ライフサイエンスコーパス: liquid crystal

1 lasticity at the interface of beads with the liquid crystal.

2 e, and the bulk elasticity of the underlying liquid crystal.

3 ing the overlap between plasmonic fields and liquid crystal.

4 e colloidal particles dispersed in a nematic liquid crystal.

5 es living swimming bacteria with a lyotropic liquid crystal.

6 r stabilized uniform lying helix cholesteric liquid crystal.

7 ng a fictitious closed loop taken inside the liquid crystal.

8 c in contact with a hydrophobic thermotropic liquid crystal.

9 imensional orientation fields in cholesteric liquid crystals.

10 an drive uniform motion of baby skyrmions in liquid crystals.

11 r a potentially rich assortment of lyotropic liquid crystals.

12 as yet unexplored regime of highly confined liquid crystals.

13 an unexplored area of research for colloidal liquid crystals.

14 ion algorithm are mirrored in the physics of liquid crystals.

15 t to drive their rapid assembly into viscous liquid crystals.

16 liquids and polymers to plastic crystals and liquid crystals.

17 dered systems, such as porous frameworks and liquid crystals.

18 ic method for the production of thermotropic liquid crystals.

19 nal colloidal platelets in layers of nematic liquid crystals.

20 cts in molecular orientation widely found in liquid crystals.

21 terpart which can be realized as a defect in liquid crystals.

22 cus on soft materials, particularly gels and liquid crystals.

23 for controlled deformation and patterning of liquid crystals.

24 by modeling the membrane particles as chiral liquid crystals.

25 nment without translational order in nematic liquid crystals.

26 We use the liquid crystal 8CB and introduce an innovative dynamic f

27 ormed by polymer microspheres dispersed in a liquid crystal, a nematic fluid of orientationally order

28 Meta-liquid crystals, a novel form of tunable 3D metamaterial

29 nations in a lyotropic colloidal cholesteric liquid crystal: a continuous helicoidal thread and a per

30 ith exchangeable links, xLCEs develop strong liquid-crystal alignment as an alternative mechanism of

31 A novel polymer-layer-free system for liquid-crystal alignment is demonstrated by various shap

32 ue to splay and bend deformations of nematic liquid crystal along oblique electric fields, so that th

33 The amorphous blue phase III of cholesteric liquid crystals, also known as the "blue fog," are among

34 ings may be realized in systems ranging from liquid crystal and colloidal experiments to tabletop rea

35 low molecular weight liquids and polymers to liquid crystal and plastic crystals.

36 We realize skyrmions in a chiral liquid crystal and, using numerical modeling and polariz

37 h as twist grain boundary and blue phases in liquid crystals and Abrikosov phases in superconductors,

38 excitations that also appear in superfluids, liquid crystals and Bose-Einstein condensates.

39 nclude phase-transition materials, graphene, liquid crystals and carrier-modulated semiconductors, wh

40 ized xenon-129 (hp-(129)Xe) in media such as liquid crystals and cell suspensions are in demand for a

41 the reorientational nonlinearity of nematic liquid crystals and imposing a linear variation of the b

42 for the first time 1) ionic, halogen-bonded liquid crystals, and 2) imidazolium-based ionic liquid c

43 equilibrium systems: two-dimensional smectic liquid crystals, and a peculiar kind of constrained two-

44 of anisotropic shapes into complex crystals, liquid crystals, and even quasicrystals was demonstrated

45 cosmology, particle physics, superfluidity, liquid crystals, and metallurgy.

46 superconductivity, superfluidity, magnetism, liquid crystals, and plasticity of solids.

47 the combined supramolecular H-bond/columnar liquid crystal approach, yielded donor/acceptor coaxial

48 Liquid crystals are aligned along the ITO line pattern a

49 When liquid crystals are confined to finite volumes, the comp

50 duced helical superstructures of cholesteric liquid crystals are highlighted.

51 Chiral nematic liquid crystals are known to form blue phases-liquid sta

52 rticles adsorbed at the interface of nematic liquid crystals are known to form ordered structures who

53 The available detergent-compatible liquid crystals are negatively charged, thus offering ef

54 Liquid crystals are the basis of a pervasive technology

55 Liquid crystals are widely used in displays for portable

56 ds our ability to use topological defects in liquid crystals as templates for the organization of nan

57 ionary phase is prepared by surface-directed liquid crystal assembly.

