The equilibrium properties of a relativistic nonneutral electron layer confined in a magnetically insulated cylindrical diode are investigated within the framework of the steady-state (3/t=O) Vlasov-Maxwell equations. The analysis is carried out for an infinitely long electron layer aligned parallel to a uniform externally applied magnetic field B 9z, which provides radial confinement of the electrons. The theoretical analysis is specialized to the class of self-consistent Vlasov equilibria fb0(,k) in which all electrons have the b 2 same canonical angular momentum (Pa=Po =const.), and the same energy (H=mc ), i.e., 0 2 fb b Rc/2Trm) 6 (H-mc )6(P6-P 0 ). One of the most important features of the analysis is that the closed analytic expressions for the self-consistent electrostatic potential %0(r) and the e-component of vector potential A 0 (r) are obtained. Moreover, all essential equilibrium quantities, such as electron density profile O 0* nb(r), total magnetic field B (r), perpendicular temperature profile Tib (r), etc., b Oz L c an be calculated self-consistently from these potentials. As a special case, the equilibrium properties of a planar diode are investigated in the limit of large aspect ratio, further simplifying the functional form of the electrostatic and vector potentials. Detailed equilibrium properties are investigated numerically for a cylindrical diode over a broad range of system parameters, including diode voltage Vo, cathode electric field, electron density nb at the cathode, diode polarity, and externally applied magnetic field B 0 .2