ライフサイエンスコーパス: liquid-crystalline

1 lipid species as long as all lipids remained liquid-crystalline.

2 P and (2)H solid-state NMR spectra show that liquid crystalline 1,2-dimyristoyl-sn-glycero-3-phosphoc

3 t the pathway and the rate of flip-flop in a liquid crystalline 1,2-dipalmitoyl-sn-glycero-3-phosphat

4 Two types of liquid crystalline [2]rotaxanes based on a conventional

5 measured for the same solution, under static liquid crystalline alignment, and under magic angle spin

6 PbSe nanorods were assembled to provide liquid-crystalline alignment or vertical alignment under

7 Self-organization of liquid crystalline and crystalline-conjugated materials

8 OXD12) exhibiting interesting enantiotropic liquid crystalline and gelation properties have been syn

9 ned from a mixed state to a coexistence of a liquid-crystalline and a gel, or a liquid-ordered and a

10 lations predict the formation of various new liquid-crystalline and plastic-crystalline phases at int

11 icantly, while anionic membranes in the gel, liquid crystalline, and liquid ordered phases induce the

12 of the thermal stability of semicrystalline, liquid-crystalline, and glassy organic semiconductor thi

13 Non-lamellar liquid crystalline aqueous nanodispersions, known also a

14 well as probably control their conversion, a liquid crystalline arrangement is established in the sto

15 of viral double-stranded RNA, packaged in a liquid crystalline array.

16 the 3,4,5-substituted derivatives displayed liquid crystalline behavior (Col(h) and Col(r)), only th

17 hese complexes display thermotropic columnar liquid crystalline behavior in spite of having only a si

18 This represents a unique example of liquid-crystalline behavior observed for such large and

19 Liquid crystalline behaviour is generally limited to a s

20 Achieving liquid-crystalline behaviour in inorganic fluids should

21 to the novel materials presented herein its liquid-crystalline behaviour is rather different, indica

22 ropy (or high uniaxial anisotropy) favouring liquid-crystalline behaviour.

23 lting occurs, and C16:0-LacCer converts to a liquid crystalline bilayer (L(alpha)) phase of reduced p

24 nriched in dipalmitoylphosphatidylcholine, a liquid-crystalline bilayer phase, and an extremely mobil

25 nformations of the polyunsaturated chains in liquid-crystalline bilayers, which favor chain extension

26 ted layer structures in a series of rod-coil liquid crystalline block copolymers (BCPs), poly(styrene

27 lipid-assisted translocation of CPPs across liquid-crystalline cell membranes.

28 tially from most of these, but is closest to liquid crystalline cetyl pyridinium bromide.

29 eukaryotes arranged on permanently condensed liquid-crystalline chromosomes.

30 henylene with the shortest alkoxy chains was liquid crystalline (Col(r)).

31 ange of micellar, rod-like, bicontinuous and liquid-crystalline complex fluids.

32 f parallel DNA ligands in the self-assembled liquid-crystalline complex.

33 xyphenyl)pyridine ligands leads to emissive, liquid-crystalline complexes containing bound Cl and dim

34 al shift under isotropic and weakly aligning liquid crystalline conditions is very sensitive to minut

35 This liquid-crystalline conjugated polymer was realized by in

36 -concentration solutions, both isotropic and liquid crystalline, could be particularly useful for mak

37 gy and bilayer organization typical of their liquid-crystalline counterparts, making them useful memb

38 The lipidic liquid-crystalline cubic phase (LCP) is a membrane-mimet

39 s colloidal system, we describe analogies to liquid crystalline deformations with bend, splay and twi

40 aged into preformed bacteriophage capsids to liquid crystalline density by the action of a portal pro

41 has been prepared from the nitro-substituted liquid crystalline derivative.

42 analogs of spermine to induce and stabilize liquid crystalline DNA.

43 ayer could result from the appearance of gel/liquid-crystalline domain boundaries at this POPE conten

44 the cooperative dynamics and deformation of liquid-crystalline domains and their boundaries.

45 bled by graphene: Graphene sheets aligned in liquid crystalline elastomers are capable of absorbing n

46 ighly nonlinear mechanical properties of the liquid crystalline elastomers examined here enables stra

47 y dispersing swimming Bacillus subtilis in a liquid crystalline environment with spatially varying or

48 rface, a planar alignment is promoted in the liquid crystalline film.

