Abstract
In this paper we study the homogenization of a class of energies concentrated on lines. In dimension (i.e., in codimension ) the problem reduces to the homogenization of partition energies studied by \cite{AB}. There, the key tool is the representation of partitions in terms of functions with values in a discrete set. In our general case the key ingredient is the representation of closed loops with discrete multiplicity either as divergence-free matrix-valued measures supported on curves or with -currents with multiplicity in a lattice. In the dimensional case the main motivation for the analysis of this class of energies is the study of line defects in crystals, the so called dislocations.
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