For quadratic-band-crossing semimetals, a static sigma-2 mass gives Chern number +-sgn(tx tz), while elliptically polarized light gives Chern number +-sgn(phi); the claimed linear-polarization trivial insulator is actually gapless in the first-order Floquet model.
Quantum Geometry and Landau Levels of Quadratic Band Crossings
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abstract
We study the relation between the quantum geometry of wave functions and the Landau level (LL) spectrum of two-band Hamiltonians with a quadratic band crossing point (QBCP) in two-dimensions. By investigating the influence of interband coupling parameters on the wave function geometry of general QBCPs, we demonstrate that the interband coupling parameters can be entirely determined by the projected elliptic image of the wave functions on the Bloch sphere, which can be characterized by three parameters, i.e., the major $d_1$ and minor $d_2$ diameters of the ellipse, and one angular parameter $\phi$ describing the orientation of the ellipse. These parameters govern the geometric properties of the system such as the Berry phase and modified LL spectra. Explicitly, by comparing the LL spectra of two quadratic band models with and without interband couplings, we show that the product of $d_1$ and $d_2$ determines the constant shift in LL energy while their ratio governs the initial LL energies near a QBCP. Also, by examining the influence of the rotation and time-reversal symmetries on the wave function geometry, we construct a minimal continuum model which exhibits various wave function geometries. We calculate the LL spectra of this model and discuss how interband couplings give LL structure for dispersive bands as well as nearly flat bands.
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Tunable phase transitions from semimetals to Chern insulators in two-dimensional quadratic-band-crossing materials
For quadratic-band-crossing semimetals, a static sigma-2 mass gives Chern number +-sgn(tx tz), while elliptically polarized light gives Chern number +-sgn(phi); the claimed linear-polarization trivial insulator is actually gapless in the first-order Floquet model.