49 the electric-field-induced orientation of a liquid-crystalline film of 4-n-pentyl-4'-cyanobiphenyl w

50 ed through the synthesis of two thermotropic liquid-crystalline fluorescent benzobis(imidazolium) sal

51 otenoids accumulate in a lipid-dissolved and liquid-crystalline form, respectively.

52 , is packed inside its icosahedral capsid in liquid-crystalline form, with concentrations near or mor

53 a previously unknown, low-symmetry lyotropic liquid crystalline Frank-Kasper sigma phase.

54 concentrations, NFs align to form a nematic liquid crystalline gel with a well-defined spacing deter

55 n, liquid crystalline micellar solution, and liquid crystalline hexagonal phase solution, were compar

56 d biological membranes is characterized by a liquid-crystalline, highly dynamic state.

57 In this hierarchical approach, a liquid crystalline host serves as the scaffold to order

58 the organisation of the materials inside the liquid crystalline host.

59 The scope of the new procedure (relative to liquid crystalline intermediates) is presented and is co

60 A new liquid-crystalline ion gel exhibits unprecedented proper

61 At 60 degrees C, in the liquid-crystalline L(alpha) phase, the bilayer periodici

62 pure DOPE-Me is heated slowly, the lamellar liquid crystalline (L(alpha)) phase first forms an inver

63 PC fractions, these lipids are in a miscible liquid crystalline (L(alpha)) state, whereas at lower te

64 se separation into liquid-ordered (L(o)) and liquid-crystalline (L(alpha)) phases is observed by both

65 sphocholine (PDPC), have been studied in the liquid-crystalline (L(alpha)) state and compared to the

66 more comprehensive picture of lipids in the liquid-crystalline (L(alpha)) state than formerly possib

67 Both the lower-temperature, liquid-crystalline lamellar (L(alpha)) and the higher-te

68 Liquid-crystalline lamellar phases surrounding the fat g

69 an upshift of the temperature of the gel-to-liquid crystalline (Lbeta - Lalpha) phase transition, le

70 Incorporation of liquid crystalline (LC) block can provide additional way

71 ing hydrogels comprising unique thermotropic liquid crystalline (LC) domains and magnetic nanoparticl

72 We report the formation of liquid crystalline (LC) phases of short double-stranded

73 cattering (2DWAXS), the elevated temperature liquid crystalline (LC) phases were assigned to a hexago

74 nto both thermotropic and lyotropic lamellar liquid crystalline (LC) phases.

75 f a liquid-ordered (Lo) phase, and that of a liquid-crystalline (Lc) phase as represented by model me

76 liquid-ordered (Lo) phase versus that of the liquid-crystalline (Lc) phase in multibilayer phospholip

77 These mixtures possess liquid-crystalline-like phases that can be processed.

78 e, the structure of CrgA was determined in a liquid-crystalline lipid bilayer environment by solid-st

79 The synthesis and lyotropic liquid-crystalline (LLC) phase behavior of a homologous

80 study of molecular order within a chromonic liquid crystalline material (sunset yellow) in aqueous s

81 in this work) remains the only example of a liquid-crystalline material to exhibit a phase transitio

82 cal review of semiconducting/light emitting, liquid crystalline materials and their use in electronic

83 cal review of semiconducting/light emitting, liquid crystalline materials and their use in electronic

84 we focus on the developments of light-driven liquid crystalline materials containing photochromic com

85 Recently, liquid crystalline materials endowed with photoresponsiv

86 ment and academia are increasingly examining liquid crystalline materials in a variety of polymeric f

87 A group of new liquid crystalline materials with aromatic cores compris

88 with different structures can result in new liquid crystalline materials, or in segregation of the m

89 nterest because of their significant role as liquid crystalline materials, organic light-emitting dio

90 chanically aligned lipid bilayers as well as liquid crystalline materials.

91 and diversify the scope of the light-driven liquid crystalline materials.

92 strategy for manipulating the properties of liquid-crystalline materials.

93 Liquid crystalline matrices composed of amphiphilic comp

94 Photoresponsive hybrid gold nanorod-liquid crystalline matrices were prepared and loaded int

95 a two stage release process unique to these liquid crystalline matrices.

96 The aqueous liquid crystalline media investigated include the common

97 poly(ethylene glycol), and filamentous phage liquid crystalline media, dipolar couplings were also me

98 th phage pf1 and polyethylene glycol/hexanol liquid crystalline media.

