PMCCPMCCPMCC

Search tips
Search criteria 

Advanced

 
Logo of blackwellopenThis ArticleFor AuthorsLearn MoreSubmit
Chemistry (Weinheim an Der Bergstrasse, Germany)
 
Chemistry. 2017 July 3; 23(37): 8771–8779.
Published online 2017 June 5. doi:  10.1002/chem.201701167
PMCID: PMC5518215

The Shape of Things To Come: The Formation of Modulated Nematic Mesophases at Various Length Scales

Abstract

The twist–bend nematic (NTB) phase is a recently discovered liquid‐crystalline phase that exhibits macroscopic chirality even when formed from achiral materials, and as such presents a unique testbed for studies concerning the spontaneous breaking of mirror symmetry in soft matter. It is primarily exhibited by materials for which the molecular structure is composed of two rigid aromatic units (such as biphenyl connected by a flexible spacer). The local structure of the NTB phase is nematic‐like—with molecules having an average orientational order but no positional order—with a nanoscale helix in which the pitch (i.e., the repeat distance of the helix) is of the order of several nanometres. A helix is chiral, and so the bulk NTB phase—in the absence of a biasing chiral environment—spontaneously separates into macroscopic domains of opposite handedness. After discussing the structure of this mesophase and its elucidation, this concept article presents the molecular factors that determine its incidence. The apparent dependency primarily on molecular shape and bend angle rather than particular functional group combinations manifests in this mesophase being exhibited on length scales far beyond those of simple liquid‐crystalline dimers, not only in oligomers and polymers, but also in aqueous suspensions of micron sized helical particles.

Keywords: hydrogen bonds, liquid crystals, oligomers

Introduction

The twist–bend nematic phase (NTB, also referred to as twist–bend phase or TB) presents perhaps one of the most well‐understood examples of spontaneous breaking of mirror symmetry in soft matter. In the NTB phase there exists a local helical structure of very short pitch of about 10 nm.1 In the NTB phase the molecules are tilted with respect to the helix axis, but lack positional ordering and thus the mesophase is “nematic”.2 Similarly, other modulated nematic‐like mesophases have been predicted to occur (splay–bend nematic (NSB),3, 4 and screw nematic (NS*)5, 6 to give two examples.) The pitch length of the NTB helix (P TB) has been directly measured by freeze–fracture transmission electron microscopy,1, 7, 8 by resonant carbon K‐edge small‐angle X‐ray scattering9 and by resonant selenium small‐angle X‐ray scattering.10 All three methods give a qualitative measurement of the pitch length, which is of the order of several nanometers. Deuterium NMR spectroscopy conducted in situ on samples doped with a suitable spin probe has also been interpreted as supporting the presence of a local helix with a nanoscale pitch (i.e., several molecular lengths),11 although other models have been used to interpret these results.12, 13 Examples of FFTEM, RoSAXS and 2H NMR data are given in Figure 1. These methods have proved invaluable in the study of the NTB phase, providing the strongest evidence yet for the presently accepted model of this phase, and it is to be expected that they will find great utility in the study of other modulated nematic and smectic mesophases as they arise. For example, in addition to the NTB and NSB mesophases already mentioned, an extension of Landau–de Gennes theory of nematics has been used to predict the existence of two as yet experimentally undiscovered polar nematic phases with transverse (NTP) and longitudinal (NLP) polarisation.14

Figure 1
The twist–bend nematic phase: a) Cartoon depiction of a bent, U‐shaped dimers with a bend angle of ≈110° forming a NTB phase whose pitch (P TB) is about 3.5 times the dimer length. b) Resonant small‐angle ...

