Abstract
Antidot lattices with top and back gate tunability allow the electronic transport properties of a sample to be studied at a constant electron density while the two-dimensional electron system is shifted in the $z$ direction. The antidot potential is found to remain essentially unaltered in our sample during a constant density sweep, while other parameters such as the background mobility or wave function symmetry in the $z$ direction vary. The impact of these changes on the classical commensurability peaks, the Aharonov-Bohm-type oscillations, and on a weak-localization-type feature around $B=0\phantom{\rule{0.3em}{0ex}}\mathrm{T}$ are investigated. In addition, a peak splitting appears in oscillations superimposed on the main commensurability peak at high electron densities.
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