Abstract
The classical electron dynamics in two-dimensional antidot lattices subjected to a magnetic field with a strong in-plane component is studied numerically. The anisotropy of the Fermi contour of the two-dimensional electron gas, produced by the parallel field, strongly modify the electron trajectories. We calculate the Poincar\'e surface of the section, and magnetoresistance with such distorted Fermi contour and obtain good agreement with experimental results.
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