A helix is inherently chiral and so the helical NTB phase spontaneously separates into macroscale domains of opposite handedness when formed from an achiral material. Due to their flexibility liquid crystal (LC) dimers can adopt a range of conformations, some of which—for example a single gauche in the alkyl chain—will be chiral. In the absence of a biasing chiral environment, such conformers are expected to occur in pairs that are separated by a mirror plane (Figure 2 b) with equal probability, thus the conformationally averaged structure is achiral. The +/− gauche conformers of CB5CB (1,ω‐bis(4‐cyanobiphenyl‐4′‐yl)pentane) are higher in energy than the trans conformers by about 1.8 kJ mol−1 at the B3LYP/6‐31G(d) level of DFT with a rotational barrier of about 14.4 kJ mol−1 (Figure 2 c), which implies that there is rapid interconversion between these states within the temperature range of interest (300–450 K for the 1,ω‐bis(4‐cyanobiphenyl‐4′‐yl)alkane (CBnCB) materials).16, 17 In the case of a biasing chiral environment such as the presence of a chiral additive, or when the material that exhibits the phase is itself chiral, only one hand of the NTB helix forms.18 It has been demonstrated that the local chirality of the NTB phase results in a small chiral biasing of the conformer distribution of bimesogens, but that the spontaneous conformational chirality is not the origin of the chirality of the NTB phase.19

Figure 2
Spontaneous breaking of mirror symmetry and chiral conformational isomerism: a) Cartoon depictions of the local molecular organisation present in the achiral uniaxial nematic phase and the spontaneously chiral twist–bend nematic phase ...

Although initially reported only in methylene linked dimers,21, 22 the NTB phase has been observed in dimers with various linking groups,23, 24, 25, 26 as well as in bent–core materials8 and presently there are about 140 dimeric materials known to exhibit the twist–bend nematic phase.27 A number of different mesogenic units have been studied within the context of the NTB phase as shown in Figure 3 a–c. In addition to the well‐studied cyanobiphenyl derivatives, the NTB phase has been observed for materials with mesogenic units incorporating heterocycles,28 laterally fluorinated rings,22, 29 cyclohexyl and bicyclohexyl rings,30 photoisomerisable azo‐linkers,31 and trimeric systems formed from hydrogen‐bonded dimers of benzoic acid derivatives.32 The largest sub‐grouping within this number is materials possessing methylene linking groups, a nonamethylene spacer and two mesogenic units comprised of two rigid cyclic units (40 in total).33 The bias towards this subdivision is a product of availability of chemical reagents rather than some advantage conferred by this particular combination of structural features. We reported previously for this subdivision, and indeed all comparable divisions that we are aware of, that a linear relationship exists between the NTB–N and N–Iso transition temperatures (Figure 3 d).33 This result complements earlier studies that found no correlation between the incidence of this phase and molecular properties, such as polarisability or electric dipole moment.30, 34 Such an outcome was first noted in a theoretical treatment by Greco et al.35 and later Vaupotic et al. proposed that “the internal structure of the TB nematic is driven mainly by steric interactions.”36 Experimental results would appear to be in agreement with these theoretical treatments; the NTB phase is driven by molecular shape and steric interactions rather than any combination of functional groups and so forth.37 The twist–bend nematic phase can be observed for mixtures between a dimer (or bimesogen, trimesogen etc.) and a rod‐like molecule. Tuchband et al. have demonstrated that for mixtures of the dimer CB7CB with the rod‐like 5CB (4‐pentyl‐4′‐cyanobiphenyl) both the mean NTB pitch length and distribution of pitch lengths (measured by FFTEM38 and carbon K‐edge RoSAXS39) increases with increasing concentration of the rod‐like component. As CB7CB is “bent” and 5CB is rod‐like the increase in pitch length as a function of 5CB concentration may indicate a relationship between the molecular bend angle and the periodicity of the NTB helix.39

Figure 3
Molecular structure and the twist–bend nematic phase: a) core structures incorporating terminal nitrile units;21, 28, 34 b) core structures incorporating fluoro groups or hydrogen bonds;22, 23, 24, 29, 32 c) core structures ...

