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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://dk.um.si/IzpisGradiva.php?id=87754"><dc:title>Reconfiguration of nematic disclinations in plane-parallel confinements</dc:title><dc:creator>Harkai,	Saša	(Avtor)
	</dc:creator><dc:creator>Rosenblatt,	Charles	(Avtor)
	</dc:creator><dc:creator>Kralj,	Samo	(Avtor)
	</dc:creator><dc:subject>liquid crystals</dc:subject><dc:subject>topological defects</dc:subject><dc:subject>disclinations</dc:subject><dc:subject>reconfiguration</dc:subject><dc:description>We study numerically the reconfiguration process of colliding |m|=1/2 strength disclinations in an achiral nematic liquid crystal (NLC). A Landau–de Gennes approach in terms of tensor nematic-order parameters is used. Initially, different pairs {m1,m2} of parallel wedge disclination lines connecting opposite substrates confining the NLC in a plane-parallel cell of a thickness h are imposed: {1/2,1/2}, {−1/2,−1/2} and {−1/2,1/2}. The collisions are imposed by the relative rotation of the azimuthal angle θ of the substrates that strongly pin the defect end points. Pairs {1/2,1/2} and {−1/2,−1/2} “rewire” at the critical angle θ(1)c=3π/4 in all cases studied. On the other hand, two qualitatively different scenarios are observed for {−1/2,1/2}. In the thinner film regime ℎ&lt;ℎc, the disclinations rewire at θ(2)c=5π/4. The rewiring process is mediated by an additional chargeless loop nucleated in the middle of the cell. In the regime ℎ&gt;ℎc, the colliding disclinations at θ(2)c reconfigure into boojum-like twist disclinations.</dc:description><dc:publisher>MDPI</dc:publisher><dc:date>2023</dc:date><dc:date>2024-03-28 08:15:08</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>87754</dc:identifier><dc:language>sl</dc:language></rdf:Description></rdf:RDF>
