I. Introduction
In radar detection based upon array of sensors or pulse trains [1] –[3], the Interference Covariance Matrix (ICM) might comprise several contributions associated with different interference sources. The most common sources are
the electronic devices generating thermal noise, which is always present and leads to an ICM component modeled as , where is the thermal noise power and is the identity matrix;
the specific operating environment, whose backscattering gives rise to the clutter component;
jamming systems which can significantly modify the ICM depending on the jamming type and the radar signal processing. More precisely, if the radar performs spatial processing using sensors, then barrage noise jammers [4] illuminating the victim radar from the angle of arrival , , would yield the following ICM component \begin{equation} \sum _{k=1}^{K_J}\sigma _{J,k}^2 {\boldsymbol {v}}(\theta _{J,k}){\boldsymbol {v}}^{\dagger }(\theta _{J,k}), \end{equation} where denotes conjugate transpose, and \begin{equation} {\boldsymbol {v}}(\theta _{J,k})=[1 \quad e^{j2 \pi \nu _s(\theta _{J,k})} \quad \ldots \quad e^{j2 \pi \nu _s(\theta _{J,k})(N-1)}]^T \end{equation} are the power and the spatial steering vector of the -th jammer. In the last equation, denotes transpose and is the spatial frequency and is a function of . In the case of temporal processing, a noise jammer usually produces an ICM contribution equal to , where is the overall jammer power. Finally, still in the context of temporal processing, equation (1) can be modified to account for the effect of multi-tone continuous-wave jammers replacing with \begin{equation} {\boldsymbol {v}}(\nu _{J,k})=[1 \quad e^{j 2 \pi \nu _{J,k}} \quad \ldots \quad e^{j 2 \pi \nu _{J,k}(N-1)}]^T, \end{equation} where is the number of transmitted tones and is the normalized Doppler frequency of the th tone. Such jammers can emulate the radar cross section of Swerling 1 targets.