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dc.contributor.authorZappone, Bruno
dc.contributor.authorMamuk, Atilla Eren
dc.contributor.authorGryn, Iryna
dc.contributor.authorArima, Valentina
dc.contributor.authorZizzari, Alessandra
dc.contributor.authorBartolino, Roberto
dc.contributor.authorPetschek, Rolfe
dc.date.accessioned2020-11-20T14:39:22Z
dc.date.available2020-11-20T14:39:22Z
dc.date.issued2020
dc.identifier.issn0027-8424
dc.identifier.urihttps://doi.org/10.1073/pnas.2000849117
dc.identifier.urihttps://hdl.handle.net/20.500.12809/394
dc.descriptionMamuk, Atilla Eren/0000-0002-1524-3342; Kasianiuk, Iryna/0000-0002-8448-5433en_US
dc.descriptionWOS: 000555848400008en_US
dc.descriptionPubMed ID: 32661146en_US
dc.description.abstractSpontaneous breaking of symmetry in liquid crystal (LC) films often reveals itself as a microscopic pattern of molecular align-ment. In a smectic-A LC, the emergence of positional order at the transition from the nematic phase leads to periodic textures that can be used as optical microarrays, templates for soft lithography, and ordering matrices for the organization and manipulation of functional nanoparticles. While both 1d and 2d patterns have been obtained as a function of the LC film thickness and applied fields, the connection has not been made between pattern formation and the peculiar critical behavior of LCs at the nematic-smectic transition, still eluding a comprehensive theoretical explanation. In this article, we demonstrate that an intense bend distortion applied to the LC molecular director while cooling from the ne-matic phase produces a frustrated smectic phase with depressed transition temperature, and the characteristic 1d periodic texture previously observed in thin films and under applied electric fields. In light of De Gennes' analogy with the normal-superconductor transition of a metal, we identify the 1d texture as the equivalent of the intermediate state in type I superconductors. The bend dis-tortion is analog to the magnetic field in metals and penetrates in the frustrated phase as an array of undercooled nematic domains, periodically intermixed with bend-free smectic-A domains. Our findings provide fundamental evidence for theories of the nematic-smectic transition, highlighting the deep connection be-tween phase frustration and pattern formation, and perspectives on the design of functional smectic microarrays.en_US
dc.description.sponsorshipScientific and Technical Research Council of Turkey-International Doctoral Research Fellowship Programme 2214/Aen_US
dc.description.sponsorshipWe are grateful to Charles Rosenblatt at Case Western Reserve University for his comments and suggestions. We thank Roberto Termine of Consiglio Nazionale delle Ricerche, Istituto di Nanotecnologia, for his help with the stylus profilometer. A.E.M. also acknowledges the support of the Scientific and Technical Research Council of Turkey-International Doctoral Research Fellowship Programme 2214/A.en_US
dc.item-language.isoengen_US
dc.publisherNatl Acad Sciencesen_US
dc.item-rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectLiquid Crystalsen_US
dc.subjectSuperconductorsen_US
dc.subjectPhase Transitionsen_US
dc.subjectPattern Formationen_US
dc.subjectPhase Frustrationen_US
dc.titleAnalogy between periodic patterns in thin smectic liquid crystal films and the intermediate state of superconductorsen_US
dc.item-typearticleen_US
dc.contributor.departmentMÜ, Fen Fakültesi, Fizik Bölümüen_US
dc.contributor.institutionauthorMamuk, Atilla Eren
dc.identifier.doi10.1073/pnas.2000849117
dc.identifier.volume117en_US
dc.identifier.issue30en_US
dc.identifier.startpage17643en_US
dc.identifier.endpage17649en_US
dc.relation.journalProceedings of the National Academy of Sciences of the United States of Americaen_US
dc.relation.publicationcategoryMakale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanıen_US


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