<HashMap><database>biostudies-literature</database><scores/><additional><submitter>Chen X</submitter><funding>National Science Foundation (NSF)</funding><funding>DOE</funding><funding>Colorado Office of Economic Development and International Trade</funding><funding>Colorado Office of Economic Development and International Trade (OEDIT)</funding><funding>National Science Foundation</funding><pagination>e2217150120</pagination><full_dataset_link>https://www.ebi.ac.uk/biostudies/studies/S-EPMC9974471</full_dataset_link><repository>biostudies-literature</repository><omics_type>Unknown</omics_type><volume>120(8)</volume><pubmed_abstract>We have structurally characterized the liquid crystal (LC) phase that can appear as an intermediate state when a dielectric nematic, having polar disorder of its molecular dipoles, transitions to the almost perfectly polar-ordered ferroelectric nematic. This intermediate phase, which fills a 100-y-old void in the taxonomy of smectic LCs and which we term the "smectic Z&lt;sub>A&lt;/sub>," is antiferroelectric, with the nematic director and polarization oriented parallel to smectic layer planes, and the polarization alternating in sign from layer to layer with a 180 Å period. A Landau free energy, originally derived from the Ising model of ferromagnetic ordering of spins in the presence of dipole-dipole interactions, and applied to model incommensurate antiferroelectricity in crystals, describes the key features of the nematic-SmZ&lt;sub>A&lt;/sub>-ferroelectric nematic phase sequence.</pubmed_abstract><journal>Proceedings of the National Academy of Sciences of the United States of America</journal><pubmed_title>The smectic Z&lt;sub>A&lt;/sub> phase: Antiferroelectric smectic order as a prelude to the ferroelectric nematic.</pubmed_title><pmcid>PMC9974471</pmcid><funding_grant_id>1710711</funding_grant_id><funding_grant_id>DE-SC0012704</funding_grant_id><funding_grant_id>2005170</funding_grant_id><funding_grant_id>1420736</funding_grant_id><funding_grant_id>APP-35428</funding_grant_id><pubmed_authors>Korblova E</pubmed_authors><pubmed_authors>Zhernenkov M</pubmed_authors><pubmed_authors>Wang C</pubmed_authors><pubmed_authors>Glaser MA</pubmed_authors><pubmed_authors>Walba DM</pubmed_authors><pubmed_authors>Maclennan JE</pubmed_authors><pubmed_authors>Chen X</pubmed_authors><pubmed_authors>Freychet G</pubmed_authors><pubmed_authors>Radzihovsky L</pubmed_authors><pubmed_authors>Martinez V</pubmed_authors><pubmed_authors>Zhu C</pubmed_authors><pubmed_authors>Clark NA</pubmed_authors></additional><is_claimable>false</is_claimable><name>The smectic Z&lt;sub>A&lt;/sub> phase: Antiferroelectric smectic order as a prelude to the ferroelectric nematic.</name><description>We have structurally characterized the liquid crystal (LC) phase that can appear as an intermediate state when a dielectric nematic, having polar disorder of its molecular dipoles, transitions to the almost perfectly polar-ordered ferroelectric nematic. This intermediate phase, which fills a 100-y-old void in the taxonomy of smectic LCs and which we term the "smectic Z&lt;sub>A&lt;/sub>," is antiferroelectric, with the nematic director and polarization oriented parallel to smectic layer planes, and the polarization alternating in sign from layer to layer with a 180 Å period. A Landau free energy, originally derived from the Ising model of ferromagnetic ordering of spins in the presence of dipole-dipole interactions, and applied to model incommensurate antiferroelectricity in crystals, describes the key features of the nematic-SmZ&lt;sub>A&lt;/sub>-ferroelectric nematic phase sequence.</description><dates><release>2023-01-01T00:00:00Z</release><publication>2023 Feb</publication><modification>2025-04-04T20:04:42.687Z</modification><creation>2025-04-04T20:04:42.687Z</creation></dates><accession>S-EPMC9974471</accession><cross_references><pubmed>36791101</pubmed><doi>10.1073/pnas.2217150120</doi></cross_references></HashMap>