99 However, none of the existing liquid-crystalline media used to align water-soluble pro

100 biological macromolecules weakly aligned by liquid-crystalline media, are important global angular r

101 In this communication, we present a robust liquid crystalline medium that is positively charged, pi

102 idual dipolar couplings obtained in a single liquid crystalline medium, DMPC/DHPC bicelles (DMPC = di

103 DP ribosylation factor 1 (ARF1) aligned in a liquid crystalline medium.

104 sive chiral molecular switch into an achiral liquid crystalline medium.

105 accommodation between lipids, whereas in the liquid-crystalline membrane, in which the distance betwe

106 In the liquid-crystalline membrane, the complexed M2TMP shows d

107 sembly of Cu alkanethiolates into an ordered liquid crystalline mesophase plays an essential role in

108 d more ordered with thermal annealing in the liquid crystalline mesophase.

109 LCP is a liquid-crystalline mesophase composed of lipids and wate

110 Lipid based lyotropic liquid crystalline mesophases have demonstrated exceptio

111 hich fibrillar collagen structures form from liquid crystalline mesophases is not well characterized.

112 Ordered nanostructured lyotropic liquid crystalline mesophases may form in select mixture

113 red to ionic liquid crystals (ILs that adopt liquid crystalline mesophases, ILCs) for predicting the

114 as well as the ability to self-assemble into liquid crystalline mesophases.

115 ray diffraction to characterize the columnar liquid-crystalline mesophases in concentrated solutions

116 everal media, conventional aqueous solution, liquid crystalline micellar solution, and liquid crystal

117 an ABA triblock copolymer with a side-group liquid-crystalline midblock and liquid-crystal-phobic en

118 ergosterol increases acyl chain order in the liquid crystalline model membranes, but to differing deg

119 In bulk phase, liquid crystalline molecules are organized due to non-co

120 nd solute molecules undergoes dehydration, a liquid crystalline multilamellar matrix is produced that

121 Interestingly, the silica-nanoparticle-doped liquid-crystalline nanocomposites were found to be able

122 ical nucleic acids, deformable liposomes and liquid crystalline nanodispersions.

123 t when the electrophoresis is performed in a liquid-crystalline nematic fluid, the effect becomes str

124 amic covalent chemistry is incorporated into liquid crystalline networks (LCNs) to facilitate spatiot

125 fined lamellae are a structural feature of a liquid crystalline neutral lipid core that is a determin

126 is method is illustrated for the case of the liquid crystalline oil 4-pentyl-4'-cyanobiphenyl (5CB).

127 Cells transfected with hCERK showed a higher liquid crystalline order than control cells with stimula

128 romosome exhibit multistability with varying liquid crystalline ordering that may allow discrete unfo

129 its high sensitivity to probe the impact of liquid-crystalline ordering on charge mobility in polyme

130 Combining such nanoobjects with liquid-crystalline orderings to control their assembly a

131 Targeting filamentous bacteriophage or the liquid crystalline organization of the biofilm matrix ma

132 der of alignment within the culture showed a liquid-crystalline pattern containing interspersed topol

133 d(GpG) is very similar to that observed for liquid crystalline Pf1 bacteriophage, but of opposite si

134 he static magnetic field when dissolved in a liquid crystalline Pf1 suspension.

135 eposited from the hexagonal (H(I)) lyotropic liquid crystalline phase are shown to be excellent amper

136 amer in both the solid state and the aqueous liquid crystalline phase are well reproduced.

137 ely little is known about how defects in one liquid crystalline phase arise from defects or deformati

138 tive magneto-LC effect in columnar hexagonal liquid crystalline phase as probed by differential scann

139 s of the 2H NMR spectra were observed in the liquid crystalline phase at and above 0 degrees C.

140 We report the discovery of a lyotropic liquid crystalline phase based on a 3-D hexagonal close-

141 The liquid crystalline phase behavior of 4-[6-(4'-cyanobiphe

142 ensions were prepared in which the lyotropic liquid crystalline phase behavior of the hybrid material

143 e addition of equimolar CHOL in the lamellar liquid crystalline phase causes a smaller increase in or

144 responsible for the formation of the layered liquid crystalline phase consisting of hexagonally order

145 The liquid crystalline phase consisting of the potassium sal

146 type of lipid bilayer disk or bicelle, and a liquid crystalline phase formed by a cationic lipid.

147 n lipid bilayer in the biologically relevant liquid crystalline phase has been examined by performing

148 suggested that freezing the LDL core into a liquid crystalline phase imposes structural constraints

149 ences of the formation of a novel electronic liquid crystalline phase in its vicinity.

