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Floquet dynamics in multi-Weyl semimetals
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Multi-Weyl semimetals(m-WSMS) are characterized by anisotropic non-linear energy dispersion along 2-D plane and a linear dispersion in orthogonal direction. They have topological charge J and are realized when two or multiple Weyl nodes with nonzero net monopole charge bring together onto a high-symmetry point. The model Hamiltonians of such systems show various phases such as trivial normal insulators (NIs), WSMs and quantum anomalous Hall(QAH) states depending on the model parameters. We study a periodic driving of such Hamiltonians in trivial NI phase by circularly polarized light and shows this phase can be tunable to Weyl semimetals phase. This transition can be accomplished with large anomalous Hall conductivity which could be observed in transport measurements or pump-probe angle resolved photoemission spectroscopy experiments.
Forward citations
Cited by 2 Pith papers
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Phase transition from Weyl to self-linked semimetal using bi-circular laser
The paper reports laser-tunable double-ring and self-linked Fermi surfaces in a non-Hermitian triple Weyl model, but the linked topology is inferred from 2D slices rather than proven.
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Helicons in multi-Weyl semimetals
Helicon modes in multi-Weyl semimetals keep the linear-plus-quadratic wavevector dispersion of single Weyl semimetals, with the frequency scale set by charge-dependent plasma frequencies.
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