{"id":3616,"date":"2021-10-19T10:08:51","date_gmt":"2021-10-19T08:08:51","guid":{"rendered":"https:\/\/equipes.lps.u-psud.fr\/matrix\/?p=3616"},"modified":"2022-01-24T10:01:11","modified_gmt":"2022-01-24T09:01:11","slug":"a-freedericksz-like-transition-in-a-biaxial-smectic-a-phase","status":"publish","type":"post","link":"https:\/\/equipes.lps.u-psud.fr\/matrix\/a-freedericksz-like-transition-in-a-biaxial-smectic-a-phase\/","title":{"rendered":"A Fr\u00e9edericksz-like transition in a biaxial smectic A phase"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\"><strong>Liquid-crystal (LC) displays exploit a physical phenomenon called the Fr\u00e9edericksz transition. This effect is only observed with \u201cnematic\u201d LCs which are fluids of rod-like molecules aligned in the same direction. The Fr\u00e9edericksz transition consists in the reorientation of this direction by an electric field. There is however another large class of LCs, called \u201csmectics\u201d, where the molecules are not only all aligned but they also form equidistant layers. Smectics do not show the Fr\u00e9edericksz transition because the reorientation would disturb the lamellar structure. Consequently, smectics are not used in display technology up to now.<\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Usual LC molecules have a rod-like cylindrical shape and they are all aligned in the same direction, called the \u201c<strong>n<\/strong>-director\u201d, in the nematic LC phase. Moreover, they also spontaneously form layers in smectic LC phases which can be regarded as 1-dimensional stacks of fluid layers. In search for new display mechanisms, scientists have recently considered exotic molecular shapes, such as banana-like or board-like ones that strongly differ from the usual rod-like cylindrical shape. These molecules are \u201cbiaxial\u201d, meaning that they lack revolution symmetry. Then, they can form biaxial smectics, labelled \u201cSmA<sub>b<\/sub>\u201d, where not only their longest axis is aligned along the <strong>n<\/strong>-director, but also their medium one, along the so-called \u201c<strong>m<\/strong>-director\u201d.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">During the electro-optic investigation of these compounds, an international team coordinated by scientists from Laboratoire de Physique des Solides discovered that the SmA<sub>b<\/sub> phase displays an effect highly reminiscent of the Fr\u00e9edericksz transition of nematics (Figure 1). Using polarized-light microscopy, birefringence and dielectric measurements, they showed that it is a Fr\u00e9edericksz transition affecting the <strong>m<\/strong>-director (Figure 2). This biaxial Fr\u00e9edericksz transition is actually possible in a biaxial smectic because it does not alter the <strong>n<\/strong>-director field and therefore the lamellar structure is preserved. Moreover, they found that the relaxation time of this effect is much shorter than that of the usual Fr\u00e9edericksz transition of nematics, so that the biaxial SmA<sub>b<\/sub> phase could be exploited in electro-optic devices that require fast switching.<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig1.png\" alt=\"\" class=\"wp-image-3617\" width=\"676\" height=\"338\" srcset=\"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig1.png 1000w, https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig1-300x150.png 300w, https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig1-768x384.png 768w\" sizes=\"auto, (max-width: 676px) 100vw, 676px\" \/><\/figure><\/div>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><em>Figure 1.<\/em><\/strong><em> (left) <em>Domains (size \u00bb&nbsp;100&nbsp;\u00b5m) of smectic phase (red) in a nematic cell (orange). (right) When an electric field is applied, the birefringence of the smectic domains changes. This induces a red-to-green transition and the appearance of twin domains separated by walls (black lines).<\/em><\/em> <\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter size-large is-resized\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig2-1024x416.png\" alt=\"\" class=\"wp-image-3618\" width=\"658\" height=\"267\" srcset=\"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig2-1024x416.png 1024w, https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig2-300x122.png 300w, https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig2-768x312.png 768w, https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig2-1536x625.png 1536w, https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-content\/uploads\/sites\/12\/2021\/10\/Fig2.png 1731w\" sizes=\"auto, (max-width: 658px) 100vw, 658px\" \/><\/figure><\/div>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><em>Figure 2.<\/em><\/strong><em> (left) <em>The biaxial LC molecules have a board-like shape, with their longest dimension defining the layer thickness (delimited by the red dotted lines) of the smectic phase. (right) Upon application of an electric field E, the boards rotate, which changes the apparent birefringence of the material, just like the usual Fr\u00e9edericksz transition, but does not affect the smectic layers. (The black (resp. blue) double-headed arrows represent the <\/em><\/em><strong><em>n<\/em><\/strong><em><em>-director (resp. the <\/em><\/em><strong><em>m<\/em><\/strong><em><em>-director).<\/em><\/em> <\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Reference<\/strong><br>Fr\u00e9edericksz-Like Transition in a Biaxial Smectic-A Phase<br>C. Meyer, P. Davidson, D. Constantin, V.i Sergan, D. Stoenescu, A. Kne\u017eevi\u0107, I. Dokli, A. Lesac, I. Dozov<br>Phys. Rev. X, <strong>2021<\/strong>, 11, 031012<br><a rel=\"noreferrer noopener\" href=\"https:\/\/journals.aps.org\/prx\/abstract\/10.1103\/PhysRevX.11.031012\" target=\"_blank\">doi: 10.1103\/PhysRevX.11.031012<\/a><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong>Contacts<\/strong><br><a href=\"mailto:patrick.davidson@universite-paris-saclay.fr\" target=\"_blank\" rel=\"noreferrer noopener\">Patrick Davidson<\/a><br><a href=\"mailto:ivan.dozov@universite-paris-saclay.fr\">Ivan Dozov<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Liquid-crystal (LC) displays exploit a physical phenomenon called the Fr\u00e9edericksz transition. This effect is only observed with \u201cnematic\u201d LCs which are fluids of rod-like molecules aligned in the same direction. &#8230;<\/p>\n","protected":false},"author":25,"featured_media":3619,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[3],"tags":[],"class_list":["post-3616","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-publication"],"_links":{"self":[{"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/posts\/3616","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/users\/25"}],"replies":[{"embeddable":true,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/comments?post=3616"}],"version-history":[{"count":4,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/posts\/3616\/revisions"}],"predecessor-version":[{"id":3704,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/posts\/3616\/revisions\/3704"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/media\/3619"}],"wp:attachment":[{"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/media?parent=3616"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/categories?post=3616"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/equipes.lps.u-psud.fr\/matrix\/wp-json\/wp\/v2\/tags?post=3616"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}