A. Schmidt et Mq. Bao, THE MODULATION OF RADAR BACKSCATTER BY LONG OCEAN WAVES - A QUADRATICALLY NONLINEAR PROCESS, J GEO RES-O, 103(C3), 1998, pp. 5551-5562
Radar imaging of ocean scenes requires knowledge of the modulation of
the radar backscatter by long ocean waves. By using the conventional c
omposite surface theory, the modulation of the radar backscatter can b
e related to a single parameter of the ocean wave field, such as slope
or orbital velocity of the long waves. Usually, this relationship is
assumed to be linear and described by a linear modulation transfer fun
ction (MTF). Consequently, most investigations of the modulation of th
e ocean radar backscatter concentrate on the calculation of this Linea
r MTF. However, the coherence between the variations of the backscatte
red radar power and those of the orbital velocity associated with the
long waves is generally low at C and X bands. In this paper we make th
e hypothesis that the low coherence is due to a nonlinear relationship
between the radar backscatter and the long ocean waves (rather than t
o the neglect of other possible modulation sources). In order to quant
ify this nonlinearity, we estimate linear and quadratic MTFs from time
series of the backscattered radar power and the Doppler shift of the
backscattered radar signal. The latter is directly related to the orbi
tal velocity of the long waves. The data were acquired by a scatterome
ter mounted on a sea-based platform in the North Sea. We define the co
herence as the fraction of the output spectrum that can be related to
the input spectrum by a measured transfer function, which can be eithe
r linear or linear and quadratic. We find that the coherence between t
he backscattered radar power and the Doppler shift can be increased by
up to 0.14 by using linear and quadratic MTFs instead of a linear one
. However, at X band the coherence never becomes larger than 0.5. Thus
we conclude that the modulation process cannot be described fully by
a quadratically nonlinear system which relates the radar backscatter t
o the orbital velocity of the long waves. Therefore a higher order of
nonlinearity has to be considered.