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Anyons, Zitterbewegung and dynamical phase transitions in topologically nontrivial systems
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Nontrivial topology in physical systems is the driving force behind many phenomena. Notably, phases of matter must be classified in part by their topological properties. Phases with topological order (TO), such as the fractional quantum Hall effect (QHE), can support anyonic excitations obeying fractional statistics with potential application in topological quantum computing. States lacking intrinsic TO can still be in topological phases provided certain symmetries are imposed. On their own, these symmetry-protected phases do not support anyons, but they can still have other interesting features, such as protected boundary states. In this thesis we present our research into several nontrivial systems. First, we present the results on light propagation in the valley modes of inversion-symmetry broken honeycomb lattices. We find that a rotating spiral pattern, leading to Zitterbewegung, arises in the intensity profile of the beam as a result of the nontrivial topology of the valleys. Next, we present the numerical demonstration of dynamical topological phase transitions driven by nonlinearity of the photonic medium, which occur in soliton SSH lattices. The phase transitions, marked by the appearance of topological edge states in the band gap, occur due to the setup which enables continually changing values of the intracell and intercell soliton couplings. Finally, we propose a scheme for creating and manipulating synthetic anyons in a noninteracting system by perturbing it with specially tailored localized probes. The external probes are needed because noninteracting systems do not possess the kind of TO required to support anyons. We start from a 2DEG in a uniform magnetic field (in an integer QHE state) and introduce thin solenoids carrying a fractional magnetic flux. We find a suitable ground state and demonstrate the fractional braiding statistics in the coordinates of the solenoids.
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Cited by 1 Pith paper
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Robust translational invariance in topological bands against lattice potentials and disorders
The paper defines fundamental length scales for Landau levels and fractional quantum Hall phases below which discrete lattice potentials stop breaking continuous magnetic translational symmetry.
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