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Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

Principles of Modern Radar - Volume 2 1891121537

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5.2 CS Theory 157The combined space-time steering vector for a target is then given as the Kronecker product<strong>of</strong> the temporal and spatial steering vectors, that is,a( f s , f d ) = a t ( f d ) ⊗ a s ( f s )For a given range bin, the vector a( f s , f d ) represents the data that the radar would collectover a CPI if only a single target having unit scattering amplitude were present at theangle-Doppler location encoded by f s and f d . Specifically, the steering vector a( f s , f d )corresponds to a single column <strong>of</strong> the A matrix for this MTI problem.Let us discretize the frequency variables into N s ≥ J spatial frequency bins andN d ≥ K Doppler frequency bins spaced uniformly across the allowed ranges for eachvariable to obtain N = N s N d unique steering vectors. We can organize the resultingsteering vectors into a matrix A ∈ C M×N . Neglecting range ambiguities, we can definethe scene reflectivity function at a given range as x ∈ C N , where the rows <strong>of</strong> x areindexed by angle-Doppler pairs 8 ( f s , f d ). We then obtain the linear relationship betweenthe collected data and the scene <strong>of</strong> interest asy = Ax + ewhere e in this case will include the thermal noise, clutter, and other interference signals.A more realistic formulation would include measured steering vectors in the matrix A.Thus, we see that the data for a multichannel pulsed radar problem can be placed easilyinto the framework (5.1).5.2.2.4 CommentsThe overall message is that most radar signal processing tasks can be expressed in terms <strong>of</strong>the linear model (5.1). Additional examples and detailed references can be found in [17].We should also mention that both <strong>of</strong> these examples have used the “standard” basisfor the signal <strong>of</strong> interest: voxels for SAR imaging and delay-Doppler cells for MTI. Inmany cases, the signal <strong>of</strong> interest might not be sparse in this domain. For example, aSAR image might be sparse in a wavelet transform or a basis <strong>of</strong> canonical scatterers. 9 Asanother example, in [18], the authors explore the use <strong>of</strong> curvelets for compressing formedSAR images. Suppose that the signal is actually sparse in a basis such that x = α,with α sparse. In this case, we can simply redefine the linear problem asy = Aα + e (5.10)to obtain a model in the same form with the forward operator A. Indeed, many <strong>of</strong> theearly CS papers were written with this framework in mind with A = , where isthe measurement operator, and is the sparse basis. In this framework, one attempts todefine a measurement operator that is “incoherent” from the basis . We will not dwellon this interpretation <strong>of</strong> the problem and refer the interested reader to, for example, [19].8 Note that x in this context is the same image reflectivity function used in common STAP applications [15].9 Selection <strong>of</strong> the appropriate sparse basis is problem dependent, and we refer the reader to the literaturefor more detailed explorations.

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