Recently discovered vortex electron beams [1][2][3] share the wave property of helical wavefronts with vortices observed in optical, acoustical and radio waves. [4][5][6][7][8] This vortex property gives the wave orbital angular momentum (OAM) which can be transferred to particles to make them rotate as was demonstrated with light optics and acoustical waves. [9][10][11][12] Electron vortex beams also carry an orbital angular momentum which is quantised to m h per electron with m the topological charge of the vortex. Breaking the circular symmetry of the vortex wave in free space by elastic interaction with a nanoparticle that does not have circular symmetry is theoretically expected to lead to an exchange of angular momentum between beam and particle because angular momentum is no longer a good quantum number. [ 13 ] This means that also with electron beams one expects that transfer of OAM to nanoparticles is possible.Here, we show experimental evidence of OAM induced rotation of supported Au nanoparticles by impact with m = ± 1 electron vortex beams with the direction of rotation determined by the sign of m . This observation is a qualitative confi rmation of the theoretical prediction and adds transfer of angular momentum to nanoparticles to the already wide range of possible applications of electron vortex beams. The observed rotation of the nanoparticles also allows studying the friction of the Au nanoparticles with their support on the nanoscale leading to a rotational diffusion coeffi cient in agreement with previously reported theoretical values. [ 14 ] Electron vortex beams have been produced in transmission electron microscopes in different ways but they all have in common that the electron wave function in a plane perpendicular to the optical axis can be described by a product of azimuthal and radial parts:With m the topological charge and f( r , z ) the radial distribution function that generally depends on z as the beam focusses and diverges along the optical axis z . Making use of a fork aperture in the condenser plane of a transmission electron microscope as sketched in Figure 1 we can produce vortex beams of m = −1,0, + 1 with diameters down to the atomic level [ 15 ] depending on the convergence angle α . Neglecting lens aberrations we can obtain an expression for the beam profi le at the beam waist: [ 16 ] fIn this experiment we make use of dispersed colloidal Au nanoparticles on a supporting thin fi lm of Si 3 N 4 of thickness 15 nm. We illuminate one such nanoparticle with a diameter of approximately 3 nm with an electron vortex with a radial distribution matching the size of the nanoparticle as sketched in Figure 1 . Imaging the elastically transmitted electrons through the particle allows us to observe the lattice planes of the particle as in conventional high resolution transmission electron microscopy. Figure 2 shows the resulting images as a function of time for illuminating the particle either with the left or right handed vortex beam m = + −1. Arrows in the images indicate the (111) lat...