The fact that light beams are able to carry a mechanical angular momentum is well-known. In paraxial beams, angular momentum can be represented as a sum of the spin (SAM) and orbital (OAM) angular momentum. After paper Allen et al.[1], a lot of articles devoted to the generation, study and the use of beams with orbital angular momentum, or "vortex beams", have been published. To date, vortex beams were obtained in the range from radio frequencies [2] to the soft X-ray radiation [3]. Nevertheless, there are only five studies [4][5][6][7][8], in which vortex beams in the terahertz range have been generated.Recently, using radiation of the Novosibirsk free electron laser [9] and silicon binary spiral phase axicons, terahertz Bessel beams with OAM with topological charges 1 l r and 2 l r have been generated for the first time [7]. The intensity distributions of the beams formed by the axicons are in good agreement with the distributions calculated for Bessel beams, but they are identical for both left-handed and right-handed helicities. To determine the characteristics of the beams associated with their rotation, we applied classical experiments on diffraction and interference, adapting them to the terahertz range.A direct method of detecting the rotation of a beam was its diffraction on a half-plane (Fig. 1, a). Similar experiments with Laguerre-Gaussian and Bessel vortex beams were performed in the visible region in [11], where for the Bessel beams only qualitative results were obtained because of the short laser wavelength and the tiny interference pattern.In Fig. 1, b the diffraction patterns calculated numerically at several distances are shown. In the experiments, a 16.32 12.24 u mm 2 microbolometer array (MBA) with pixel size of 0.051 mm was used as a detector for imaging of diffraction pattern. Because of geometrical restrictions, only planes located at a distance z of more than 35 mm could be recorded. The recorded patterns were identical with the calculated ones.The diffraction patterns shown in Fig. 1 clearly demonstrate the rotation of the beam. According to the theory [12], the rate of change of azimuthal angle of the trajectory of the Poynting vector with z is given by 2