Super Bloch oscillations arise when an additional periodic driving force is added to F 0 , resulting in: F ( t ) = F 0 + Δ Δ F sin ⁡ ⁡ ( ω ω t + φ φ ) The details of the motion depend on the ratio between the driving frequency ω ω and the Bloch frequency ω ω B . A small detuning ω ω − − ω ω B results in a beat between the Bloch cycle and the drive, with a drastic change of the particle motion. On top of the Bloch oscillation, the motion shows a much larger oscillation in position space that extends over hundreds of lattice sites. Those Super Bloch oscillations directly correspond to the motion of normal Bloch oscillations, just rescaled in space and time.