“…However, if the array consists of multimode waveguides, the rate of light energy transport across the structures and the amplitude of the collective Bloch oscillations may strongly depend on the particular superposition of the excited individual modes, due to difference in the overlap integrals of different modes with neighboring waveguides [19]. In that scenario, resonant mode conversion utilizing longitudinal waveguide modulation [15], affords rich possibilities for the dynamical control of the weights of guided modes and, therefore, the global diffraction rate [20,21]. Different approaches are available to realize resonant mode conversion, including periodic mechanical stress and photo-induced gratings [22][23][24].…”