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Register a new userAcoustic Dirac degeneracy and topological phase transitions realized by rotating scatterers
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The artificial crystals for classical waves provide a good platform to explore the topological physics proposed originally in condensed matter systems. In this paper, acoustic Dirac degeneracy is realized by simply rotating the scatterers in sonic crystals, where the degeneracy is induced accidentally by modulating the scattering strength among the scatterers during the rotation process. This gives a flexible way to create topological phase transition in acoustic systems. Edge states are further observed along the interface separating two topologically distinct gapped sonic crystals.
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The study of magnonic thermal Hall effect has recently attracted attention because this effect can be associated with topological phases activated by Dzyaloshinskii-Moriya interaction, which acts similar to a spin-orbital coupling in an electronic system. A topological phase transition may arise when there exist two or more distinct topological phases, and this transition is often revealed by a gap closing. In this work, we consider a ferromagnetic honeycomb lattice described by a Hamiltonian that contains Heisenberg exchange interaction, Dzyaloshinskii-Moriya interaction, and an applied Zeeman field. When expanding the spin operators in the Hamiltonian using Holstein-Primakoff (HP) transformation to the order of $S^{1/2}$, where $S$ is the magnitude of spin, the thermal Hall conductivity stays negative for all values of parameters such as the strength of Zeeman interaction and temperature. However, we demonstrate in this work that by including the next order, $S^{-1/2}$, in HP transformation to take into account magnon-magnon interaction, the Hartree type of interaction gives rise to topological phase transitions driven by temperature. When the temperature increases, we find that the gap of the magnonic energy spectrum closes at Dirac points at a critical temperature, $T_c$, and the gap-closing is indeed the signature for a topological phase transition as confirmed by showing that the Chern numbers are distinct above and below $T_c$. Finally, our analysis points out that thermal Hall conductivity exhibits sign reversal at the same temperature. This phenomenon can be used in experiments to verify the topological nature of magnons in honeycomb magnets.
Recent studies indicated that helical organic molecules, such as DNA and $alpha$-helical protein, can behave as Thouless quantum pumps when a rotating electric field is applied perpendicularly to their helical axes. Here we investigate the influence of long-range hoppings on this topological pumping of electrons in single-helical organic molecules. Under variation of the long-range hoppings governed by a decay exponent $mu$, we find an energy gap in the molecular band structure closes at a critical value $mu_c$ of the decay exponent and reopens for $mu$ deviating from $mu_c$. The relevant bulk bands in a pumping cycle acquire different Chern numbers in the strong ($mu<mu_c$) and weak ($mu>mu_c$) long-range hopping regimes, with a sudden jump at criticality. This topological phase transition is also shown to separate two distinct behaviors of the midgap end states in the pumping process. The end states carry quantized current pumped by the rotating electric field and the current forms a plateau by sweeping the Fermi energy over the gap. In the strong hopping phase, the quantized current plateau is positive, which is reversed to a negative one with smaller amplitude in the weak hopping phase. However, the reversal is a smooth crossover, not a sharp transition, due to the finite sizes of the molecules. We show that these transport characteristics of the topological phase transition could also be observed at finite temperatures.
We show how transitions between different Lifshitz phases in bilayer Dirac materials with and without spin-orbit coupling can be studied by driving the system. The periodic driving is induced by a laser and the resultant phase diagram is studied in the high frequency limit using the Brillouin-Wigner perturbation approach to leading order. The examples of such materials include bilayer graphene and spin-orbit coupled materials such as bilayer silicene. The phase diagrams of the effective static models are analyzed to understand the interplay of topological phase transitions, with changes in the Chern number and topological Lifshitz transitions, with the ensuing changes in the Fermi surface. Both the topological transitions and the Lifshitz transitions are tuned by the amplitude of the drive.
A recently proposed curvature renormalization group scheme for topological phase transitions defines a generic `curvature function as a function of the parameters of the theory and shows that topological phase transitions are signalled by the divergence of this function at certain parameters values, called critical points, in analogy with usual phase transitions. A renormalization group procedure was also introduced as a way of flowing away from the critical point towards a fixed point, where an appropriately defined correlation function goes to zero and topological quantum numbers characterising the phase are easy to compute. In this paper, using two independent models - a model in the AIII symmetry class and a model in the BDI symmetry class - in one dimension as examples, we show that there are cases where the fixed point curve and the critical point curve appear to intersect, which turn out to be multi-critical points, and focus on understanding its implications.
The traditional concept of phase transitions has, in recent years, been widened in a number of interesting ways. The concept of a topological phase transition separating phases with a different ground state topology, rather than phases of different symmetries, has become a large widely studied field in its own right. Additionally an analogy between phase transitions, described by non-analyticities in the derivatives of the free energy, and non-analyticities which occur in dynamically evolving correlation functions has been drawn. These are called dynamical phase transitions and one is often now far from the equilibrium situation. In these short lecture notes we will give a brief overview of the history of these concepts, focusing in particular on the way in which dynamical phase transitions themselves can be used to shed light on topological phase transitions and topological phases. We will go on to focus, first, on the effect which the topologically protected edge states, which are one of the interesting consequences of topological phases, have on dynamical phase transitions. Second we will consider what happens in the experimentally relevant situations where the system begins either in a thermal state rather than the ground state, or exchanges particles with an external environment.
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