The odd parity of the central spacer found in all NTB dimers confers a bent molecular shape, and theoretical treatments indicate that the thermal stability of the NTB phase should display a dependency on just how bent (or not) the molecular structure of a given material is.42 In 2016 we reported that the angle between the two mesogenic units is one of the prime factors in determining the thermal stability of the twist–bend nematic phase.43 These investigations were undertaken, in part, to see if theoretical predictions of a link between the bending angle and the NTB phase would be borne out in experimental work. Bend angles were taken to be the all‐trans conformer that we found to be dominant using solution‐based 1D 1H NOESY NMR spectroscopy; indeed this is also reported to be the dominant conformer in the bulk NTB phase from 2H NMR data coupled with DFT calculations.19 The dominance of the all‐trans conformer over other conformations has been demonstrated for both methylene‐ and ether‐linked dimers using proton‐enhanced local field (PELF) NMR spectroscopy on CB7CB19 and dielectric spectroscopy on 1′′‐(2′,4‐difluorobiphenyl‐4′‐yloxy)‐9′′‐(4‐cyanobiphenyl‐4′‐yloxy)nonane (FFO9OCB), respectively.44 In reality the use of a single conformer to describe the bend angle is insufficient for flexible molecules, such as LC dimers, and so we opted to study a new set of materials computationally, obtaining a library of conformers from which we can then obtain the full distribution of bend angles as well as a weighted average molecular bend.45 Table 1 shows the transition temperatures of some cyanobiphenyl dimers with varying linking group and spacer composition. Some values were obtained from a survey of the literature (compounds 3,17 6,46 7,31 8 43), whilst novel compounds were synthesised (compounds 1, 2, 4, 5).45

Table 1
Transition temperatures [°C] for compounds 17, with the trivial names of 3 and 6 also given. Values were taken from.17, 43, 45, 46 *.

Both materials bearing two alkyne linking groups (1 and 2) were non mesogenic, with 2 decomposing upon heating. Paterson et al. reported 1‐(4‐cyanobiphenyl‐4′‐yloxy)‐6‐(4‐cyanobiphenyl‐4′‐yl)hexane (CB6OCB—compound 6 in this work), finding that replacing one of the two methylene groups adjacent to the 4‐cyanobiphenyl mesogenic unit in CB7CB confers a modest increase in the NTB–N transition temperature, T NTB–N.46 Positioning a single ether link in the centre of CB7CB (to give an isomer of 6/CB6OCB) lead to the finding that T NTB‐N drops dramatically relative to both parent materials. Increasing the rigidity of the central spacer of 6 by incorporating an alkyne unit (5) reduces both the clearing point and NTB–N transition temperatures. When two ether‐linking units are used (7/CBO5OCB) there is a prominent reduction in T NTB–N relative to both compounds 3 and 6. The use of two ketones as linking units (8) led to a large increase in both T NTB–N and T N–Iso relative to the parent compound 3.43

Performing relaxed scans using the AM1 semi empirical method to obtain a library of conformers for compounds 38 (Figure 4 a) allows a Boltzmann weighted average bend angle to be obtained (Figure 4 b) and also the ratio between hairpin and bent conformers (bend angle <60° and bend angle ≥60°, <150° respectively) to be determined (Figure 4 c). As with previous work, this demonstrates the importance of the bend angle and the intimate relationship that exists between this and the thermal stability of the NTB mesophase (i.e., the onset temperature),43 and reaffirms the conclusion that materials lacking an overall bent shape (i.e., even parity homologues) cannot exhibit the NTB phase as it is presently understood. It is also apparent that the clearing point does not appear to display such a strong dependence on the bend angle.

Figure 4
How the conformational landscape influences the twist–bend nematic mesophase: a) Top: the AM1 minimised all‐trans form of compound 7 with arrows showing the bonds allowed to undergo threefold rotation during the conformer search ...

