ライフサイエンスコーパス: liquid crystal

1 n 4-cyano-4'-pentylbiphenyl (5CB), a nematic liquid crystal.

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

3 r stabilized uniform lying helix cholesteric liquid crystal.

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

5 c in contact with a hydrophobic thermotropic liquid crystal.

6 shown that the spindle behaves as an active liquid crystal.

7 andedness of a helical organization within a liquid crystal.

8 helical superstructure, i.e., a cholesteric liquid crystal.

9 dynamic phases of superconductors and chiral liquid crystals.

10 eter-sized knots in helical fields of chiral liquid crystals.

11 imensional orientation fields in cholesteric liquid crystals.

12 cts in molecular orientation widely found in liquid crystals.

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

14 for controlled deformation and patterning of liquid crystals.

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

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

17 by modeling the membrane particles as chiral liquid crystals.

18 he packing of focal conic domains in smectic liquid crystals.

19 nment without translational order in nematic liquid crystals.

20 r a potentially rich assortment of lyotropic liquid crystals.

21 as yet unexplored regime of highly confined liquid crystals.

22 e self-assembly and nanosegregation of these liquid crystals.

23 e report the first alternating network cubic liquid crystals.

24 ide ions, both in isotropic solutions and in liquid crystals.

25 cks of both micellar and chromonic lyotropic liquid crystals.

26 "diabolic" domains in bend-free textures of liquid crystals.

27 (2) area with no micromechanical elements or liquid crystals.

28 catalysis, and components of materials like liquid crystals.

29 Strong-coupling theories of electronic liquid crystals(18,19) are consistent with these observa

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

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

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

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

34 ogen-modified nanoparticles are dispersed in liquid crystal above the nematic-isotropic transition te

35 ually considered to resist all deformations, liquid crystals actually have an intrinsic propensity to

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

37 diverse areas as well as comparing them with liquid crystals, amphidynamic crystals, ordered crystals

38 modulation, and switching of thermo-optical, liquid crystal and phase change media.

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

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

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

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

43 ductors, proteins, ultrathin magnetic films, liquid crystals and metallic alloys(5,6), with the notab

44 hene oxide particles, dispersed in a nematic liquid crystal, and contained within a microfluidic chan

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

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

47 the same way bimodal blends of surfactants, liquid crystals, and polymers are used to engineer the m

48 tes the first report of amphiphilic CD-based liquid crystals applied as proton conductive materials.

49 Nematic liquid crystals are anisotropic fluids that self-assembl

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

51 duced helical superstructures of cholesteric liquid crystals are highlighted.

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

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

54 akthrough in the design of inverse chromonic liquid crystals, as assembly under such mild conditions

55 The first deltic ionic liquid crystals based on aminocyclopropenium ions have b

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

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

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

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

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

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

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

63 mechanism for the formation of cavity-cored liquid crystals, but also provides a convenient approach

64 ed to rotate a glass rod on the surface of a liquid crystal by synthetic molecular motors.

65 Colloidal interactions in nematic liquid crystals can be described as interactions between

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

67 via molecular entanglement (conformation) to liquid-crystal (centimetre-scale) chirality.

68 a 3-dimensional (3D) droplet of cholesteric liquid crystal (CLC) embedded in an isotropic liquid.

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

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

71 Cholesteric liquid crystals (CLCs) are a unique class of light-manip

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

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

74 In liquid-crystal colloids(5-7), elastic interactions betwe

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

76 e salient features of two-dimensional active liquid crystals composed of energy-consuming anisotropic

77 tep gram-scale electrosynthesis of a nematic liquid crystal compound, demonstrating its practicality.

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

79 duction of helical superstructure in nematic liquid crystals containing a very small quantity of the

80 tices, superconductors, magnetic flux tubes, liquid crystals, cosmic strings, and DNA is the phenomen

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

82 -Hilliard simulations of phase separation in liquid crystal demonstrate qualitatively that partitioni

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

84 We synthesized the liquid crystal dimer and trimer members of a series of f

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

86 However, while the liquid crystal dimer exhibits a temperature-dependent va

87 We consider tangential anchoring of the liquid crystal director at the droplet surface.

88 The branched structures with confined liquid crystal director fields can be produced reversibl

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

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

91 ration with an actively addressed reflective liquid crystal display with control over black states.

