Editing Liquid crystal (section)

==Effect of chirality==
As already described, [[chirality (chemistry)|chiral]] liquid-crystal molecules usually give rise to chiral mesophases. This means that the molecule must possess some form of asymmetry, usually a [[stereogenic]] center. An additional requirement is that the system not be [[racemic]]: a mixture of right- and left-handed molecules will cancel the chiral effect. Due to the cooperative nature of liquid crystal ordering, however, a small amount of chiral dopant in an otherwise achiral mesophase is often enough to select out one domain handedness, making the system overall chiral.

Chiral phases usually have a helical twisting of the molecules. If the pitch of this twist is on the order of the wavelength of visible light, then interesting optical interference effects can be observed. The chiral twisting that occurs in chiral LC phases also makes the system respond differently from right- and left-handed circularly polarized light. These materials can thus be used as [[polarizer|polarization filters]].<ref>{{cite journal| title = Video camera system using liquid-crystal polarizing filter toreduce reflected light| doi =10.1109/11.735903|journal=IEEE Transactions on Broadcasting|volume = 44| issue =4|date = 1998| page = 419| vauthors = Fujikake H, Takizawa K, Aida T, Negishi T, Kobayashi M }}</ref>

It is possible for chiral LC molecules to produce essentially achiral mesophases. For instance, in certain ranges of concentration and [[molecular weight]], DNA will form an achiral line hexatic phase. An interesting recent observation is of the formation of chiral mesophases from achiral LC molecules. Specifically, bent-core molecules (sometimes called banana liquid crystals) have been shown to form liquid crystal phases that are chiral.<ref>{{cite journal | vauthors = Achard MF, Bedel JP, Marcerou JP, Nguyen HT, Rouillon JC | s2cid = 35942754 | title = Switching of banana liquid crystal mesophases under field | journal = The European Physical Journal E | volume = 10 | issue = 2 | pages = 129–34 | date = February 2003 | pmid = 15011066 | doi = 10.1140/epje/e2003-00016-y | bibcode = 2003EPJE...10..129A }}</ref> In any particular sample, various domains will have opposite handedness, but within any given domain, strong chiral ordering will be present. The appearance mechanism of this macroscopic chirality is not yet entirely clear. It appears that the molecules stack in layers and orient themselves in a tilted fashion inside the layers. These liquid crystals phases may be [[ferroelectric]] or anti-ferroelectric, both of which are of interest for applications.<ref>{{cite journal | vauthors = Baus M, Colot JL | title = Ferroelectric nematic liquid-crystal phases of dipolar hard ellipsoids | journal = Physical Review A | volume = 40 | issue = 9 | pages = 5444–5446 | date = November 1989 | pmid = 9902823 | doi = 10.1103/PhysRevA.40.5444 | bibcode = 1989PhRvA..40.5444B | url = https://dipot.ulb.ac.be/dspace/bitstream/2013/39767/4/02137fa4-0709-490a-b691-101e483af30c.txt | access-date = March 4, 2021 | archive-date = April 27, 2021 | archive-url = https://web.archive.org/web/20210427211925/https://dipot.ulb.ac.be/dspace/bitstream/2013/39767/4/02137fa4-0709-490a-b691-101e483af30c.txt | url-status = live }}</ref><ref>{{cite journal| title = Pressure-Temperature Phase Diagrams of Ferroelectric Liquid Crystals|journal=J. Phys. Soc. Jpn.|volume = 71|date = 2002| issue =2| page = 509| doi =10.1143/JPSJ.71.509|bibcode = 2002JPSJ...71..509U| last1 = Uehara| first1 = Hiroyuki| last2 = Hatano| first2 = Jun | name-list-style = vanc }}</ref>

Chirality can also be incorporated into a phase by adding a chiral [[dopant]], which may not form LCs itself. [[Twisted nematic field effect|Twisted-nematic]] or [[Super-twisted nematic display|super-twisted nematic]] mixtures often contain a small amount of such dopants.