ライフサイエンスコーパス: lyotropic

1 Lyotropic aggregation of rhodoxanthin (E/Z)-isomer mixtu

2 (E/Z)-ratios by thermal (E/Z)-isomerization, lyotropic aggregation, and two different formulation tec

3 structures that exhibit thermotropic and/or lyotropic behavior.

4 derivative capable of self-assembling into a lyotropic chiral nematic phase in aqueous solution.

5 s are carried out using Sunset Yellow FCF, a lyotropic chromonic LC with a small twist elastic consta

6 orphology, and deposition patterns of drying lyotropic chromonic liquid crystal droplets.

7 In this work, lyotropic chromonic liquid crystals (LCLCs) are confined

8 nd templating has been demonstrated by using lyotropic chromonic liquid crystals (LCLCs) as these mat

9 ent measurements of the elastic constants in lyotropic chromonic liquid crystals (LCLCs) have reveale

10 r growth, the intrinsic tumbling behavior of lyotropic chromonic liquid crystals can be suppressed, w

11 Achiral nematic lyotropic chromonic liquid crystals have been reported t

12 However, upon confinement of lyotropic chromonic liquid crystals in cylindrical geome

13 rticles in linear defects-disclinations in a lyotropic colloidal cholesteric liquid crystal: a contin

14 Thus, these lyotropic DDQCs are long-lived metastable morphologies,

15 celles into previously unrecognized, aqueous lyotropic dodecagonal quasicrystals (DDQCs), which exhib

16 inued susceptibility to LOR (associated with lyotropic formation of the hexagonal II phase) and assoc

17 interfacial water within a "normal" (Type I) lyotropic gyroid phase formed by a gemini dicarboxylate

18 icelles and cylinders up to the formation of lyotropic hexagonal or lamellar phases results from coop

19 aspartate, chloride, etc., produce a marked lyotropic (Hofmeister) effect on the repetitive structur

20 This material is based on a polymerizable lyotropic (i.e., amphiphilic) liquid crystal (1) that fo

21 mesogenic properties, both thermotropic and lyotropic (in DMF) mesophases were observed in one of me

22 ces self-assembly into both thermotropic and lyotropic lamellar liquid crystalline (LC) phases.

23 d bacteria when swimming in solutions of the lyotropic LC disodium cromoglycate (DSCG).

24 lue phases, achiral bent-core LCs, etc.) and lyotropic LCs (DNA LCs, nanocellulose LCs, and graphene

25 patterning, templating, and when extended to lyotropic LCs, a process leading to uniform-sized spheri

26 of azobenzene photosurfactants (AzoPS) into lyotropic liquid crystal (LLC) phases, which are explore

27 The lyotropic liquid crystal (LLC) systems consist of amphip

28 r concentration, the helical polymer forms a lyotropic liquid crystal (LLC) that further orients unid

29 The antibiotic squalamine forms a lyotropic liquid crystal at very low concentrations in w

30 The mechanical strengthening of the lyotropic liquid crystal by the two-tailed 1,2-dioleoyl-

31 The obtained lyotropic liquid crystal engineering design rules can be

32 of gas (CO(2)) diffusion across a prototype lyotropic liquid crystal membrane.

33 Here we show that topologically-active lyotropic liquid crystal nanoparticles (LCNPs) can trigg

34 media, the vast majority have supported some lyotropic liquid crystal phase formation.

35 We focus upon the generation of 'dilutable' lyotropic liquid crystal phases with two- and three-dime

36 ation of this unique class of nonamphiphilic lyotropic liquid crystal shares enormous similarity to t

37 The lyotropic liquid crystal state formed by these polymers

38 Thus, we have experimentally realized a lyotropic liquid crystal system that can be truly engine

39 l of polystyrene nanosphere templates from a lyotropic liquid crystal-templated silica sol-gel matrix

40 hat combines living swimming bacteria with a lyotropic liquid crystal.

41 strength of the cubic-phase monoolein/water lyotropic liquid crystal.

42 fraction, dispersed polymer nanofibers form lyotropic liquid crystalline (LC) mesophases with comple

43 ollable, rapid, and continuous production of lyotropic liquid crystalline (LLC) nanoparticles (both c

44 pack into a previously unknown, low-symmetry lyotropic liquid crystalline Frank-Kasper sigma phase.

45 Lipid based lyotropic liquid crystalline mesophases have demonstrate

46 remarkable array of tunable and pH-sensitive lyotropic liquid crystalline mesophases including the in

47 Ordered nanostructured lyotropic liquid crystalline mesophases may form in sele

48 in modulating the biophysical properties of lyotropic liquid crystalline nano-self-assemblies.

49 Here we have engineered highly sensitive lyotropic liquid crystalline nanoparticles that reversib

50 s electrodeposited from the hexagonal (H(I)) lyotropic liquid crystalline phase are shown to be excel

51 We report the discovery of a lyotropic liquid crystalline phase based on a 3-D hexago

52 tion, suspensions were prepared in which the lyotropic liquid crystalline phase behavior of the hybri

53 the metal, in the simultaneous presence of a lyotropic liquid crystalline phase of nonionic surfactan

54 chemically deposited from the hexagonal (H1) lyotropic liquid crystalline phase of the nonionic surfa

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

56 round a prolate ellipsoidal type I hexagonal lyotropic liquid crystalline phase.