58 The antibiotic squalamine forms a lyotropic liquid crystal at very low concentrations in water (0.3-

59 The study of liquid crystals at equilibrium has led to fundamental in

60 only an overview of the state of the art in liquid crystals based sensing scheme but also highlight

61 ge the gap between science and technology of liquid crystals based sensing scheme.

62 uid crystals organization forms the basis of Liquid-crystals based sensing scheme which has been expl

63 Liquid-crystal blue phases (BPs) are highly ordered at t

64 ination lines, reminiscent of those found in liquid-crystal blue phases.

65 ional photonic-crystalline properties called liquid-crystal blue phases.

66 that photosensitive azo-dye doped Blue-phase liquid crystals (BPLC) formed by natural molecular self-

67 Cubosomes formed from blue phase liquid crystals (BPs) dispersed in aqueous media exhibit

68 Colloidal particles dispersed in liquid crystals can form new materials with tunable elas

69 Colloidal dispersions in liquid crystals can serve as a soft-matter toolkit for t

70 nuniform director, (ii) local melting of the liquid crystal caused by the bacteria-produced shear flo

71 oelectric effect in in-plane switching (IPS) liquid crystal cell.

72 clination lines can be stably formed in thin liquid crystal cells by means of a judicious combination

73 erse droplets of one-dimensional cholesteric liquid crystal (CLC) containing a photosensitive chiral

74 A cholesteric liquid crystal (CLC) formed by chiral molecules represen

75 tructure, i.e., thermoresponsive cholesteric liquid crystal (CLC), by integrating a judiciously chose

76 exture torons in a thin layer of cholesteric liquid crystal (CLC), frustrated by homeotropic anchorin

77 nomenon is particularly noticeable in chiral liquid crystals (CLCs) due to the combined effect of the

78 ystals--otherwise referred to as cholesteric liquid crystals (CLCs)--are self-organized helical super

79 ls, this self-assembly is similar to that of liquid crystal colloids and originates from long-range e

80 and true self-assembly mechanisms in nematic liquid crystal colloids rely on specific interactions be

81 hirality in defining the mesoscopic order of liquid crystal colloids, suggesting that this feature ma

82 l for predicting the response time of cation-liquid crystal combinations.

83 inclusions into a moderately chiral nematic liquid crystal confined to a homeotropic cell creates lo

84 ally for partially ordered materials such as liquid crystals, confined liquids, and disordered crysta

85 Bacteria recognize subtle differences in liquid crystal deformations, engaging in bipolar swimmin

86 ng the light beam emerging from a q-plate, a liquid crystal device that modifies the polarization of

87 a high-transmission in-plane-switching (IPS) liquid crystal device.

88 D, with potential applications as diverse as liquid crystals, diagnostic technology and composite rei

89 trate a giant flexoelectro-optic behavior of liquid crystal dimer CB7CB.

90 hile using a thinner structure, similar to a liquid crystal display (LCD), and enable more efficient

91 supercapacitor watchstrap is used to power a liquid crystal display as an example of load-bearing pow

92 es with built-in laser target projection and liquid crystal display shutters for alternate occlusion

93 Owing to the significant price drop of liquid crystal displays (LCDs) and the efforts to save n

94 cations such as photovoltaics, touch panels, liquid crystal displays, and organic light-emitting diod

95 scent qdots that are now used in three-color liquid-crystal displays in large televisions.

96 ic molecular mesogens, like the ones used in liquid-crystal displays, these defect structures are ind

97 with examples ranging from cell membranes to liquid-crystal displays.

98 atics are a fundamentally different class of liquid crystals, driven away from equilibrium by the aut

99 s presented here suggest that particle-laden liquid crystal droplets could provide a unique and versa

100 Here we demonstrate that liquid crystal droplets deposited on microthin biofibers

101 from nematic to smectic A in hybrid-aligned liquid crystal droplets on water substrates, using exper

102 ition patterns of drying lyotropic chromonic liquid crystal droplets.

