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Competition between helical and heliconical twist in the development of complex soft matter structures

dc.contributor.authorYildiz Ozdemir, Busra
dc.contributor.authorOzkonstanyan, Aykun
dc.contributor.authorAnders, Christian
dc.contributor.authorKaraca Balta, Demet
dc.contributor.authorOcak Gumrukcu, Hale
dc.contributor.authorTschierske, Carsten
dc.contributor.authorAlaasar, Mohamed
dc.date.accessioned2026-06-27T15:25:48Z
dc.date.issued2026
dc.description.abstractChirality strongly influences the self-assembly of soft matter systems, yielding new superstructures with numerous potential applications. Here, two series of 4-cyanoresorcinol-based bent-core liquid crystals (BCLCs) in which molecular chirality is provided by the introduction of a branched (S)-2-alkyloxypropyl end chain at both or only one end of the aromatic core have been synthesized and characterized to study the effects of chain branching and molecular chirality on liquid crystalline (LC) self-assembly. Two new LC phases with tilted and twisted arrangements of the molecules, restricted rotation around the long axis, preferred face-to-face stacking of the polyaromatic cores, and only a short correlation length of lamellar ordering were discovered; one is achiral and isotropic (MIso) while the other is chiral and low birefringent (ML*). With decreasing density of the chain branching (i.e., stereogenic centers), the achiral MIso phase is replaced by the birefringent heliconical ML* phase, an amorphous type III blue phase (BPIII), a heliconical tilted smectic phase (SmC*), and a chiral cybotactic nematic phase composed of SmC* clusters (NCybC*). In this NCybC* phase, the twist is heliconical, in contrast to the conventional non-cybotactic chiral nematics where it is helical. The heliconical twist is favored and the helical twist is suppressed by the emergence and growth of SmC-type cybotactic clusters. At the transition to a denser, face-to-face-packed core, saddle-splay emerges, and helical twist can become stronger, supporting layer deformation and causing a transition from the heliconical SmC* via ML* to the achiral MIso phase as the density of chain-branched stereogenic centers increases and temperature decreases.en
dc.description.sponsorshipTUBITAK International Cooperation Projects Research Support Group [221N431]
dc.description.sponsorshipDeutsche Forschungsgemeinschaft (DFG) [AL2378/1-2, 424355983, 436494874 - GRK 2670]
dc.description.sponsorshipAlexander von Humboldt Foundation at Martin Luther University, Halle, Germany
dc.description.urihttps://doi.org/10.1039/d5tc03348a
dc.identifier.doi10.1039/d5tc03348a
dc.identifier.eissn2050-7534
dc.identifier.endpage1276
dc.identifier.issn2050-7526
dc.identifier.issue3
dc.identifier.startpage1260
dc.identifier.urihttps://hdl.handle.net/20.500.14981/70883
dc.identifier.volume14
dc.identifier.wos001623143800001
dc.language.isoeng
dc.publisherROYAL SOC CHEMISTRY
dc.relation.ispartofJOURNAL OF MATERIALS CHEMISTRY C
dc.rightsopenAccess
dc.subjectLIQUID-CRYSTALLINE PHASE
dc.subjectBENT-CORE MESOGENS
dc.subjectMIRROR SYMMETRY-BREAKING
dc.subjectPOLAR ORDER
dc.subjectDARK CONGLOMERATE
dc.subjectBLUE-PHASE
dc.subjectCHIRALITY SYNCHRONIZATION
dc.subjectSMECTIC PHASE
dc.subjectROD-LIKE
dc.subjectMOLECULES
dc.subjectMaterials Science
dc.subjectPhysics
dc.titleCompetition between helical and heliconical twist in the development of complex soft matter structures
dc.typeArticle
dspace.entity.typePublication
local.import.sourceWOS

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