92 Core projection systems including liquid crystal displays and digital micromirror devices

93 diodes) and colloidal nanocrystals (e.g., in liquid crystal displays and future quantum light sources

94 arises under conditions similar to those in liquid crystal displays and may enable dynamic materials

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

96 an experimental geometry resembling that of liquid crystal displays.

97 rve as good candidates for chemo sensors and liquid crystal displays.

98 stationary cross-polarizers in, for example, liquid crystal displays.

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

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

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

102 thesis of room-temperature columnar discotic liquid crystals (DLCs).

103 In achiral liquid crystals, dopant knotted and unknotted strands in

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

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

106 ions of water droplets inside radial nematic liquid crystal droplets to form various structures, rang

107 nt surface morphologies, revealed by nematic liquid crystal droplets.

108 ition patterns of drying lyotropic chromonic liquid crystal droplets.

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

110 al is composed of a compliant and deformable liquid crystal elastomer (LCE) matrix that can achieve m

111 this study, waveguided light is harnessed by liquid crystal elastomer (LCE) nanocomposites to drive a

112 Here, we develop patterned liquid crystal elastomer (LCE) particles by recapitulati

113 photocurable, thus DLP-printable main-chain liquid crystal elastomer (LCE) resin is reported and use

114 Employing liquid crystal elastomer-carbon nanotube composites as a

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

116 effect of dynamic soft elasticity in nematic liquid crystal elastomers (LCE), the temperature-depende

117 Photoresponsive liquid crystal elastomers (LCEs) are a unique class of a

118 Liquid crystal elastomers (LCEs) are an attractive platf

119 Liquid crystal elastomers (LCEs) are anisotropic polymer

120 Liquid crystal elastomers (LCEs) are of interest for app

121 3D printable and reconfigurable liquid crystal elastomers (LCEs) that reversibly shape-m

122 square centimetre and can be converted into liquid crystal elastomers by ultraviolet curing.

123 s have reported light-induced actuation with liquid crystal elastomers combined with azobenzene photo

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

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

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

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

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

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

130 rientationally ordered fluids, i.e., nematic liquid crystals, enabled by a visible-light-driven chira

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

132 experimental regimes where generic, achiral liquid crystals exhibit spontaneously broken surface sym

133 Cholesteric liquid crystals fabricated using these new fluorescent m

134 shba-Dresselhaus spin-orbit interaction in a liquid crystal-filled optical cavity.

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

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

137 that exhibit birefringence, thus indicating liquid crystal formation.

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

139 When a liquid crystal forming particles are confined to a spati

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

141 common to sea invertebrates using monolithic liquid crystal gels (LCGs) with inherent light responsiv

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

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

144 effective description of wrinkle patterns as liquid crystals [H.

145 posed as the quantum analogue of cholesteric liquid crystals-has attracted considerable interest(3-15

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

147 mercially available room-temperature achiral liquid crystal host 5CB, which also acts as a halogen-bo

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

149 bited a high helical twisting power (HTP) in liquid crystal hosts and a large change of HTP value upo

150 en doped into commercially available achiral liquid crystal hosts, this molecular switch efficiently

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

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

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

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

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

156 The director field adopted by a confined liquid crystal is controlled by a balance between the ex

157 cture associated with a colloid in a nematic liquid crystal is dictated by molecular orientation at t

158 The first single-diamond cubic phase in a liquid crystal is reported.

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

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

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

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

163 Spontaneous breaking of symmetry in liquid crystal (LC) films often reveals itself as a micr

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

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

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

167 tutorial review includes an introduction to liquid crystal (LC)-based materials and highlights devel

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

169 mage resistance of saturated and unsaturated liquid crystals (LC's) under a wide range of laser excit

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

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

172 the elastic constants in lyotropic chromonic liquid crystals (LCLCs) have revealed an anomalously sma

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

174 rable complex colloids comprising immiscible liquid crystals (LCs) and fluorocarbon oils.