57 iquid interface, similar to the formation of lyotropic liquid crystalline phases by common surfactant

58 The outstanding diverse functionalities of lyotropic liquid crystalline phases found in nature and

59 They form lyotropic liquid crystalline phases in helicogenic solve

60 These copolymers form uncrosslinked, lyotropic liquid crystalline phases of large micelles be

61 he formation of the known classes of lipidic lyotropic liquid crystalline phases, their structure, an

62 the high mesogen concentration required for lyotropic liquid crystalline spinning.

63 dition of the acidic lipid component to this lyotropic liquid crystalline system reduces its range of

64 The water solubility of lyotropic liquid crystals (LCs) makes them very attracti

65 rmed of thermodynamically stable cubic phase lyotropic liquid crystals (LLCs) could replace the prese

66 Lyotropic liquid crystals (LLCs) have well-defined inter

67 nts of the elastic constants in the micellar lyotropic liquid crystals (LLCs) that are formed by surf

68 ree most common bicontinuous cubic phases in lyotropic liquid crystals and block copolymers.

69 mesophase transition at room temperature in lyotropic liquid crystals constructed from arylazopyrazo

70 monium chloride micelles for the assembly of lyotropic liquid crystals generates new structural compl

71 l evaluation, and therapeutic application of lyotropic liquid crystals in the field of parenteral sus

72 ueous interconnected networks of cubic-phase lyotropic liquid crystals, urate permeates only through

73 to engineer a potentially rich assortment of lyotropic liquid crystals.

74 ilding blocks of both micellar and chromonic lyotropic liquid crystals.

75 The synthesis and lyotropic liquid-crystalline (LLC) phase behavior of a h

76 The aqueous, lyotropic liquid-crystalline phase behavior of the alpha

77 PtGeQ and C(n)PyPtSnSe were templated by the lyotropic liquid-crystalline phase of alkylpyridinium su

78 This is the first new inverse lyotropic liquid-crystalline phase to be reported for tw

79 first use of magnetic-alignment behavior of lyotropic liquid-crystalline polymer macro-nanodiscs (>2

80 Achieving control and tunability of lyotropic materials has been a long-standing goal of liq

81 , and contrary to what is perceived for soft lyotropic materials in general, the self-assembly method

82 ugh liquid-liquid phase separation (LLPS) of lyotropic mesophases from isotropic solutions upon a con

83 mainly (2)H 1D/2D-NMR in chiral polypeptide lyotropic mesophases, are presented and analyzed.

84 sses) in the presence of molecular porogens, lyotropic mesophases, supramolecular architectures, emul

85 Lyotropic mesophases, where membranes conform to periodi

86 o assemble into high-aspect ratio (>10(3) ), lyotropic nanotubes in the presence of excess acid.

87 This lyotropic nematic exhibited the slowest dielectric relax

88 crostructures of reduced graphene oxide in a lyotropic nematic liquid crystal of graphene oxide flake

89 eter of 10 mum, dispersed in water, formed a lyotropic nematic liquid crystal phase.

90 re traditionally classified as thermotropic, lyotropic or polymeric, based on the stimulus that gover

91 hat poly(norbornene) BBPs exhibit long-range lyotropic ordering as a result of their rodlike characte

92 the lack of rigidity necessary to access the lyotropic ordering that underpins the formation of colla

93 OR15amr and COR6.6r on the cryostability and lyotropic phase behavior of liposomes are examined.

94 ll quaternary mixtures showed highly regular lyotropic phase behavior with the same sequence of phase

95 The lyotropic phase behaviour of model lipid systems that de

96 ported for two decades and is the only known lyotropic phase whose structure consists of a close pack

97 ction of the fatty acid with ozone, and that lyotropic-phase formation also occurs in more complex mi

98 We suggest that lyotropic-phase formation likely occurs in the atmospher

99 centrations of water and surfactant in these lyotropic phases also triggers formation of the related

100 el of the uncharged lipid displays the usual lyotropic phases as a function of the relative volume fr

101 self-assembly (PISA) can be used to prepare lyotropic phases comprising diblock copolymer nano-objec

102 ate that the droplets contained crystal-like lyotropic phases including hexagonal and cubic close-pac

103 Lyotropic polymer liquid crystals are unique systems for

104 s, which, moreover, exhibit viscoelastic and lyotropic properties.

105 hich forms 2.3 nm diameter water channels by lyotropic self-assembly.

106 The influence of select salts from the lyotropic series (NH(4)Cl, KCl, NaCl, MgCl(2), CaCl(2),

107 e expect an ion's position in the Hofmeister lyotropic series to be determined by a combination of dr

108 e guanidinium cation effect according to the lyotropic series.

109 h layered materials such as thermotropic and lyotropic smectic liquid crystals and block copolymers.

110 This is unusual for a lyotropic system, where flexibility typically destabiliz

111 Such phases are found in lyotropic systems (for example, lipid-water, soap-water)

112 e transition temperatures of other lipid and lyotropic systems.