1978
DOI: 10.1143/jjap.17.219
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Observation of Forming Process of Bubble Domain Texture in Liquid Crystals

Abstract: The forming process of bubble domains observed in a large pitch cholesteric is investigated under various circumstances. In this experiment the bubble domians of a negative dielectric anisotropy are formed by an application of an electric field below that required for dynamic scattering. The domains of a positive dielectric one are formed by applying thermal turbulence. It is found that the bubble domains are formed through the inherent or field-induced striped texture. The change from stripe to bubble and the… Show more

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Cited by 26 publications
(14 citation statements)
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“…11 The helical structure of cholesteric LCs (CLCs) does not readily accommodate many confinement geometries. When CLCs are confined in slit cells with the cell gap close to cholesteric pitch, bubble domain defects are often observed under thermal quenching, 12 external electric field, [13][14][15][16][17][18] or illuminations of focused laser beams. [19][20][21][22][23] By microscopically reconstructing the director fields, Smalyukh and coworkers showed that the bubble domain defects are made of either torons or baby Skyrmions (2D Skyrmions).…”
Section: Introductionmentioning
confidence: 99%
“…11 The helical structure of cholesteric LCs (CLCs) does not readily accommodate many confinement geometries. When CLCs are confined in slit cells with the cell gap close to cholesteric pitch, bubble domain defects are often observed under thermal quenching, 12 external electric field, [13][14][15][16][17][18] or illuminations of focused laser beams. [19][20][21][22][23] By microscopically reconstructing the director fields, Smalyukh and coworkers showed that the bubble domain defects are made of either torons or baby Skyrmions (2D Skyrmions).…”
Section: Introductionmentioning
confidence: 99%
“…We have found that some of the studied laser-generated structures can also be obtained spontaneously when cooling the samples from the isotropic phase (although less reliably and without the control of spatial locations) and after applying low-frequency (10 Hz) electric fields to induce hydrodynamic instability. These localized structures, along with torons and hopfions, are several members of the large family of so-called cholesteric bubbles that were typically studied when occurring spontaneously, but not well understood in past experimental works [20,[34][35][36][37][38][39][40][41][42][43][44]. We note that the study of axially symmetric cholesteric configurations reported here is not exhaustive.…”
Section: Nested Axially Symmetric Structures Of Multiple Torons Anmentioning
confidence: 86%
“…We note that the study of axially symmetric cholesteric configurations reported here is not exhaustive. In fact, several other configurations might have been already identified in prior literature [20,[23][24][25][26][34][35][36][37][38][39][40][41][42][43][44][45][46][47][48] that we have not explored so far using our 3D imaging experiments and different types of generation (laser realignment, low-frequency electric field, temperature quench with and without temperature gradients). In addition, in future work, studies of mutually linked multi-toron and multihopfion configurations that also belong to this family will be reported [51].…”
Section: Nested Axially Symmetric Structures Of Multiple Torons Anmentioning
confidence: 99%
“…in CLC systems effectively, it becomes feasible to create stable/metastable structures with 3D inhomogeneous configuration of the LC director field. One example of such structures that can be interesting and promising from the point of view of practical application in optics is the so‐called cholesteric “bubbles” or bubble domain (BD) texture . This texture is usually observed for d / P in the vicinity of 1 and represents a self‐assembled single layer of uniformly sized bubbles embedded in the medium with uniform homeotropic orientation.…”
Section: Diffraction Structures In Clc Materials Induced By Electric mentioning
confidence: 99%