  We give a theoretical study of unusual resistive (dynamic) localized states
in anisotropic Josephson junction ladders, driven by a DC current at one edge.
These states comprise nonlinearly coupled rotating Josephson phases in adjacent
cells, and with increasing current they are found to expand into neighboring
cells by a sequence of sudden jumps. We argue that the jumps arise from
instabilities in the ladder's superconducting part, and our analytic
expressions for the peculiar voltage (rotational frequency) ratios and I-V
curves are in very good agreement with direct numerical simulations.
