A variety of transport phenomena observed at laterally confined two- d
imensional electron systems (2DES) prove the occurrence of non-local c
ontributions to the electronic conductance in these systems. However,
this non-local regime accompanied by a non-equilibrium population of t
he edge states with respect to the 2D bulk state is quenched at rather
low values of current-driving electric fields. We analyse the non-Ohm
ic behaviour of SdH oscillations at GaAs/GaAlAs Quantum Hall conductor
s on the basis of a model including edge and bulk conduction and deduc
e the non-equilibrium population of edge and bulk states quantitativel
y.The spatial separation between edge and bulk states was changed by t
ilting the samples with respect to the magnetic field. The resulting a
ngular dependences of equilibration parameters could be quantitatively
explained by the change of the ratio of spin splitting to cyclotron e
nergy being present in 2DES in tilted magnetic fields.