We demonstrate optical coherent control of the emission direction of THz radiation. Femtosecond laser pulses are used to excite different types of ultrafast photocurrents along different directions in a bulk GaAs sample. The overall emission pattern can be modified by changing the phase of the optical excitation. With this method, THz beam steering of about 8 degrees is realized. A simple dipole-based model allows us to relate the size of the steering effect to the amplitude ratio between the different photocurrent contributions and to diffraction effects resulting from the excitation spot size.Research and development in the THz frequency range has been significantly intensified in many scientific and technical areas during the last decades. The main drivers for this process were existing and envisaged applications in communications, spectroscopy, material science, and security 1 . Among these drivers, the need for spatial control has become more and more important. For instance, communications at high frequencies requires the realization of different propagation channels 2 . Furthermore, spatially-resolved spectroscopy and imaging applications are based on a relative movement between the THz field and the device under test (DUT) 3 . One possible approach to accomplish such demands is given by a steerable THz emitter. Various technical realizations based on changes of laser excitation angles or diffractive gratings have been introduced so far 4-8 . However, mechanical movement of components within a measurement setup limits the speed of the measurement process and diffraction effects usually show strong frequency-dependant steering angles. Thus, the development of techniques that allow for non mechanical and broadband steering of the THz beam is desirable.In this work, we present an alternative approach for fast and reliable control of the emission direction of THz radiation. The beam steering as demonstrated here does not rely on mechanical movements of any parts of the setup or on beam shaping apertures but is realized by optical coherent control, i.e., by modifying the phase of the optical excitation pulse. Beam steering is realized by controlling the interference between different optically-induced currents in a bulk GaAs sample. Due to the nonlinear properties of the GaAs crystal, it is possible to induce shift currents, which result from a spatial shift of the center of the electron charge during excitation 9 . Those currents depend on the phase of the excitation pulse and, along certain crystal axes, the direction can be reversed by changing the phase of the excitation. Additionally,