103 ctrochemical immunosensor based on the ionic liquid crystal (E)-1-decyl-4-[(4-decyloxyphenyl)diazenyl

104 ilica as the substrate to align the discotic liquid crystal, edge-plane carbon surfaces were formed.

105 onance and a combination of bulk and surface liquid crystal effects that manifest at different voltag

106 lection band of a single crystal cholesteric liquid crystal elastomer (CLCE).

107 Two-dimensional liquid-crystal elastomer (LCE) sheets with preprogrammed

108 rative soft-lithography on a backing splayed liquid-crystal elastomer (LCE).

109 on of soft, ordered materials referred to as liquid crystal elastomers.

110 t soft microrobots consisting of photoactive liquid-crystal elastomers can be driven by structured mo

111 Liquid-crystal elastomers with exchangeable links (xLCEs

112 of responsive materials including hydrogels, liquid-crystal elastomers, shape-memory polymers, and aq

113 switch that drives the twisting of strips of liquid-crystal elastomers.

114 by the symmetries associated with electronic-liquid-crystal (ELC) phases.

115 es the application potential of graphene for liquid crystal electro-optic devices with complex and hi

116 d inversion of the handedness of cholesteric liquid crystals enabled by photoisomerizable chiral mole

117 these distortion-separated charges to induce liquid crystal-enabled electro-osmosis.

118 platform for versatile applications such as liquid crystal-enabled electrokinetics, micropumping and

119 The obtained lyotropic liquid crystal engineering design rules can be used to e

120 re related to a biconvex shape of the chiral liquid crystal film; the rings are due to interference.

121 ction at the free surface of aligned nematic liquid crystal films.

122 ing from particles dispersed in free nematic liquid crystal films.

123 ed to the design of improved chemoresponsive liquid crystals for selectively detecting other chemical

124 saddle-splay elastic constant for chromonic liquid crystals for the first time.

125 re we report the organization of cholesteric liquid crystal formed by nanorods in spherical droplets.

126 delivery strategy based on a supramolecular liquid crystal formed by peptide amphiphiles (PAs) that

127 olide nonapeptide, the in vitro release from liquid crystal formulations was accurately quantified as

128 oride micelles for the assembly of lyotropic liquid crystals generates new structural complexity and

129 sturb the alignment of rod-like molecules of liquid crystals, giving rise to long-range interactions

130 fects at the mesoscale, manifested in chiral liquid crystal guest materials confined in a chiral, nan

131 The B4 phase of bent-core liquid crystals has been shown to be an assembly of twis

132 f-assembling properties of columnar discotic liquid crystals have stimulated intense research toward

133 mixture of shape-persistent liquid crystals, liquid crystals having reactive end groups, molecular ph

134 were doped into a dual-frequency cholesteric liquid-crystal host to appraise both their compatibility

135 eir organo-solubility and compatibility in a liquid-crystal host.

136 volume-based concept is transferred to ionic liquid crystals (ILs that adopt liquid crystalline mesop

137 an oblique helicoidal state of a cholesteric liquid crystal in a wide temperature range (including ro

138 ver, upon confinement of lyotropic chromonic liquid crystals in cylindrical geometries, here we uncov

139 tational changes of surface-anchored nematic liquid crystals in response to chemical stimuli.

140 Unconventional ionic liquid crystals in which the liquid crystallinity is ena

141 uid crystals, and 2) imidazolium-based ionic liquid crystals in which the occurrence of liquid crysta

142 ed for the first time to reconstruct the air-liquid crystal interface of a nematic material, namely,

143 Surprisingly, the liquid/crystal interfacial free energy does not appear i

144 nterestingly, the smectic order in the ionic-liquid-crystal ionogel facilitates ionic transport.

145 icrystalline tilings as platelets in nematic liquid crystals is inherently capable of a continuous va

146 structures (i.e. cholesteric, chiral nematic liquid crystals) is currently in the limelight because i

147 In the liquid crystal isotropic phase, electric field-induced c

148 Liquid crystal (LC) assembly is exceptionally sensitive

149 Liquid crystal (LC) based sensors covered with LPS monol

150 angles using a fringe field switching (FFS) liquid crystal (LC) cell.

151 The structure and physical properties of liquid crystal (LC) mixtures are a function of compositi

152 tions resulted in phase transition to either liquid crystal (LC) or coarse emulsion (CE).