The twist–bend nematic phase as exhibited by liquid‐crystalline dimers is seemingly fairly well understood in terms of the molecular factors that govern the incidence of this phase, and so our attention now turns to oligomeric materials that exhibit this mesophase. Jansze et al. reported in 2014 on a novel hydrogen‐bonded liquid‐crystalline trimer that also exhibited the twist–bend nematic phase (Figure 5 a).32 This material, known as 4‐[6‐(4′‐cyanobiphenyl‐4‐yl)hexyloxy]benzoic acid (CB6OBA), has an odd‐parity spacer unit—the homologous even‐parity material (CB5OBA) does not exhibit the NTB phase, mirroring trends seen for dimers and bimesogens. Shortly after this Wang et al. reported a hybrid calamitic/bent–core trimer that exhibited the NTB phase.47 This material, shown in Figure 5 b, with two cyanobiphenyl mesogenic units appended to a central resorcinol derived bent–core type mesogenic unit. In 2016 a methylene‐linked tetramer (T49 or RM1697, Figure 5 d) was reported by us; this material exhibits enantiotropic nematic and twist–bend nematic mesophases,48 as does the related linear trimer T39 (RM1698, Figure 5 c).49 Both T39 and T49 can be prepared in the same manner; an intermediate with one complete mesogenic unit and one half‐complete mesogenic unit bearing a phenol is esterified with an appropriate dicarboxylic acid to yield a trimer/tetramer.

Figure 5
Oligomeric twist–bend nematogens known in the literature as of late 2016: a) the hydrogen bonded trimer CB6OCB;32 b) Wang's timer, note that a melting point was not reported;47 c) the trimer T39;49 d) the tetramer ...

It had been hypothesised that higher oligomers should exhibit the twist–bend nematic phase,48, 49 and whereas dimers, trimers and tetramers are readily accessible the synthesis of higher methylene‐linked oligomers has not been reported. We therefore devised a synthetic approach (Figure 6) to these materials that relies on an intermediate containing two half‐complete mesogenic units (4‐hydroxyphenyl and benzyl 4‐carboxyphenyl benzoate) separated by a spacer, in this case heptamethylene.50 Esterification of the free phenol with a suitable carboxylic acid followed by debenzylation by means of hydrogenolysis yields another carboxylic acid; this is then free to be esterified with another portion of the phenol/masked‐acid intermediate, extending the length of the molecule in a stepwise manner, providing essentially monodisperse oligomeric materials. To date we have used this approach to prepare a linear tetramer (O47) and a linear hexamer (O67), both of which exhibit the twist–bend nematic mesophase (Figure 6). Assuming threefold rotation—a simplification in itself—about each methylene unit the number of conformers of each oligomer is large enough to make study of the conformational landscape of these materials in their entirety (as opposed to truncated forms) challenging. While an abundance of liquid‐crystalline trimers and tetramers are known in the literature, higher oligomers are something of a rarity. It is believed that with refinement (and possibly automation) of the stepwise “n+1” approach we can prepare linear “oligomeric” materials of almost any length with a polydispersity approaching unity. However, as with polymers, there will exist some length scale at which globular shapes dominate over linear forms, and beyond this point the NTB phase may not be observed.

Figure 6
Oligomeric twist–bend nematogens: a) truncated synthetic route to O47 and O67, with the transition temperatures of related dimer given alongside the two oligomers;50 b) comparison of the all‐trans geometries and end‐to‐end ...

Liquid‐crystalline dimers and oligomers have long been considered as effective model compounds for semi‐flexible main‐chain liquid‐crystal polymers.51 It is therefore logical to postulate as to the existence of polymeric materials that exhibit the twist–bend nematic, as well as other modulated nematic phases exhibited by low‐molecular‐weight dimers. Long before the twist–bend nematic phase was topical, a series of methylene‐linked main‐chain polymers (Figure 7 a) were found to exhibit a nematic‐to‐nematic phase transition.52 After some speculation,1 subsequent reinvestigation of these materials indicates that the lower temperature nematic phase, denoted as N2 in the original paper, is in fact the twist–bend nematic phase.53

Figure 7
The NTB phase on length scales beyond the molecule: a) molecular structures of copolymers (n=5, 7 or 9) reported by Ungar et al. that exhibit nematic to nematic transitions (denoted as N–N2 in the original paper). b), c) Polarised ...