150 The liquid crystalline phase is a necessary requirement for

151 These data suggest that the LDL core in the liquid crystalline phase is characterized by the appeara

152 Interestingly, a smectic-type liquid crystalline phase is observed at temperatures bet

153 nment tensors through steric interactions, a liquid crystalline phase of cetylpyridinium bromide alig

154 The chiral nematic liquid crystalline phase of d(GpG) consists of long colu

155 The fully hydrated liquid crystalline phase of the dimyristoylphosphatidych

156 deposited from the hexagonal (H1) lyotropic liquid crystalline phase of the nonionic surfactant octa

157 It is based on the formation of a lyotropic liquid crystalline phase on the surface of the liquid fi

158 esicle dispersions, even though the lamellar liquid crystalline phase thickness of C20BAS is only 32

159 The half-time for the liquid crystalline phase to switch is very fast and prop

160 Kdo(2)-Lipid A suspensions revealed a gel-to-liquid crystalline phase transition at 36.4 degrees C (T

161 The gel-to-liquid crystalline phase transition is successively weak

162 But below the gel-to-liquid crystalline phase transition temperature, an addi

163 roup mobility of SM both above and below the liquid crystalline phase transition temperature, whereas

164 ent 31P NMR was used to determine the gel-to-liquid crystalline phase transition temperatures of the

165 metry, we found that the width of the gel-to-liquid crystalline phase transition was 2 degrees C broa

166 Both chiral liquid crystalline phase transitions and competing inter

167 ructural specificity effect of polyamines on liquid crystalline phase transitions of DNA and suggest

168 bility and monitor the gel-to-gel and gel-to-liquid crystalline phase transitions of SM as a function

169 Films deposited from the hexagonal liquid crystalline phase were shown to be ion selective,

170 n to self-assemble into a hexagonal columnar liquid crystalline phase, and respond to applied electri

171 phase in equilibrium with an ordered nematic liquid crystalline phase, results in a clear phase separ

172 nsport and light emission is affected by the liquid crystalline phase.

173 nsport and light emission is affected by the liquid crystalline phase.

174 olate ellipsoidal type I hexagonal lyotropic liquid crystalline phase.

175 ty that averages the dipolar coupling in the liquid crystalline phase.

176 ak hydrophobic interactions, indicative of a liquid crystalline phase.

177 o 16:0-22:6PE-d(31)/SM (1:1) bilayers in the liquid crystalline phase.

178 umns assemble further into a two-dimensional liquid crystalline phase.

179 SM and increased acyl chain ordering in the liquid crystalline phase.

180 s from unbinding of dislocations-a 'hexatic' liquid crystalline phase.

181 mol % PCer, PSM and PCer mix ideally in the liquid crystalline phase; in the gel phase, PCer becomes

182 ve also confirmed uptake by the resin in the liquid-crystalline phase and release in the gel phase.

183 ning calorimetry indicates a transition to a liquid-crystalline phase at 81 degrees C.

184 The aqueous, lyotropic liquid-crystalline phase behavior of the alpha-helical p

185 between them, as the baseline, we report the liquid-crystalline phase behaviors of two other related

186 Thermotropic and enantiotropic liquid-crystalline phase formation of 1PnX salts is favo

187 When cooled from the untilted L(alpha) liquid-crystalline phase into the tilted gel phase, vesi

188 C(n)PyPtSnSe were templated by the lyotropic liquid-crystalline phase of alkylpyridinium surfactant [

189 ese measurements point to the formation of a liquid-crystalline phase of P3HT solutions within a spec

190 TP-I and TPF4 are both highly mobile in the liquid-crystalline phase of the membrane while the inact

191 ed to approximately 5-15 microm, whereas the liquid-crystalline phase P-d31OPC permeated to substanti

192 This is the first new inverse lyotropic liquid-crystalline phase to be reported for two decades

193 e conducted at temperatures below the gel to liquid-crystalline phase transition of the membrane lipi

194 ring has confirmed the retention of a gel to liquid-crystalline phase transition of the surfactant, o

195 oss-linked polymer is controlled by a gel to liquid-crystalline phase transition.

196 .5 A, indicating that the bilayers were in a liquid-crystalline phase, and several sharp low-angle re

197 rs in bilayers of phosphatidylcholine in the liquid-crystalline phase.

198 ilayers are fully hydrated and in the fluid (liquid-crystalline) phase.

