡)𝑐𝑜𝑠𝜓(𝑡)=Γ(𝑡) (S2) where 𝛿(𝜓)= 𝛼#𝑠𝑖𝑛$𝜓𝑐𝑜𝑠$𝜓+#$[𝛾$𝑐𝑜𝑠2𝜓+𝛼'+𝛼%+𝛼&] (S3) 𝛽(𝜓)=−#$[𝛾$𝑐𝑜𝑠2𝜓+𝛾#]

Coupling of orientation, shear flow, applied torque, shear stress [14,15]: Shear flow equation: 𝛿(𝜓(𝑡))- · 1975 · arXiv 2110.1082

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An active hydroelastic liquid crystal phase of a fluttering ferroelectric nematic

cond-mat.soft · 2024-12-26 · conditional · novelty 7.0

AC-driven ferroelectric nematic liquid crystals enter a dissipative active state whose textures minimize viscous drag, favoring director splay and polarization normal to interfaces.

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An active hydroelastic liquid crystal phase of a fluttering ferroelectric nematic cond-mat.soft · 2024-12-26 · conditional · none · ref 3
AC-driven ferroelectric nematic liquid crystals enter a dissipative active state whose textures minimize viscous drag, favoring director splay and polarization normal to interfaces.

(S1) Rotation equation: 𝛾#-4(2)-2+𝛽(𝜓(𝑡))-.$(0,2)-0=𝑃𝐸(𝑡)𝑐𝑜𝑠𝜓(𝑡)=Γ(𝑡) (S2) where 𝛿(𝜓)= 𝛼#𝑠𝑖𝑛$𝜓𝑐𝑜𝑠$𝜓+#$[𝛾$𝑐𝑜𝑠2𝜓+𝛼'+𝛼%+𝛼&] (S3) 𝛽(𝜓)=−#$[𝛾$𝑐𝑜𝑠2𝜓+𝛾#]

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