Abstract

We investigated a periodic flexoelectric domain pattern, which appeared as regular parallel stripes in an achiral bent core nematic liquid crystal when dc electric field was applied. We found that such a pattern was first formed at the substrate surface and took place in sandwich cells with a gap larger than 2μm. The field-induced periodic pattern was preserved in the field-off state by a polymer network formed in the cell and was found to exhibit a polar as well as a linear electro-optic response due to in-plane switching of the sample optic axis. A comparison between this response and the one obtained in short cholesteric liquid crystals, aligned in ULH (uniform lying helix) texture, and short pitch ferroelectric liquid crystals, respectively, suggested that a heliconical molecular order is most probably formed in the field-induced periodic stripe pattern, with the helix axis orthogonal to the stripes. To our knowledge, this is the first experimental evidence of field-induced chiral-symmetry breaking in the flexoelectric periodic stripe pattern in achiral bent core nematic, resulting in heliconical molecular order, resembling the one of twist-bend (TB) nematic phase in this kind of nematics.

Highlights

  • Liquid crystal materials composed of bent core (BC) or so-called banana shape molecules were introduced more than two decades ago

  • In the current paper we present the results of our study on the periodic stripe pattern formation in a BC nematic subjected to a dc electric field

  • According to Ref. 24, the BC nematic material M1118, used in the present study, has negative dielectric anisotropy (∆ε

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Summary

Periodic pattern formation in an achiral bent core nematic

Omaima Elamain,[1] Gurumurthy Hegde,2,a and Lachezar Komitov1,a 1Department of Physics, University of Gothenburg, SE-412 96 Gothenburg, Sweden 2Centre for Nano-Materials and Displays, BMS College of Engineering, Bull Temple Road, Basavanagudi, 560019 Bangalore, India (Received 18 May 2018; accepted 5 September 2018; published online 28 September 2018)

INTRODUCTION
RESULTS AND DISCUSSION
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