199 oundaries between the ordered and disordered liquid crystalline phases (L and L) were similar for SM

200 nded compounds of molybdenum and tungsten in liquid crystalline phases are described.

201 ispersed with cellulose nanocrystals to form liquid crystalline phases are developed.

202 s work provides new insights into the use of liquid crystalline phases as templates for nanocrystal s

203 rface, similar to the formation of lyotropic liquid crystalline phases by common surfactants.

204 The liquid crystalline phases of matter each possess distinc

205 Liquid crystalline phases of matter permeate nature and

206 he expression of metastability, a feature of liquid crystalline phases that might be exploited in low

207 on could be suppressed, and room-temperature liquid crystalline phases were obtained.

208 For liquid crystalline phases, it is important to understand

209 The morphologies of three dilute liquid crystalline phases, which are widely used for bio

210 emble into nanoscale fibers, aggregates, and liquid crystalline phases.

211 ouplings for molecules dissolved in oriented liquid crystalline phases.

212 chain and 1 is the methyl group) do not form liquid-crystalline phases as a consequence of strong alt

213 We also report spontaneous formation of liquid-crystalline phases at high concentrations ( appro

214 bient temperature (293 K), at which gel- and liquid-crystalline phases coexist in the peptide-free PO

215 g of graphene oxide flakes in self-assembled liquid-crystalline phases enables laser patterning of co

216 to the trends mentioned for the 1PnX salts, liquid-crystalline phases of mPnYX are found more freque

217 The observation that the liquid-crystalline phases of mPnYX salts have lower clea

218 Liquid-crystalline phases of stacked lipid bilayers repr

219 ng uniform lattice orientation in frustrated liquid-crystalline phases, like cubic blue phases, is a

220 sidue mercury transporter MerF determined in liquid crystalline phospholipid bilayers under physiolog

221 The receptor is in liquid crystalline phospholipid bilayers, without modifi

222 ly (13)C/(15)N labeled protein in unoriented liquid crystalline phospholipid bilayers.

223 rane mimetic environment (e.g., micelles) vs liquid crystalline phospholipid bilayers.

224 ly(3-hexylthiophene-2,5-diyl), P3HT, and the liquid-crystalline poly(2,5-bis (3-tetradecylthiophen-2-

225 ected against dissolution into the LCLC by a liquid crystalline polymer layer.

226 A nanoporous smectic liquid crystalline polymer network has been exploited to

227 ilms prepared from azobenzene-functionalized liquid crystalline polymer networks (azo-LCNs).

228 ls consist of molecular switches embedded in liquid-crystalline polymer springs.

229 iew, we detail the historical development of liquid crystalline polymeric materials, with emphasis on

230 to responsive helices based on hydrogels and liquid crystalline polymers have been reported, they hav

231 of controlled diameter, made from main-chain liquid crystalline polymers using a mini-emulsion techni

232 Light-driven phenomena and properties of liquid crystalline polymers, elastomers, and networks ha

233 Liquid-crystalline polymers are materials of considerabl

234 Such stretchable liquid-crystalline polymers have previously been demonst

235 phenyl methylpolysiloxane and dimethyl (50% liquid crystalline) polysiloxane] were compared, and ret

236 )(H(2)O)(4)] SMM, differing in the number of liquid-crystalline promoters, (L(x,y,z-CB)), were synthe

237 he four-ring derivatives 2c and 2d exhibited liquid crystalline properties (2c: Cr 95 SmA 158 I and 2

238 Such features suggest liquid crystalline properties during the evolution of th

239 The same complex displays liquid crystalline properties on heating from rt to abov

240 e, we demonstrate that the piezoelectric and liquid-crystalline properties of M13 bacteriophage (phag

241 copolymers self-assemble due to a balance of liquid crystalline (rod-rod) and enthalpic (rod-coil) in

242 self-assembly into phases with crystalline, liquid crystalline, rotator, or noncrystalline phases wi

243 ng can be engineered and pre-programmed in a liquid crystalline rubbery material given a well-control

244 that manipulates the alignment director of a liquid crystalline sample to obtain anisotropic magnetic

245 to the applied magnetic field in a spinning liquid crystalline sample, the dipolar couplings present

246 rs, such as dipolar coupling, in an oriented liquid crystalline sample.