Barry et al. reported a first‐order phase transition driven by entropy in suspensions of helical flagella from an isotropic liquid into a liquid‐crystalline state with novel chiral symmetry (Figure 7).54 It was also demonstrated that achiral rods (in this case non‐helical flagella) do not show this phase, but rather exhibit a simple nematic. The optical textures are shown in Figure 7 and consist of a striped pattern with alternating light and dark regions, these correspond to differing director orientations. As shown in Figure 7 c, fluorescent labelling of flagella reveals that they are always in phase with one another and despite the lack of positional order there is long‐range “phase” ordering.54 It was proposed that the formation of this conical phase—as opposed to a simple nematic or chiral nematicphase—is driven by simple packing (steric) constraints; the excluded volume between two helices being significantly larger when they are out‐of‐phase with respect to one another (Figure 7 e, left) than when they are in phase (Figure 7 e, right) and so minimisation of the excluded volume dictates a preference for in‐phase packing leading to the emergence of the conical mesophase. Parallels exist between this lyotropic phase and the NTB phase not only in terms of their shape‐driven origins, but also their properties. Helical flagella were observed to diffuse along the helical axis in a manner akin to a “nut on a bolt” with diffusion being significantly faster parallel to this axis with respect to perpendicular diffusion. Recent 2H NMR diffusiometry experiments have demonstrated similar anisotropic diffusion in the twist–bend nematic phase of CB7CB.55

Summary and Outlook

In an achiral material the spontaneous breaking of mirror symmetry leads to domains of the NTB phase of opposite handedness. By adding a small percentage of a chiral agent (< wt %) macroscopic (>200 μm2) domains of single handedness can be obtained, and these could be exploited through templating to give three‐dimensional nanostructured materials.56, 57 When used as a reaction solvent the twist–bend nematic phase may also present a more efficient method of chirality transfer than that afforded by conventional chiral liquid‐crystalline phases due to the short helical pitch, manifesting as a long chiral correlation length. Relative to dimers, there are relatively few examples of oligomeric materials known to exhibit the twist–bend nematic phase and this appears to be a logical direction for future research. Lastly we speculate, as others have done,1 that the entropy‐driven first‐order “conical nematic” phase exhibited by flagella may be a lyotropic analogue of the twist–bend nematic phase.

The molecular factors underpinning the twist–bend nematic phase in liquid‐crystalline dimers and bimesogens are now largely understood. The discovery of a linear relationship between T NTB–N and T N–Iso taken in conjunction with experimental demonstration of the importance of bend angle demonstrates that this mesophase is driven by gross shape, the minimisation of free or excluded volume and entropy. It may be possible to exploit the NTB phase in display devices—provided that the difficulty in obtaining suitable alignment is overcome—and there are reports of fast electrooptic response for some materials, which occur near to the N→NTB phase transition.29 Twist–bend nematic materials have been demonstrated to exhibit switchable reflection of light and this may find some applications.58, 59 Manipulation of the striped optical texture of the planar aligned NTB phase has been demonstrated to be possible using applied AC fields, and this may find use in spatial light modulation.60

Conflict of interest

The author declares no conflict of interest.

Acknowledgements

I thank Professor John W. Goodby FRS for interesting discussions concerning the NTB phase as well as for proof reading this manuscript. I thank the University of York for funding research placements for both Matthew Stevens and Frank Simpson. The work undertaken by Matthew and Frank on twist–bend nematic LC oligomers stimulated the writing of this concept article, and for that I am extremely grateful to them both for their efforts.

