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1 ontaneous polar symmetry breaking in a fluid smectic.
2 ientation of the layers for simple, lamellar smectics.
3 two mesophases: chevron smectic C (cSmC) and smectic A (SmA).
4 diacrylate monomers dissolved in fluid-layer smectic A and smectic C liquid crystal (LC) hosts exhibi
5 ucturing the Gaussian and mean curvatures of smectic A films with free surface in the process of sint
6 itu thermal phase transition from nematic to smectic A in hybrid-aligned liquid crystal droplets on w
7 heliconical twist-bend phase into a lamellar smectic A mesophase, additionally this material exhibits
8 of defects may be related across the nematic-smectic A phase transition, and presents new possibiliti
9   3a forms a nematic phase, while 3b forms a smectic A phase.
10 ratios increase the temperature range of the smectic A phases beyond the decomposition temperatures;
11 nes increased not only the fluidity of their smectic A phases but also their thermal and chemical sta
12                                          The smectic A(F) is a phase of small polar, rod-shaped molec
13             We report the observation of the smectic A(F), a liquid crystal phase of the ferroelectri
14 he pyrenyl dendrimers exhibit a multilayered smectic A-like phase, thereafter referred to as LamSmA p
15 ains, periodically intermixed with bend-free smectic-A domains.
16                                         In a smectic-A LC, the emergence of positional order at the t
17  toric focal conic domains (TFCDs) arrays of smectic-A liquid crystals is studied.
18 al assembly of focal conic domains (FCDs) in smectic-A liquid crystals that break the underlying symm
19         Here, we show, unambiguously, that a smectic-A type of phase is formed by increasing the DNA'
20 ng clear evidence of an elementary lamellar (smectic-A) phase in DNA solutions-are two exciting devel
21 urface charge of the disks, we find nematic, smectic and columnar organizations with symmetries rangi
22 h height modulation was also observed in the smectic and hexatic phases.
23            Unlike fluid threads in modulated smectics and columnar phases, where translational order
24 ntal and vertical) and ordering (nematic and smectic), and depending on the dimensionality of the str
25  Here, we present the first observation of a smectic B (Sm(B)) phase in a system of charged colloidal
26           Supramolecular interactions in the smectic biogels play an important role for their high pl
27 tures arise from a common structure: "giant" smectic blocks of planar layers of thickness l(b) > 200
28 ly stable structure to be a uniformly tilted smectic bow-phase (banana phase), with all layer pairs h
29 sotropic droplets dispersed over a spherical smectic bubble, observed under microgravity conditions o
30 stomers that exhibit two mesophases: chevron smectic C (cSmC) and smectic A (SmA).
31 omers dissolved in fluid-layer smectic A and smectic C liquid crystal (LC) hosts exhibited significan
32 state of matter which we conclude is a polar smectic C phase, and so we term it SmC(P).
33                                      Two new smectic C* mesogens containing a hexyloxy side chain and
34                         The rod-coils formed smectic C-like and O-like morphologies with domain sizes
35  additional short-range structures including smectic C-type correlations in all three phases-N, SmZ(A
36 icrodomains of thermoplastic elastomers with smectic clay of similar characteristic dimensions.
37   Here we explore the intrinsic structure of smectic colloidal layers dictated by the interplay betwe
38  of the bilayer bending modulus K(C) and the smectic compression modulus B.
39             This tensorial theory for simple smectics considerably simplifies numerics, facilitating
40 ures ranging from laminar states to multiple smectic domains and arrays of edge dislocations, which w
41 ture such as membranes, block copolymers and smectics exhibit intriguing morphologies with nontrivial
42  this layer structure, which we designate as smectic-fA phase, is thermodynamically stabilized by bot
43 ion and restructuring, initially equilibrium smectic films with negative and zero Gaussian curvature
44 onal twists, cholesteric helical ribbons and smectic helicolidal nanofilaments.
45  zero and positive mean curvature of the air-smectic interface has a profound effect on the rate of s
46 ld-less and has no hysteresis, while for the smectic it has a clear threshold and shows hysteresis me
47 s including crystalline discrete assemblies, smectic lamellar liquid crystals, and large uni- or mult
48 a surface-relief grating to control both the smectic layer and director orientations.
49 rector and polarization oriented parallel to smectic layer planes, and the polarization alternating i
50 propose a geometric model to reconstruct the smectic layer structure in the gaps between neighboring
51                                 Two distinct smectic layer structures are observed for DNA concentrat
52 lay stripes spaced by defects and coupled to smectic layer undulations.
53 n the order of 10(3), and the absence of any smectic layer X-ray diffraction peaks.