153 aces formed between coexisting isotropic and liquid crystal (LC) phases to provide insight into how m

154 We developed a liquid crystal (LC) sensor system for detecting mercuric

155 A multi-layer liquid crystal (LC) spatial light modulator offers a lar

156 The performance of liquid crystal (LC) spatial light modulators depends cri

157 In this paper, construction of the liquid crystal (LC)-based sensing platform for simple an

158 We report a new mechanism for liquid crystal (LC)-based sensor system for trypsin dete

159 er an assembly of gold nanorods dispersed in liquid crystals (LC) is demonstrated.

160 Confined liquid crystals (LC) provide a unique platform for techn

161 In this work, lyotropic chromonic liquid crystals (LCLCs) are confined in spherical drople

162 en demonstrated by using lyotropic chromonic liquid crystals (LCLCs) as these materials show spontane

163 ts of 2D nanomaterials, and the formation of liquid crystals (LCs) allows the creation of continuous

164 The orientations of liquid crystals (LCs) anchored on monolayers formed from

165 al symmetry-broken configurations of nematic liquid crystals (LCs) confined to cylindrical capillarie

166 Topological defects in liquid crystals (LCs) have been widely used to organize

167 ed for aligning the molecular orientation in liquid crystals (LCs) in patterns with designer complexi

168 The water solubility of lyotropic liquid crystals (LCs) makes them very attractive to stud

169 Liquid crystals (LCs), because of their long-range molec

170 Liquid crystals (LCs), owing to their anisotropy in mole

171 Design and synthesis of photochromic liquid crystals (LCs), photoinduced phase transitions in

172 rphous blue phase III (BPIII) of cholesteric liquid crystals (LCs), which can impart optical isotropy

173 ambers, that strong confinement of colloidal liquid crystals leads to novel defect-stabilized symmetr

174 e light focusing, including zoom, fluid, and liquid-crystal lenses.

175 urface, leading to multiparticle sheets with liquid-crystal-like organization.

176 Properties unique to liquid crystals likely enable long-range signal transduc

177 ll filled with a mixture of shape-persistent liquid crystals, liquid crystals having reactive end gro

178 e introduce a class of active matter--living liquid crystals (LLCs)--that combines living swimming ba

179 Nematic liquid crystals make promising chemoresponsive systems,

180 rns shows that the structural order of these liquid crystals matches that of solid crystals, often of

181 display in terms of the physical property of liquid crystal material and the electrode structure.

182 vations on 40-120 nm films of four bent-core liquid crystal materials show that the filaments are pre

183 h and upconversion nanoparticles, doped in a liquid crystal media, were able to self-organize into an

184 Adding colloidal nanoparticles into liquid-crystal media has become a promising pathway eith

185 mers with various degree of complementarity, liquid crystal microdomains are formed via the selective

186 Here, by combining liquid crystal microfluidic experiments, nonequilibrium

187 rs, sensors, nonlinear optical chromophores, liquid crystals, microporous polymers for energy storage

188 terfacial geometries in sintering of smectic liquid crystals might pave the way for new approaches to

189 d in this work by introducing into a nematic liquid crystal mixture a cylindrical body that exhibits

190 he unusual molecular environment provided by liquid crystal mixtures.

191 S-nucleophiles including the synthesis of a liquid crystal molecule.

192 is itself an assembly of achiral, bent-core liquid crystal molecules that phase-separate into a cong

193 lar boundary conditions for the alignment of liquid crystal molecules, so that they generate a host o

194 ion that facilitates planar anchoring of the liquid-crystal molecules at the droplet surface, as conf

195 design and synthesize a new type of nematic liquid crystal monomer (LCM) system with strong dipole-d

196 topological defects are prepared by aligning liquid-crystal monomers within micropatterned epoxy chan

197 inated fibrillar adhesives to hybrid nematic liquid crystal network (LCN) cantilevers.