175 tro-active nanostructures sensing materials, liquid crystals (LCs) are emerging as a choice of materi

176 Liquid crystals (LCs) are great candidates for light con

177 Liquid crystals (LCs) are omnipresent in living matter,

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

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

180 onofilament fibers with low-molecular-weight liquid crystals (LCs) stabilized by an outer polymer she

181 Here we leverage this knowledge to design liquid crystals (LCs) supported on ultrathin polycrystal

182 or pressure measurements to identify aqueous liquid crystals (LCs) that are in osmotic equilibrium wi

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

184 In liquid crystals (LCs), defects exist as points of discon

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

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

187 phiphiles against interfaces of thermotropic liquid crystals (LCs; 4-cyano-4'-pentylbiphenyl) trigger

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

189 We show that glasses with aligned smectic liquid crystal-like order can be produced by physical va

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

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

192 elastic constants in the micellar lyotropic liquid crystals (LLCs) that are formed by surfactants, b

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

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

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

196 Here, by combining liquid crystal microfluidic experiments, nonequilibrium

197 preprograming the alignment of a cholesteric liquid crystal mixed with a photo-responsive chiral dopa

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

199 he unusual molecular environment provided by liquid crystal mixtures.

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

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

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

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

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

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

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

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

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

209 Columnar polymers and liquid crystals obtained from pai-conjugated cone-shaped

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

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

212 s were created through a phase separation of liquid crystal oligomers (LCOs) droplet coupled to homeo

213 ns of drops composed of polydisperse nematic liquid crystal oligomers (NLCOs).

214 ising for the development of next-generation liquid crystal on silicon spatial light modulators.

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

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

217 gram on a widely-accessible device such as a liquid-crystal or digital light processing display, crea

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

219 es (polymers), and supramolecules (crystals, liquid crystals, or thin films) containing main-group el

220 ince silencing Integrin-beta1 disrupted both liquid-crystal order and organization of the sinusoidal

221 ot randomly oriented but follow a long-range liquid-crystal order.

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

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

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

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

226 op layer, a SiO(2) -spaced polymer dispersed liquid crystal (PDLC) intermediate layer, and a flexible

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

228 n achieve macroscopic shape change through a liquid crystal phase transition.

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

230 erstructure is reported, i.e., a cholesteric liquid crystal phase, in orientationally ordered fluids,

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

232 s paper, we demonstrate a flexoelectro-optic liquid crystal phase-only device that uses a chiral nema

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

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

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

236 sition of a molecule without any equilibrium liquid crystal phases.

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

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

239 centration, the designs form two-dimensional liquid-crystal phases, which accentuate the inherent str

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

241 We explore and discuss the liquid crystal photonics in the prototype that has a nov

242 duce a method to use polarization optics via liquid crystal photonics to improve the foveated display

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

244 ition of only few optical components such as liquid crystal polarizers to a typical Raman setup.

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

246 Liquid crystal polymer networks respond with an anisotro

247 can drive (chiral) shape transformations in liquid crystal polymer networks, with photogenerated pol

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

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

250 charatnam-Berry (PB) phases can be made with liquid crystal polymers by using a plasmonic photopatter

251 Interfacing molecular photoswitches with liquid crystal polymers enables the amplification of the

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

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

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

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

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

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

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

259 as a miniature platform for controlling the liquid crystal self-assembly of bio-derived polymers, an

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

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

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

263 actually implemented by means of a versatile liquid crystal spatial light modulator, can represent a

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

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

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

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

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

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

270 Hydrazone-doped liquid crystal systems thus diversify the toolbox availa

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

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

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

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

275 A new method is based on liquid crystal templating.

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

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

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

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

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

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

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

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

284 lso show that a recent application of active liquid-crystal theory to such systems is untenable.

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

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

287 g microtubule bundles in a passive colloidal liquid crystal to form a three-dimensional active nemati

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

289 perspectral image cube is created by using a liquid crystal tunable filter (LCTF) to select a specifi

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

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

292 elical superstructures, that is, cholesteric liquid crystals, when doped into the commercially availa

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

294 oach to preparing supramolecular luminescent liquid crystals, which will serve as good candidates for

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

296 One of the phases is a nematic liquid crystal with a highly anisotropic viscosity, allo

297 cillating electric field applied to a chiral liquid crystal with polycrystalline quasi-hexagonal arra

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

299 Liquid crystals with helical cholesteric order offer a p

300 ike other extrinsic mechanisms, we find that liquid crystals with high anchoring strengths can ensure