54       Such spatial segregation caused by the smectic layering dramatically enhanced photopolymerizati
55               The diffraction peaks from the smectic layering have not been observed to date but deta
56 e perpendicular orientation of the mesogenic smectic layers (lam) with respect to the BCPE cylinders
57    This mode undergoes "self-healing" of the smectic layers after disruption by shock-induced flow.
58 2-methylbenzene (C6M) oriented normal to the smectic layers and collected within them.
59 l diacrylate (HDDA) oriented parallel to the smectic layers and intercalated, whereas rod-shaped meso
60                                     However, smectic layers are sensitive to shock-induced flow and a
61 C spacer leads to hierarchical ordering with smectic layers of mesogens existing alongside larger len
62 scovered smectic Z(A) (SmZ(A)) phase, having smectic layers with the molecular director parallel to t
63 d lubricating the thermal contraction of the smectic layers within the blocks.
64 -sticks) attain a folded conformation in the smectic layers, and argue that this layer structure, whi
65  phase having the director parallel to fluid smectic layers, significantly increasing its temperature
66 ch fills a 100-y-old void in the taxonomy of smectic LCs and which we term the "smectic Z(A)," is ant
67 ese stabilization methods can be extended to smectic LCs to create droplets with more complex interna
68 s are responsible for the liquid crystalline smectic-like behaviour of such systems at intermediate l
69                                              Smectic-like order in vapor-deposited films was characte
70                                              Smectic-like ordering of the nanorods appears very early
71  biaxial nematic phases, polar and antipolar smectic-like phases, and even the long-predicted, elusiv
72  equilibration mechanism predicts the highly smectic-like vapor-deposited structure to be a result of
73 nd spatial patterning of defect domains in a smectic liquid crystal (LC) by geometric confinement in
74 ms, fluid molecular monolayer and multilayer smectic liquid crystal films suspended in air, is report
75                                         This smectic liquid crystal is thus a fluid conglomerate.
76                                 This fragile smectic liquid crystal layering, the material with the s
77 ntials to dominate, leading to an electronic smectic liquid crystal phase in which electrons are orde
78                       Upon transition to the smectic liquid crystal phase, optical memory of the writ
79 ariety of simple bent-core molecules exhibit smectic liquid crystal phases of planar fluid layers tha
80  dicationic compounds, respectively, display smectic liquid crystal phases.
81 limiting ferroelectricity to crystals and to smectic liquid crystal stackings of fluid layers.
82            We show that glasses with aligned smectic liquid crystal-like order can be produced by phy
83 cid)s that self-assemble into highly ordered smectic liquid crystalline mesophases were investigated
84 26)PA(2) and is identified as a thermotropic smectic liquid crystalline phase.
85                                 A nanoporous smectic liquid crystalline polymer network has been expl
86 materials such as thermotropic and lyotropic smectic liquid crystals and block copolymers.
87       Here, we report a class of fluid polar smectic liquid crystals in which local splay prevails in
88 r and interfacial geometries in sintering of smectic liquid crystals might pave the way for new appro
89 des two equilibrium systems: two-dimensional smectic liquid crystals, and a peculiar kind of constrai
90         An example of particular interest is smectic liquid crystals, where the two-dimensional layer
91 kin to the packing of focal conic domains in smectic liquid crystals.
92 we identify growing dense regions similar to smectic liquid crystals.
93                                            A smectic liquid-crystal phase made from achiral molecules
94  the behavior of other amphiphiles that form smectic liquid-crystal phases.
95 re amorphous and that they transition into a smectic liquid-crystalline phase surrounding an amorphou
96             Study of a diverse set of chiral smectic materials, each of which has twist grain boundar
97 olesteric materials and chiral ferroelectric smectic materials, it is of great interest to probe ligh
98                       We show that the polar smectic mesophase exhibited by the first molecule discov
99 pheres, to relieve distortion of an internal smectic mesophase.
100  long-range 2D hydrogen-bond networks in the smectic mesophases over a wide temperature window.
101 and ordering of lamellar superstructures and smectic mesophases, as manifested by liquefaction and so
102 ear p-alkoxyphenyl units led to bilayer-type smectic mesophases, wedge-shaped units resulted in colum
103 nstrated in the nematic, chiral-nematic, and smectic mesophases.
104 ns from or into the nematic, cholesteric and smectic mesophases.
105 and perspectives on the design of functional smectic microarrays.
106 on density, and thus has nematic rather than smectic molecular ordering.
107                   We report the SmAP(F), the smectic of fluid polar orthorhombic layers that order in
108 ribing the combined presence of nematic and 'smectic' or stripe-like orders seen in recent scanning t
109                           Interestingly, the smectic order in the ionic-liquid-crystal ionogel facili
110  informed engineering of different levels of smectic order in vapor-deposited glasses to suit various
111                                          The smectic order is treated as an electronic charge density
112                         At 95 degrees C, the smectic order melted to form a hexatic phase.
113 ry is partially broken, with the nematic and smectic order parameters increasing over days.