198 For example, liquid-crystal networks can be programmed to undergo sti

199 th fast cis-to-trans thermal relaxation into liquid-crystal networks, we generate photoactive polymer

200 l droplets, have been studied in the nematic liquid crystal (NLC) 4-cyano-4'-pentylbiphenyl (5CB): Bo

201 Nematic liquid crystals (NLCs) of achiral molecules and racemic

202 anisotropic dyes and wide ranging choice of liquid crystals nonlinear optical mechanisms, these all-

203 The liquid crystal nonsymmetric dimer, 1-(4-butoxyazobenzene

204 educed graphene oxide in a lyotropic nematic liquid crystal of graphene oxide flakes using a pulsed n

205 propriate combinations of metal cations with liquid crystals of suitable molecular structure.

206 approaches, such as the self-organization of liquid crystals, offer potential advantages over top-dow

207 Spatial inhomogeneity of liquid crystals offers the capability to organize colloi

208 ly of DNA origami filaments into cholesteric liquid crystals, one-dimensional supramolecular twisted

209 t devices driven by bacterial fluids, active liquid crystals or chemically engineered motile colloids

210 modulators based on quantum-well structures, liquid crystals, or meta-materials, significantly improv

211 e lacking because macroscopic orientation of liquid-crystal order, which is required for reversible a

212 ted solutions of short DNA oligomers develop liquid crystal ordering as the result of a hierarchicall

213 n the presence of abiotic condensing agents, liquid crystal ordering markedly enhances ligation effic

214 li, which can even be used to manipulate the liquid crystal organisation in time.

215 This delicate nature of force balance in liquid crystals organization forms the basis of Liquid-c

216 eved to result from an interplay between the liquid crystal orientation at the particles' surface, th

217 Chiral nematic liquid crystals--otherwise referred to as cholesteric li

218 re then propagates well into the bulk of the liquid crystal, particularly for nematic and smectic pha

219 The sensors exploit thermochromic liquid crystals patterned into large-scale, pixelated ar

220 le the study and application of thermotropic liquid crystal phase behavior without thermal degradatio

221 taneously aligns into an equilibrium nematic liquid crystal phase that is also macroscopically ferrom

222 y, we introduce a new methodology to control liquid crystal phase transitions in anisotropic colloida

223 Upon transition to the smectic liquid crystal phase, optical memory of the written stat

224 spersed in water, formed a lyotropic nematic liquid crystal phase.

225 In contrast, the liquid-crystal phase in supercooled n-butanol is found t

226 he shear forces of bubbling, and we observed liquid-crystal phase transitions in (MBBA).

227 ght-handed to left-handed through an achiral liquid-crystal phase, whereas its reverse process occurs

228 Specific precursor polymers form discotic liquid crystal phases during the pyrolysis process.

229 nents gave rise to hexagonal columnar (Colh) liquid crystal phases, which are stable at room temperat

230 Liquid-crystal phases are generally regarded as being "i

231 Remarkably, electronic liquid-crystal phases can exist in two-dimensional elect

232 e-handed columns and a columnar hexagonal 2D liquid crystal, Phi(h).

233 A highly-effective liquid crystal photoalignment method is used to maximize

234 atly advances this tuning and demonstrates a liquid crystal-plasmonic system that covers the full RGB

235 show that anisotropic photosensitive nematic liquid crystals (PNLC) made by incorporating anisotropic

236 The use of nematic liquid crystal polydomains confined in a polymer network

237 eet of a hydrogen-bonded, uniaxially aligned liquid crystal polymer network.

238 They are made from liquid crystal polymer networks in which an azobenzene d

239 Liquid crystal polymer networks respond with an anisotro

240 propose randomly ordered polydomain nematic liquid crystal polymer networks to reversibly generate n

241 enzene molecules are often incorporated into liquid-crystal polymer films to make them photoresponsiv

242 of long-lived photomechanical deformation in liquid-crystal polymer networks.

243 ontinuum level for designing and engineering liquid crystal polymeric devices.

244 Furthermore, the assembly of the liquid crystals promotes a substantial increase in the c

245 otubes act as a conductive network, with the liquid crystal providing a host medium to allow the cond

246 Numerous applications of liquid crystals rely on control of molecular orientation

247 zing an engineered surface which allows full liquid crystal reorientation while maximizing the overla

248 Blue phases of liquid crystals represent unique ordered states of matte

249 c materials has been a long-standing goal of liquid crystal research.

250 constraints in the molecular ordering of the liquid crystal, resulting in the formation of defects.

