We demonstrate ultrafast all-optical deflection of spatial solitons in an AlxGa1−xAs slab waveguide using 190 fs, 1550 nm pulses which are used to generate and deflect the spatial soliton. The steering beam is focused onto the top of the waveguide near the soliton pathway and the soliton is steered due to refractive index changes induced by optical Kerr, or free carrier (Drude) effects. Angular deflections up to 8 mR are observed.Optical spatial solitons are shape-invariant wavepackets maintained by the balancing of linear and nonlinear optical effects. The nonlinear processes which compensate for diffraction and produce guiding can be induced via, e.g., an intensity dependent refractive index (Kerr effect), photorefractive effects or cascaded second order optical nonlinearities.[1] While interesting objects of study in themselves, solitons are also being considered for information processing applications such as optically reconfigurable logic devices [2]. The switching of spatial solitons is an essential process for many applications, and popular embodiments include nonlinear interactions of co-propagating spatial solitons [3,4] or electro-optically induced pathway distortions. All-optical ultrafast reconfiguration of soliton pathways, e.g., due to the Kerr effect, in the telecommunication wavelength regime (1.3-1.6 µm) is an attractive goal and offers higher switching speeds compared to electro-optic methods. However, besides the co-propagating schemes one should consider other techniques that have been discussed in the more general realm of "light by light'' switching such as optically or electrooptically induced birefringence [5,6], optically induced prisms [7] or gratings [8].Here we demonstrate an ultrafast, non-planar switching scheme for spatial solitons formed in a 2D Al x Ga 1−x As waveguiding layer by inducing a localized refractive index perturbation in the spatial soliton pathway using femtosecond light pulses normally incident on the waveguide. The general principle of the technique is depicted in Fig. 1 which shows an optical soliton formed at the entrance facet of a 2D waveguide by an ultrashort laser pulse. A separate ultrashort pump pulse is focussed onto the top of the waveguide, introducing an index change ∆n in the waveguiding layer with the spatial profile of the pump pulse. The ∆n, which can be generated on either side of the spatial soliton pathway, causes the soliton to deflect while remaining intact: The robust nature of solitons propagation means that it is not not necessary to form an optically induced prism of a particular shape [9]. The deflection direction also depends on the sign of ∆n which is > 0 for the optical Kerr effect and < 0 for any free carrier (Drude) induced index change in Al x Ga 1−x As. For ∆n > 0 the soliton path bends towards the index gradient, whereas for ∆n < 0 deflection occurs in the opposite direction. Temporal control of the deflection is achieved by delaying the soliton forming pulse with respect to the pump pulse; temporal resolution is related to the con...