Fluctuation Modes of a Bent-Core Nematic Liquid Crystal

ORAL

Abstract

We present a dynamic light scattering study of the bent-core nematic liquid crystal compound \textit{DT6Py6E6.} We utilize a ``dark'' scattering geometry, which allows us to search for fluctuation modes that are not purely associated with the uniaxial director. Indeed, we observe two modes (hydrodynamic and non-hydrodynamic) in addition to the expected twist-bend director mode. We present a model for the additional modes based on fluctuations of the biaxial order parameter, which leads to an estimate of 10-100 nm for the correlation length associated with these fluctuations.

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Authors

  • Madhabi Majumdar

    Physics Department, Kent State University

  • Carla Benton

    Fratii Buzesti College, Craiova, Romania, Cleveland State University, University of Gothenburg, Sweden, Case Western Reserve University, HISKP Universitaet Bonn, IKP-3 Forschungszentrum Juelich, IAS-4 Forschungszentrum Juelich, Ruhr-Universitaet Bochum, IUPUI, Miami University, Physics Department, Kent State University, LCI, Kent State University, National High Magnetic Field Lab, Brookhaven National Laboratory, University of Wisconsin Oshkosh, The University of Akron

  • Carla Benton

    Fratii Buzesti College, Craiova, Romania, Cleveland State University, University of Gothenburg, Sweden, Case Western Reserve University, HISKP Universitaet Bonn, IKP-3 Forschungszentrum Juelich, IAS-4 Forschungszentrum Juelich, Ruhr-Universitaet Bochum, IUPUI, Miami University, Physics Department, Kent State University, LCI, Kent State University, National High Magnetic Field Lab, Brookhaven National Laboratory, University of Wisconsin Oshkosh, The University of Akron

  • Carla Benton

    Fratii Buzesti College, Craiova, Romania, Cleveland State University, University of Gothenburg, Sweden, Case Western Reserve University, HISKP Universitaet Bonn, IKP-3 Forschungszentrum Juelich, IAS-4 Forschungszentrum Juelich, Ruhr-Universitaet Bochum, IUPUI, Miami University, Physics Department, Kent State University, LCI, Kent State University, National High Magnetic Field Lab, Brookhaven National Laboratory, University of Wisconsin Oshkosh, The University of Akron

  • Carla Benton

    Fratii Buzesti College, Craiova, Romania, Cleveland State University, University of Gothenburg, Sweden, Case Western Reserve University, HISKP Universitaet Bonn, IKP-3 Forschungszentrum Juelich, IAS-4 Forschungszentrum Juelich, Ruhr-Universitaet Bochum, IUPUI, Miami University, Physics Department, Kent State University, LCI, Kent State University, National High Magnetic Field Lab, Brookhaven National Laboratory, University of Wisconsin Oshkosh, The University of Akron

  • Carla Benton

    Fratii Buzesti College, Craiova, Romania, Cleveland State University, University of Gothenburg, Sweden, Case Western Reserve University, HISKP Universitaet Bonn, IKP-3 Forschungszentrum Juelich, IAS-4 Forschungszentrum Juelich, Ruhr-Universitaet Bochum, IUPUI, Miami University, Physics Department, Kent State University, LCI, Kent State University, National High Magnetic Field Lab, Brookhaven National Laboratory, University of Wisconsin Oshkosh, The University of Akron