251 such as scars, pleats, folds, blisters, and liquid crystal ripples.

252 e particles' surface, the orientation at the liquid crystal's air interface, and the bulk elasticity

253 ts, one can gain additional control over the liquid crystal's elasticity.

254 rates, alignments layers, nature and type of liquid crystals, sensing compartments, various interface

255 C) analysis of GGC in a DNA-origami nanotube liquid crystal shows that several structured segments ha

256 Theory has predicted the existence of a liquid-crystal smectic phase that breaks both rotational

257 c liquid to a nematic phase and finally to a liquid-crystal smectic phase.

258 a photoresponsive self-organized cholesteric liquid crystal superstructure under the simultaneous inf

259 crystallographic direction of a soft, cubic liquid-crystal superstructure, exhibiting an alternate u

260 nt, vividly colored materials from colloidal liquid crystal suspensions of cellulose nanocrystals are

261 Here we show that the elasticity of a liquid crystal system consisting of a dense suspension o

262 we have experimentally realized a lyotropic liquid crystal system that can be truly engineered, with

263 an anhydrous nanoDNA-surfactant thermotropic liquid crystal system, which exhibits distinctive electr

264 as accomplished in the nanoparticle-embedded liquid-crystal systems.

265 ol-gel matrix, followed by extraction of the liquid crystal template, affords a hierarchical macropor

266 tyrene nanosphere templates from a lyotropic liquid crystal-templated silica sol-gel matrix, followed

267 We review the scope and limitations of liquid crystal templating and look out to where the tech

268 Recently, liquid crystal templating was also realised in water.

269 A new method is based on liquid crystal templating.

270 magnetic self-interaction effects, including liquid crystal textures of fluid block domains arranged

271 We detected dissolved xenon in an aqueous liquid crystal that is disrupted by the shear forces of

272 he fabrication of monocrystalline blue phase liquid crystals that exhibit three-dimensional photonic-

273 ly processes which occur in unique phases of liquid crystals that exhibit three-dimensional photonic-

274 Ionic currents in liquid crystals that have been traditionally considered

275 odelling the epithelium as an active nematic liquid crystal (that has a long range directional order)

276 On addition of chiral dopants to the liquid crystal, the films exhibit optical textures with

277 Being a liquid crystal, the host material can be ordered at many

278 er subject to reorientation, such as nematic liquid crystals, the nonlinear interaction with light al

279 single-walled carbon nanotubes suspended in liquid crystal; the nanotubes act as a conductive networ

280 ition cannot be readily explained by current liquid crystal theories based on isotropic domains.

281 Active liquid crystal theories have been developed to study the

282 e we show that a suitably constructed active liquid crystal theory produces remarkably accurate predi

283 In comparison to conventional liquid crystals, there is considerable freedom to prescr

284 With the inclusion of a homochiral guest liquid crystal, these enantiomeric domains become diaste

285 In confined chiral nematic liquid crystals, this self-assembly is similar to that o

286 self-assembles into a smectic-ordered ionic liquid crystal through Coulombic interactions between th

287 Pseudomonas aeruginosa self-assembles into a liquid crystal through entropic interactions between pol

288 al systems ranging from classical fluids and liquid crystals, to electromagnetism, classic, and quant

289 g the Early Universe development, whereas in liquid crystals transient tangled defect lines were obse

290 l-stress relaxation through the creep of non-liquid-crystal transient networks with exchangeable link

291 een mistakenly interpreted, and is in fact a liquid-crystal transition in all atomistic models of wat

292 ciated with an isotropic to rippled lamellar liquid-crystal transition.

293 Only a small set of liquid crystals used for RDC measurements are compatible

294 the colloidal self-organization in a nematic liquid crystal using laser tweezers, particle tracking a

295 rface in conjunction with high birefringence liquid crystals, we demonstrate a tunable polarization-i

296 Liquid crystals, when confined to a spherical shell, off

297 al singularities of molecular arrangement in liquid crystals, which typically occur when the average

298 gy between the epithelium and active nematic liquid crystals will trigger further investigations of t

299 established protocols for the orientation of liquid crystals with a uniform magnetic field, and throu

300 Liquid crystals with helical cholesteric order offer a p