Notes

R. J. Mandle, Chem. Eur. J. 2017, 23, 8771.

References

1. Borshch V., Kim Y. K., Xiang J., Gao M., Jakli A., Panov V. P., Vij J. K., Imrie C. T., Tamba M. G., Mehl G. H., Lavrentovich O. D., Nat. Commun. 2013, 4, 2635. [PubMed]
2. Dozov I., Europhys. Lett. 2001, 56, 247–253.
3. S. M. Shamid, D. W. Allender, J. V. Selinger, arXiv:1405.5584 [cond-mat.soft], 2014.
4. Trojanowski K., Cieśla M., Longa L., Liq. Cryst. 2016, 44, 273–283.
5. Kolli H. B., Frezza E., Cinacchi G., Ferrarini A., Giacometti A., Hudson T. S., De Michele C., Sciortino F., Soft Matter 2014, 10, 8171–8187. [PubMed]
6. Kolli H. B., Frezza E., Cinacchi G., Ferrarini A., Giacometti A., Hudson T. S., J. Chem. Phys. 2014, 140. [PubMed]
7. Chen D., Porada J. H., Hooper J. B., Klittnick A., Shen Y., Tuchband M. R., Korblova E., Bedrov D., Walba D. M., Glaser M. A., Maclennan J. E., Clark N. A., Proc. Natl. Acad. Sci. USA 2013, 110, 15931–15936. [PubMed]
8. Chen D., Nakata M., Shao R., Tuchband M. R., Shuai M., Baumeister U., Weissflog W., Walba D. M., Glaser M. A., Maclennan J. E., Clark N. A., Phys. Rev. E 2014, 89, 022506. [PubMed]
9. Zhu C., Tuchband M. R., Young A., Shuai M., Scarbrough A., Walba D. M., Maclennan J. E., Wang C., Hexemer A., Clark N. A., Phys. Rev. Lett. 2016, 116, 147803. [PubMed]
10. W. D. Stevenson, Z. Ahmed, X. B. Zeng, C. Welch, G. Ungar, G. H. Mehl, arXiv: 1612.01180 [cond-mat.soft], 2016.
11. Beguin L., Emsley J. W., Lelli M., Lesage A., Luckhurst G. R., Timimi B. A., Zimmermann H., J. Phys. Chem. B 2012, 116, 10407–10407.
12. Gorecka E., Salamonczyk M., Zep A., Pociecha D., Welch C., Ahmed Z., Mehl G. H., Liq. Cryst. 2015, 42, 1–7.
13. Hoffmann A., Vanakaras A. G., Kohlmeier A., Mehl G. H., Photinos D. J., Soft Matter 2015, 11, 850–855. [PubMed]
14. Longa L., Pajak G., Phys. Rev. E 2016, 93, 040701. [PubMed]
15. Beguin L., Emsley J. W., Lelli M., Lesage A., Luckhurst G. R., Timimi B. A., Zimmermann H., J. Phys. Chem. B 2012, 116, 7940–7951. [PubMed]
16. Mandle R. J., Davis E. J., Archbold C. T., Cowling S. J., Goodby J. W., J. Mater. Chem. C 2014, 2, 556–566.
17. Zhang Z. P., Panov V. P., Nagaraj M., Mandle R. J., Goodby J. W., Luckhurst G. R., Jones J. C., Gleeson H. F., J. Mater. Chem. C 2015, 3, 10007–10016.
18. Archbold C. T., Davis E. J., Mandle R. J., Cowling S. J., Goodby J. W., Soft Matter 2015, 11, 7547–7557. [PubMed]
19. Emsley J. W., Lelli M., Lesage A., Luckhurst G. R., J. Phys. Chem. B 2013, 117, 6547–6557. [PubMed]