247 us, these molecules display more classically liquid-crystalline self-assembly behavior where the lame

248 update progress on the surface alignment of liquid crystalline semiconductors to obtain monodomain d

249 update progress on the surface alignment of liquid crystalline semiconductors to obtain monodomain d

250 These features are responsible for the liquid crystalline smectic-like behaviour of such system

251 ture leading to the formation of distinctive liquid-crystalline smectic phases.

252 olar coupling of a sample weakly oriented in liquid crystalline solution.

253 recise control of the polymer structure with liquid crystalline solutions demonstrates the importance

254 s (RDCs) in differentially orienting aqueous liquid crystalline solutions to obtain the side chain ch

255 ular weight for polymer solutes dissolved in liquid crystalline solvents.

256 nded conformations when dissolved in nematic liquid crystalline solvents.

257 e' (the material from which silk is spun) is liquid crystalline, spiders can draw it during extrusion

258 mesogen concentration required for lyotropic liquid crystalline spinning.

259 ntal conditions, DNA can also transform to a liquid crystalline state in vitro.

260 order in t18:1-18:0PC (S(CD) = 0.135) in the liquid crystalline state is much closer to that of c18:1

261 ellar assemblies are rapidly frozen from the liquid crystalline state to the gel phase, indicate the

262 opts a rigid beta-strand conformation in the liquid-crystalline state of anionic lipid membranes.

263 rformed for 50 ns at 350 K and 1 bar for the liquid-crystalline state of the mixtures.

264 The use of the liquid-crystalline state to control the assembly of larg

265 ers a composition-driven transition from the liquid-crystalline state to the gel state at 22.4 degree

266 nthophyll esters, prevailing in a presumably liquid-crystalline state within the nano-scaled chromopl

267 exagonal structure and stabilize the bilayer liquid-crystalline state, suggesting that sHsps can modu

268 ry large values of approximately 0.35 in the liquid-crystalline state.

269 looser as compared to the homogenous gel or liquid-crystalline state.

270 and alpha-crystallin strongly stabilize the liquid-crystalline state.

271 rientations, and interactions in the natural liquid-crystalline state.

272 s into a 2D hexagonal lattice; (ii) selected liquid-crystalline states in which crystalline lamellae

273 This liquid crystalline structure enhances biofilm function b

274 e as a nanofiber model system to exploit its liquid crystalline structure for the creation of diverse

275 In this unique self-assembled liquid crystalline structure, transverse-lying pi-conjug

276 with an ordered hexagonal columnar (Col(ho)) liquid crystalline structure, where shrinkage during the

277 ave engineered lamellar, cubic and hexagonal liquid-crystalline structure in metal-halide melts by co

278 s with nanoscale features is the transfer of liquid-crystalline structure to polymers.

279 Here we propose the design of highly open liquid-crystalline structures from rigid nanorings with

280 ing in the formation of lamellar-type binary liquid crystalline superlattices.

281 the acidic lipid component to this lyotropic liquid crystalline system reduces its range of stability

282 The high metal content of these liquid-crystalline systems significantly advances the fi

283 cules that get trapped in disordered (H1) or liquid crystalline (T1) mesophases require additive proc

284 Above and below the lipid gel-liquid crystalline temperature, partitioning is exotherm

285 Liquid crystalline textures were identified under a pola

286 that partition coefficients were greater for liquid-crystalline than solid-gel phase membranes, wheth

287 We report on new semiconducting liquid-crystalline thieno[3,2-b ]thiophene polymers, the

288 ogy on the anchoring, order, and dynamics of liquid crystalline thin films.

289 e that undergoes a thermal transition from a liquid crystalline to an isotropic liquid phase between

290 ignificantly reduced the temperature for the liquid crystalline to hexagonal phase transition in arti

291 The liquid crystalline-to-gel phase transition temperature o

292 olar CHOL essentially obliterates the gel-to-liquid crystalline transition of 16:0-18:1PE-d(31).

293 This motion is frozen below the gel-to-liquid crystalline transition temperature of the lipids.

294 ylcholine (DPPC), which has a similar gel-to-liquid crystalline transition temperature.

295 ures above that associated with their gel-to-liquid-crystalline transition (Tm); at temperatures belo

296 rms and reduction in the enthalpy of the gel-liquid-crystalline transition in DSC scans showed CHOL h

297 material and induces reversible thermotropic liquid-crystalline transitions.

298 direct or wide-field Raman imaging employing liquid-crystalline tunable filters are surveyed.

299 r phase and explains why this medium remains liquid crystalline well below the Onsager limit for disk

300 Many of these structures are liquid-crystalline with structural motifs mirrored in ce