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<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/"><rdf:Description rdf:about="https://repozitorij.uni-lj.si/IzpisGradiva.php?id=156067"><dc:title>Three-dimensional spontaneous flow transition in a homeotropic active nematic</dc:title><dc:creator>Pratley,	Vincenzo J.	(Avtor)
	</dc:creator><dc:creator>Caf,	Enej	(Avtor)
	</dc:creator><dc:creator>Ravnik,	Miha	(Avtor)
	</dc:creator><dc:creator>Alexander,	Gareth P.	(Avtor)
	</dc:creator><dc:subject>nematic fluids</dc:subject><dc:subject>active nematics</dc:subject><dc:description>Active nematics are driven, non-equilibrium systems relevant to biological processes including tissue mechanics and morphogenesis, and to active metamaterials in general. We study the three-dimensional spontaneous flow transition of an active nematic in an infinite slab geometry using a combination of numerics and analytics. We show that it is determined by the interplay of two eigenmodes – called S- and D-mode – that are unstable at the same activity threshold and spontaneously breaks both rotational symmetry and chiral symmetry. The onset of the unstable modes is described by a non-Hermitian integro-differential operator, which we determine their exponential growth rates from using perturbation theory. The S-mode is the fastest growing. After it reaches a finite amplitude, the growth of the D-mode is anisotropic, being promoted perpendicular to the S-mode and suppressed parallel to it, forming a steady state with a full three-dimensional director field and a well-defined chirality. Lastly, we derive a model of the leading-order time evolution of the system close to the activity threshold.</dc:description><dc:date>2024</dc:date><dc:date>2024-05-07 12:48:01</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>156067</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
