Fig. 1: Photonic 3D CI by cubic supercell modulation at N = NW = 2.
From: Cubic 3D Chern photonic insulators with orientable large Chern vectors

Each (a, b, d, e) panel shows the crystal unit cell, the irreducible Brillouin zone (IBZ) and the band-structure (BS). Frequencies f are given in reduced units, ∣a∣ being the scale invariant lattice parameter and c the speed of light. Sectors (c) and (f) contain the topological characterization via photonic Wilson loops (WL), in the Weyl semimetallic (WS) phase and in the 3D CI phase, respectively. a Photonic crystal constructed from cylinders of radius r0 = 0.15 and dielectric constant ε = 16 at TRS. The three lowest photonic modes display a three-fold degeneracy at R and the two lowest bands are fully degenerate in the displayed energy window. b TRS breaking implemented via a gyro-electric response with \({\eta }_{z}^{{N}_{W} = 2}=16\): the bias field is adjusted in order to split the Weyl points of approximately half the BZ, i.e. at \({k}_{z}^{\pm }=\pm \! \frac{\pi }{2| a| }\), along the \({{{{{{{\bf{S}}}}}}}}{{{{{{{\bf{R}}}}}}}}{{{{{{{{\bf{S}}}}}}}}}^{\prime}\) line where \({{{{{{{{\bf{S}}}}}}}}}^{\prime}={{{{{{{\bf{S}}}}}}}}-{{{{{{{{\bf{b}}}}}}}}}_{z}\). c Electromagnetic section Chern number calculated on 2D kz planes normal to the magnetization (upper panel) and transverse flow of the θy eigenvalue of the WL matrix summed over the entire subset of νocc bands lying below the local gap at kz (lower panel). The discontinuity of the section Chern number at the wavevector of each Weyl point \({k}_{z}^{\pm }\) is used a measure its topological charge (q± = 1). d Artificial folding of the bands on a N = 2 cubic supercell: Weyl points superimpose at Z in the new BZ. e Coupling and annihilation of Weyl points through a N = 2 supercell modulation with parameter rm = r0/20. The amplified modulation is graphically visualized via a colorbar with rmax = r0 + rm and rmin = r0 − rm. A topological direct gap (fg) at Z is opened, with gap-to-midgap (fg/fm) ratio of 1.86%. The size of gap can be appropriately tuned by choosing the value of the modulation, as in the inset. f The section Chern Cz number displays constant unit value everywhere in the BZ, establishing the system to be in the 3D CI phase. Source data are provided as a Source Data file.