We present a relativistic description of electron vortex beams in a homogeneous magnetic field. Including spin from the beginning reveals that spin-polarized electron vortex beams have a complicated azimuthal current structure, containing small rings of counterrotating current between rings of stronger corotating current. Contrary to many other problems in relativistic quantum mechanics, there exists a set of vortex beams with exactly zero spin-orbit mixing in the highly relativistic and nonparaxial regime. The well defined phase structure of these beams is analogous to simpler scalar vortex beams, owing to the protection by the Zeeman effect. For states that do show spin-orbit mixing, the spin polarization across the beam is nonuniform rendering the spin and orbital degrees of freedom inherently inseparable.Introduction-The concept of light beams carrying orbital angular momentum along the propagation axis has been widely utilized in modern optics [1][2][3]. Based on analogies of the governing wave equations, vortex beams have also been predicted and generated for electrons [4][5][6][7][8][9][10][11][12] and neutrons [13], as well as proposed for atoms [14,15]. This promises the ability to probe and manipulate matter on smaller length scales, but also opens up the possibility to consider the interaction of vortex beams with external fields [16][17][18][19][20], other vortex beams [21,22] and atoms [23].In the simplest description these vortex beams are scalar and obey the paraxial Schrödinger equation. Going beyond the paraxial approximation reveals a linking between the spin and orbital degrees of freedom arising whenever the beam is tightly confined, complicating the vortex structure [24,25]. And whereas light beams as solutions of Maxwell's equation are naturally relativistic, for particles it is important to distinguish between the nonrelativisitic regime based on Schrödinger's equation and the relativistic regime covered by the Dirac equation.Whether or not a nonrelativistic description suffices depends not only on the energy of the electron beam involved, but also on the importance the spin of the particle in the interaction in question, as spin is naturally included in the Dirac equation [26,27]. For electrons traveling through a magnetic field it is of particular importance to take the spin into account, because it interacts strongly with the field.We analytically solve the Dirac equation for an electron in a homogeneous magnetic field, a problem first considered by Landau [27,28]. The interaction with the magnetic field confines the beam and gives rise to a set of discrete energy levels (Landau levels) [16,28]. On top of that the Zeeman effect shifts the energy of the positive and negative spin states relative to each other. The quantized Landau and Zeeman contributions to the energy determine which states undergo spin-orbit mixing with each other and completely forbid spin-orbit mixing