Incoherent scatter radars measure ionosphere parameters using modified Thom
son scatter from free electrons in the target (see e.g. Hagfors, 1997). The
integrated cross section of the ionospheric scatterers is extremely small
and the measurements can easily be disturbed by signals returned by unwante
d targets. Ground clutter signals, entering via the antenna side lobes, can
render measurements at the nearest target ranges totally impossible. The E
ISCAT Svalbard Radar (ESR), which started measurements in 1996, suffers fro
m severe ground clutter and the ionosphere cannot be measured in any simple
manner at ranges less than about 120-150 km, depending on the modulation e
mployed. If the target and clutter signals have different, and clearly iden
tifiable, properties then, in principle, there are always ways to eliminate
the clutter. In incoherent scatter measurements, differences in the cohere
nce times of the wanted and unwanted signals can be used for clutter cancel
lation. The clutter cancelation must be applied to all modulations, usually
alternating codes in modern experiments, used for shorter ranges. Excellen
t results have been obtained at the ESR using a simple pulse-to-pulse clutt
er subtraction method, but there are also other possibilities.