We study the classical dynamics of a charged particle in two dimension
s, under the influence of a perpendicular magnetic and an in-plane ele
ctric field. We prove the surprising fact that there is a finite regio
n in phase space that corresponds to the otherwise drifting particle b
eing trapped by a local repulsive potential. Our result is a direct co
nsequence of Kolmogorov-Arnold-Moser theory and, in particular, of Mos
er's theorem. We illustrate it by numerical phase portraits and by an
analytic approximation to invariant curves.