20. Gaussian 09, Revision e01, M. J. Frisch, G. W. Trucks, H. B. Schlegel, G. E. Scuseria, M. A. Robb, J. R. Cheeseman, G. Scalmani, V. Barone, B. Mennucci, G. A. Petersson, H. Nakatsuji, M. Caricato, X. Li, H. P. Hratchian, A. F. Izmaylov, J. Bloino, G. Zheng, J. L. Sonnenberg, M. Hada, M. Ehara, K. Toyota, R. Fukuda, J. Hasegawa, M. Ishida, T. Nakajima, Y. Honda, O. Kitao, H. Nakai, T. Vreven, J. A. Montgomery, Jr., J. E. Peralta, F. Ogliaro, M. J. Bearpark, J. Heyd, E. N. Brothers, K. N. Kudin, V. N. Staroverov, R. Kobayashi, J. Normand, K. Raghavachari, A. P. Rendell, J. C. Burant, S. S. Iyengar, J. Tomasi, M. Cossi, N. Rega, N. J. Millam, M. Klene, J. E. Knox, J. B. Cross, V. Bakken, C. Adamo, J. Jaramillo, R. Gomperts, R. E. Stratmann, O. Yazyev, A. J. Austin, R. Cammi, C. Pomelli, J. W. Ochterski, R. L. Martin, K. Morokuma, V. G. Zakrzewski, G. A. Voth, P. Salvador, J. J. Dannenberg, S. Dapprich, A. D. Daniels, Ö. Farkas, J. B. Foresman, J. V. Ortiz, J. Cioslowski, D. J. Fox, Gaussian, Inc., Wallingford CT, 2009.
21. Cestari M., Diez-Berart S., Dunmur D. A., Ferrarini A., de la Fuente M. R., Jackson D. J., Lopez D. O., Luckhurst G. R., Perez-Jubindo M. A., Richardson R. M., Salud J., Timimi B. A., Zimmermann H., Phys. Rev. E 2011, 84, 031704. [PubMed]
22. Panov V. P., Nagaraj M., Vij J. K., Panarin Y. P., Kohlmeier A., Tamba M. G., Lewis R. A., Mehl G. H., Phys. Rev. Lett. 2010, 105, 167801. [PubMed]
23. Mandle R. J., Davis E. J., Lobato S. A., Vol C. C., Cowling S. J., Goodby J. W., Phys. Chem. Chem. Phys. 2014, 16, 6907–6915. [PubMed]
24. Mandle R. J., Voll C. C. A., Lewis D. J., Goodby J. W., Liq. Cryst. 2016, 43, 13–21.
25. Ivsic T., Vinkovic M., Baumeister U., Mikleusevic A., Lesac A., RSC Adv. 2016, 6, 5000–5007.
26. Ivšić T., Baumeister U., Dokli I., Mikleušević A., Lesac A., Liq. Cryst. 2016, 44, 93–105.
27. Mandle R. J., Soft Matter 2016, 12, 7883–7901. [PubMed]
28. Ahmed Z., Welch C., Mehl G. H., RSC Adv. 2015, 5, 93513–93521.
29. Panov V. P., Balachandran R., Nagaraj M., Vij J. K., Tamba M. G., Kohlmeier A., Mehl G. H., Appl. Phys. Lett. 2011, 99, 261903.
30. Mandle R. J., Davis E. J., Archbold C. T., Voll C. C., Andrews J. L., Cowling S. J., Goodby J. W., Chem. Eur. J. 2015, 21, 8158–8167. [PubMed]
31. Paterson D. A., Abberley J. P., Harrison W. T. A., Storey J. M. D., Imrie C. T., Liq. Cryst. 2017, 44, 127–146.
32. Jansze S. M., Martinez-Felipe A., Storey J. M., Marcelis A. T., Imrie C. T., Angew. Chem. Int. Ed. 2015, 54, 643–646; [PubMed] Angew. Chem. 2015, 127, 653–656.
33. Mandle R. J., Goodby J. W., Chem. Eur. J. 2016, 22, 18456–18464. [PubMed]
34. Mandle R. J., Davis E. J., Voll C. C. A., Archbold C. T., Goodby J. W., Cowling S. J., Liq. Cryst. 2015, 42, 688–703.
35. Greco C., Luckhurst G. R., Ferrarini A., Soft Matter 2014, 10, 9318–9323. [PubMed]
36. Vaupotic N., Curk S., Osipov M. A., Cepic M., Takezoe H., Gorecka E., Phys. Rev. E 2016, 93, 022704. [PubMed]
37. Greco C., Ferrarini A., Phys. Rev. Lett. 2015, 115, 147801. [PubMed]
38. M. R. Tuchband, M. Shuai, K. A. Graber, D. Chen, L. Radzihovsky, A. Klittnick, L. Foley, A. Scarbrough, J. H. Porada, M. Moran, E. Korblova, D. M. Walba, M. A. Glaser, J. E. Maclennan, N. A. Clark, arXiv:1511.07523 [cond-mat.soft], 2015.
