Abstract
Transverse self-diffusion of field-induced magnetic colloidal chains is measured using real-space imaging. It has been found that the mean-square displacement Δr2 depends on the aligning field H and displays two different behaviors. In short times Δr2 is subdiffusive, whereas in long times Δr2 exhibits normal diffusion. The characteristic time separating the two time regimes diverges exponentially with H, indicating fast frozen-in density fluctuations in the system. Our experimental results deviate significantly from the predictions of mode-coupling theory.