Limits to the Hall Effect and Other Nonreciprocal Effects in Three‐Dimensional Metamaterials

Metamaterials can exhibit exotic nonreciprocal properties, yet corresponding fundamental limits and design blueprints achieving them are largely unexplored. Here, we derive comprehensive bounds on the effective nonreciprocal properties of three-dimensional metamaterials and identify microstructures achieving or approaching these bounds. We assume that the underlying equations are equivalent to the conductivity problem in a weak applied magnetic field. While we focus on the Hall effect, our results are more generally applicable, particularly to the Faraday effect in the quasistatic regime and in the absence of losses and resonances. Our bounds yield three important implications: First, the effective Hall mobility of a metamaterial cannot be larger than the largest Hall mobility among the constituent materials. Second, under additional conditions, the effective Verdet constant cannot be enhanced either. Third, for diagonal Hall tensor components, the optimal values are achieved either by one of the pure phases or a rank-1 laminate formed from them, provided that the Hall coefficients of all phases have the same sign. Our work elucidates the limits of nonreciprocal metamaterials and identifies key prerequisites for obtaining exotic phenomena such as sign-inversions and enhancements. Several extensions appear within reach, for example, to the Faraday effect in metamaterials exhibiting plasmonic resonances.