39. M. R. Tuchband, M. Shuai, K. A. Graber, D. Chen, C. Zhu, L. Radzihovsky, A. Klittnick, L. M. Foley, A. Scarbrough, J. H. Porada, M. Moran, J. Yelk, D. Bedrov, E. Korblova, D. M. Walba, A. Hexemer, J. E. Maclennan, M. A. Glaser, N. A. Clark, arXiv:1703.10787 [cond-mat.soft], 2017.
40. Dawood A. A., Grossel M. C., Luckhurst G. R., Richardson R. M., Timimi B. A., Wells N. J., Yousif Y. Z., Liq. Cryst. 2016, 43, 2–12.
41. Paterson D. A., Xiang J., Singh G., Walker R., Agra-Kooijman D. M., Martinez-Felipe A., Gan M., Storey J. M. D., Kumar S., Lavrentovich O. D., Imrie C. T., J. Am. Chem. Soc. 2016, 138, 5283–5289. [PubMed]
42. Ref. [35].
43. Mandle R. J., Archbold C. T., Sarju J. P., Andrews J. L., Goodby J. W., Sci. Rep. 2016, 6, 36682. [PubMed]
44. Sebastián N., Lopez D. O., Robles-Hernandez B., de la Fuente M. R., Salud J., Perez-Jubindo M. A., Dunmur D. A., Luckhurst G. R., Jackson D. J., Phys Chem. Chem. Phys. 2014, 16, 21391–21406. [PubMed]
45. C. T. Archbold, R. J. Mandle, J. L. Andrews, S. J. Cowling, J. W. Goodby, unpublished results.
46. Paterson D. A., Gao M., Kim Y. K., Jamali A., Finley K. L., Robles-Hernandez B., Diez-Berart S., Salud J., de la Fuente M. R., Timimi B. A., Zimmermann H., Greco C., Ferrarini A., Storey J. M. D., Lopez D. O., Lavrentovich O. D., Luckhurst G. R., Imrie C. T., Soft Matter 2016, 12, 6827–6840. [PubMed]
47. Wang Y., Singh G., Agra-Kooijman D. M., Gao M., Bisoyi H. K., Xue C. M., Fisch M. R., Kumar S., Li Q., CrystEngComm 2015, 17, 2778–2782.
48. Mandle R. J., Goodby J. W., ChemPhysChem 2016, 17, 967–970. [PubMed]
49. Mandle R. J., Goodby J. W., RSC Adv. 2016, 6, 34885–34893.
50. F. P. Simpson, R. J. Mandle, J. W. Goodby, J. N. Moore, J. Mater. Chem. C 2017, 10.1039/c7tc00516d.
51. Luckhurst G. R., Macromol. Symp. 1995, 96, 1–26.
52. Ungar G., Percec V., Zuber M., Macromolecules 1992, 25, 75–80.
53. J. An, W. Stevenson, M. Xie, Y. Liu, X. Zeng, G. Ungar, presented in part at the Twist–Bend Nematics and Beyond Conference, University of Southampton, 2016.
54. Barry E., Hensel Z., Dogic Z., Shribak M., Oldenbourg R., Phys. Rev. Lett. 2006, 96, 018305. [PubMed]
55. Cifelli M., Domenici V., Dvinskikh S. V., Luckhurst G. R., Timimi B. A., Liq. Cryst. 2017, 44, 204.
56. Wang L., Li Q., Adv. Funct. Mater. 2016, 26, 10–28.
57. Zheng Z.-g., Li Y., Bisoyi H. K., Wang L., Bunning T. J., Li Q., Nature 2016, 531, 352–356. [PubMed]
58. Mathews M., Zola R. S., Yang D.-K., Li Q., J. Mater. Chem. 2011, 21, 2098–2103.
59. Wang Y., Zheng Z.-g., Bisoyi H. K., Gutierrez-Cuevas K. G., Wang L., Zola R. S., Li Q., Mater. Horiz. 2016, 3, 442–446.
60. Panov V. P., Balachandran R., Vij J. K., Tamba M. G., Kohlmeier A., Mehl G. H., Appl. Phys. Lett. 2012, 101, 234106.

Articles from Wiley-Blackwell Online Open are provided here courtesy of Wiley-Blackwell, John Wiley & Sons