114 ere we report that, in addition to the usual smectic order, multicomponent multilayer membranes can e
115 red above T(m), indicating that the PDW is a smectic order.
116 ped with lithium salt, self-assembles into a smectic-ordered ionic liquid crystal through Coulombic i
117                                              Smectic ordering in aqueous solutions of monodisperse st
118  of the nature and temperature dependence of smectic ordering in concentrated solutions of various "g
119 lpha,L-glutamate) prepared in this way shows smectic ordering in solution and in films.
120  length is large, and featuring GBs in which smectic ordering is weak, approaching thin, melted (nema
121 de larger length-scale lamellae, versus only smectic ordering without the spacer.
122 l intralayer phase separation and interlayer smectic ordering.
123 tic discotic to a fluid, but highly ordered, smectic phase at a temperature that depends on the thuli
124 2D orthorhombic crystal phase melted to a 2D smectic phase at about 91 degrees C.
125           The large temperature range of the smectic phase for the azafluorenol 3b is indicative of m
126  predicted the existence of a liquid-crystal smectic phase that breaks both rotational and translatio
127 tions revealed a structural evolution from a smectic phase to a columnar phase.
128                                          The smectic phase was characterized by 1D molecular periodic
129 from the nematic phase produces a frustrated smectic phase with depressed transition temperature, and
130           These may become restricted in the smectic phase, affecting the exchange rate of lipids wit
131 cluding nematic phases with lock structures, smectic phase, and particularly experimental observation
132            This so-called positively ordered smectic phase, whose lipids consist of less than 1% DMPE
133 sotropic and nematic states, can also form a smectic phase.
134 ematic phase and finally to a liquid-crystal smectic phase.
135 where flexibility typically destabilizes the smectic phase.
136  layered structures that can be described as smectic phases and can also order into single-crystal st
137 an the 50% that is typically achievable with smectic phases formed by more conventional convex rod- o
138 pportunity to study a transition between two smectic phases having orthogonal systems of layers.
139 d crystal (LC) compound exhibiting two fluid smectic phases in which two-dimensional, polar, orthorho
140 organizations, and temperature ranges of the smectic phases of a structurally diverse family of phosp
141 cule, LCs and is considerably greater in the smectic phases of the resulting systems relative to the
142                           We show that these smectic phases possess uniquely high free volumes of up
143                                The anhydrous smectic phases that result exhibit biomacromolecular sub
144 stent with their topology-chiral nematic and smectic phases were identified as well as the rarely obs
145 isperse polymers might provide access to new smectic phases with layer spacings that are susceptible
146 ss or promote the formation of ferroelectric smectic phases, depending on their position within the m
147                                              Smectic phases, in which macromolecular rods are organiz
148  self-organize into room-temperature bilayer smectic phases, mandated by the specific mesogenic funct
149 citations and the near-degeneracy with other smectic phases.
150  form a variety of ferroelectric nematic and smectic phases.
151 liquid crystal, particularly for nematic and smectic phases.
152  formation of distinctive liquid-crystalline smectic phases.
153                                     A stable smectic phospholipid bilayer phase aligned with the dire
154                                              Smectics represent the paradigm of such lamellar materia
155 nel seemingly erratic depinning events along smectic river networks correlated over system spanning s
156          An orientationally disordered, spin-smectic state resolves previously perceived contradictio
157        The higher-temperature phase is a new smectic state with periodic undulation of the polarizati
158 first-principles calculations reveal a "spin-smectic" state lower in energy than previous results.
159 s are commonly limited to nematic or layered smectic structures dominated by the parallel arrangement
160  three-dimensional model for two-dimensional smectics that clarifies the topology of disclinations an
161 tural generalizations of the two-dimensional smectic theory to higher dimensions and to crystals.
162 amental evidence for theories of the nematic-smectic transition, highlighting the deep connection bet
163 liar critical behavior of LCs at the nematic-smectic transition, still eluding a comprehensive theore
164                             Interestingly, a smectic-type liquid crystalline phase is observed at tem
165 s another example of the recently discovered smectic Z(A) (SmZ(A)) phase, having smectic layers with
166 d mesogens: 2N/DIO, exhibiting a nematic (N)-smectic Z(A) (SmZ(A))-ferroelectric nematic (N(F))-SmA(F
167      Ionic liquid doping also stabilizes the smectic Z(A), an additional birefringent antiferroelectr
168 xonomy of smectic LCs and which we term the "smectic Z(A)," is antiferroelectric, with the nematic di

 
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