We propose an effective scheme for the generation of intense coherent extreme ultraviolet light beams carrying orbital angular momentum (OAM). The light is produced by a high-gain harmonicgeneration free-electron laser (FEL), seeded using a laser pulse with a transverse staircase-like phase pattern. During amplification, diffraction and mode selection drive the radiation profile towards a dominant OAM mode at saturation. With a seed laser at 260 nm, gigawatt power levels are obtained at wavelengths approaching those of soft x-rays. Compared to other proposed schemes to generate OAM with FELs, our approach is robust, easier to implement, and can be integrated into already existing FEL facilities without extensive modifications of the machine layout.PACS numbers: 42.50. Tx, 42.65.Ky, 41.60.Cr Modern generation free-electron lasers (FELs) delivering high-brightness optical beams in the extreme ultraviolet (XUV) [1] and x-ray regions [2,3] have become indispensable tools for probing structural and chemical properties of matter at femtosecond temporal and nanometer spatial resolutions [4]. At present, transverse radiation profiles from FELs working at saturation are limited to a fundamental Gaussian-like mode with no azimuthal phase variation. This is true for FELs based on selfamplified spontaneous emission (SASE), where the amplification starts from electron shot-noise [5][6][7][8][9][10][11][12][13][14], as well as for seeded FELs, such as those based on high-gain harmonic-generation (HGHG), where the amplification process is triggered by a coherent input signal [1,15,16].Generation of high-order radiation modes, however, is a subject of strong interest, not only from the fundamental point of view but also in practical applications. In particular, helically phased light beams or optical vortices with a field dependence of exp (ilφ), where φ is the azimuthal coordinate and l an integer referred to as the topological charge, are currently among intensively studied topics in optics. These light beams, which carry orbital angular momentum (OAM) [17] that can be transferred to atoms, molecules, and nanostructures [18][19][20][21][22][23], have already been utilized at visible and infrared wavelengths in a wide variety of applications, ranging from micromanipulation [24], detection of spinning objects [25], microscopy [26], and optical data transmission [27][28][29]. Perhaps the most promising applications of vortex beams at short wavelengths are in x-ray magnetic circular dichroism, where different OAM states allow the separation of quadrupolar and dipolar transitions [30], photoionization experiments, where the dipolar selection rules are violated giving rise to new phenomena beyond the standard effect [31], and in resonant inelastic x-ray scattering, where vortex-beam-mediated coupling to vibrational degrees of freedom could provide important information on a wide range of molecular materials [32].In the case of visible light, OAM is commonly generated by sending the beam through a suitable optical element (e.g., ...