A numerical approach is employed to explain transport characteristics in realistic, quantum Hall-based Aharonov-Bohm (AB) interferometers. Firstly, the spatial distribution of incompressible strips, and thus the current channels, are obtained by applying a self-consistent Thomas-Fermi method to a realistic heterostructure under quantized Hall conditions. Secondly, the timedependent Schrödinger equation is solved for electrons injected in the current channels. Distinctive AB oscillations are found as a function of the magnetic flux. The oscillation amplitude strongly depends on the mutual distance between the transport channels and on their width. At an optimal distance the amplitude and thus the interchannel transport is maximized, which determines the maximum visibility condition. On the other hand, the transport is fully suppressed at magnetic fields corresponding to half-integer flux quanta. The results confirm the applicability of realistic AB interferometers as controllable current switches. Recent low-temperature transport experiments [3-8] performed at two-dimensional (2D) electron systems (2DESs) utilize the quantum Hall (QH) effect to investigate and control the electron dynamics via their AB phase. An interesting difference between the original AB experiments and QH interferometers is the fact that in the latter the electron path itself may depend on the magnetic field B. To describe electron transport in QH interferometers, the singleparticle edge-state approach [9] is common, but neglects the dependence of the area enclosed by the current-carrying channels on the magnetic field [10], as well as on the channel widths. However, as shown explicitly below, the actual paths can be obtained considering the full manybody electrostatics, which yields the spatial distribution of compressible and incompressible strips [11].The essential features of the observed AB oscillations in QH interferometers have been explained using edge-channel simulations and Coulomb interactions at the classical (Hartree) level [4,12,13]. However, a complete theoretical picture of the observed phenomenon is still missing [6,14]. To attain this, it would be particularly important to (i) describe the full electrostatics by handling the crystal growth parameters and the 'edge' definition of the interferometer and (ii) supply this scheme with a dynamical study on electronic transport in the 2DES.The objective of this work is to take important steps towards a comprehensive explanation of the AB characteristics in QH interferometers. Firstly, we apply the 3D Poisson equation and the Thomas-Fermi approximation to the given heterostructure [15], taking into account the lithographically defined surface patterns. In this way, we obtain the electron and potential distributions under QH conditions [16,17]. For completeness, we utilize this scheme for the real experimental geometry resulting from the trench-gating technique. Secondly, we determine a model potential describing the current channels and use a time-dependent propagation scheme to mon...