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Bidimensional distortion in ferroelectric liquid crystals with strong anchoring in bookshelf geometry

机译:铁电液晶的二维畸变,在书架几何形状中具有强锚定性

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In the last decade, it has been experimentally found that in certain conditions a periodic domain pattern arises in ferroelectric liquid crystals (FLC) in bookshelf geometry. Such a periodic texture appears after switching-off an external electric ???eld, even in strong anchoring conditions. It has a static character and is bidimensional, being dependent on directions normal to both the smectic planes and the cell plates. Here a new model explaining this phenomenon is proposed, valid in the case of FLC with strong anchoring. The model is based on the coupling between the spontaneous polarization ???eld in the ???rst semi-period of its modulation along the cell plates and the same ???eld in the second semi-period. This coupling competes with the FLC medium elasticity and is trapped by the anchoring. According to our model, in the ferroelectric state the biperiodic texture is favored by increasing the values of spontaneous polarization. The critical value of the spontaneous polarization for which the undeformed state becomes unstable is found. It is shown to be proportional to the square root of the ratio between the FLC elastic constant and the cell thickness. Moreover, it is inversely proportional to the sinus of the pre-tilt angle with respect to the cell walls.
机译:在过去的十年中,已经通过实验发现,在某些条件下,书架几何形状的铁电液晶(FLC)中会出现周期性畴图案。即使在强锚固条件下,在切断外部电场后,仍会出现这种周期性纹理。它具有静态特征并且是二维的,取决于垂直于近晶平面和细胞板的方向。在这里,提出了一个解释这种现象的新模型,该模型在具有强锚定作用的FLC中有效。该模型基于其调制沿细胞板的第一个半周期的自发极化场与第二个半周期的相同极化场之间的耦合。这种耦合与FLC介质的弹性竞争,并被锚固捕获。根据我们的模型,在铁电状态下,通过增加自发极化值有利于双周期织构。发现未变形状态变得不稳定的自发极化的临界值。它显示为与FLC弹性常数和孔厚度之间的比率的平方根成比例。而且,它相对于单元壁与预倾斜角的正弦成反比。

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