“…More involved constitutive relations appear in two main scenarios: (i) anisotropic media, where electric permittivity and magnetic permeability become tensors (cf. uniaxial and biaxial crystals [3][4][5][6][7], Weyl semimetals [8,9], and magnetized materials [10,11]); (ii) novel effects in matter described by extended constitutive relations that introduce additional electric and magnetic responses, encoded as linear functions of the type D = D(E, B) and H = H(E, B), in general. This happens, for instance, in bi-isotropic media [12][13][14][15], chiral materials [16], topolog-ical insulators [17][18][19][20][21][22], relativistic electron gases [23], axion electrodynamics [24][25][26], and Lorentz-violating electrodynamics [27,28], as well.…”