The invention relates to radar signal processing. More particularly, the invention relates to a single pulse imaging (SPI) radar method and system.
Radar imaging techniques, such as inverse synthetic aperture radar (ISAR), rely on measuring the Doppler shifts induced by relative motion between the target and the radar to generate an image of the target. High range resolution is achieved using pulse compression techniques, whereas high cross-range resolution relies on the accurate measurement of the Doppler shifts induced by uniform rotational motion of the target. In traditional ISAR processing, numerous pulses over a period of time must be processed using Fourier processing to measure the Doppler frequency of the moving target. If target scatterers move out of their range cells during the imaging time, or if the rotational motion is not uniform, the image will be smeared. Therefore, motion compensation algorithms must be used to produce a focused ISAR image.
Pulse compression allows a radar to obtain the range resolution of a short pulse without the need for very high peak transmit power by transmitting a long pulse that is phase or frequency modulated. The modulated pulse or waveform, is reflected back to the radar by scatterers that lie in the transmission path. This process can be viewed as the convolution of the transmitted waveform with an impulse response that is representative of the range profile illuminated by the radar. The purpose of pulse compression is then to estimate the range profile impulse response based upon the known transmitted waveform and the received radar return signal. The traditional method of pulse compression, known as matched filtering, has been shown to maximize the received signal-to-noise ratio (SNR), of the target return. A matched filter is applied by convolving the received signal with the time-reversed complex conjugate of the transmitted waveform. The traditional matched filter is limited by the range sidelobes produced by the filtering process. The sidelobes of large targets can mask the presence of nearby small targets, thus limiting the sensitivity of the radar.
Adaptive pulse compression (APC) by way of Reiterative Minimum Mean-Square Error (RMMSE), described in U.S. Pat. No. 6,940,450, issued Sep. 6, 2005 and incorporated herein by reference, is capable of accurately estimating the range profile illuminated by a radar by suppressing range sidelobes to the level of the noise floor. This is accomplished by adaptively estimating the appropriate receiver pulse compression filter to use for each individual range cell. Furthermore, the RMMSE algorithm, which has also been denoted as Adaptive Pulse Compression (APC) when applied to the radar pulse compression problem, has been shown to be robust to rather severe Doppler mismatch. A multistatic adaptive pulse compression (MAPC) formulation that can resolve a radar target in the presence of multiple radar return signals occupying a shared frequency spectrum is described in U.S. Ser. No. 11/268,755, filed Nov. 7, 2005 now U.S. Pat. No. 7,474,257, incorporated herein by reference (hereinafter “MAPC”).
It would be desirable to provide an adaptive radar processing system that can resolve a moving radar target image from a single transmitted pulse using a Doppler-sensitive variation of the multistatic adaptive pulse compression formulation thereby mitigating the need for motion compensation.
According to the invention, a single pulse imaging (SPI) radar system for creating a radar image from a plurality of Doppler phase-shifted return radar signals in a radar environment of moving targets includes a transmitter; a receiver for receiving a radar return signal; an analog-to-digital converter (ADC) coupled to the output of the receiver; a processor, coupled to the output of the ADC, that is programmed with an SPI algorithm that includes a bank of range/Doppler-dependent adaptive RMMSE-based filters; and a target detector. The algorithm estimates adaptively a range profile for each of the Doppler phase-shifted return radar signals to create the radar image of the moving targets.
Also according to the invention, a method for radar imaging using a single transmitted radar pulse includes transmitting a single radar pulse towards the moving targets; receiving a plurality of return reflected radar signals; and applying the SPI algorithm to the return signals to create the radar image of the moving targets.
Referring now to
Consider first a simplistic scenario whereby all of the scatterers are moving at the same velocity, v, relative to the radar platform. The motion relative to the radar platform induces a Doppler phase shift, θ, in the received signal for each scatterer. Let the length-N vector s denote the discrete-time version of the transmitted waveform. The length-N vector x(λ,θ)=[x(λ,θ)x(λ−1.θ) . . . x(λ−N+1.θ)] represents a set of N contiguous samples of the range profile impulse response. Note that the range profile is a function of θ, highlighting the fact that all of the scatterers in the range profile are moving at the same relative velocity and therefore induce the same Doppler phase shift θ in the radar return signal. The λth sample of the received radar return is defined as
y(λ,θ)=(x(λ,θ)∘e(θ))Ts+v(λ). (1)
for λ=0, . . . , L+N−2, where v(λ) is additive noise. (□)T is the transpose operation, L is the total number of contiguous range gates desired to be estimated (i.e. the processing window), and ∘ indicates the Hadarmard product (element-by-element multiplication). The N-dimensional vector e(θ)=[1ejθej2θ . . . ej(N-1)θ]T represents the relative phase shifts of the N contiguous samples of x(λ,θ) where θ is the Doppler phase shift between successive received samples.
Although the received radar return model of (1) is for scatterers moving at the same relative velocity, the model can easily be generalized to include scatterers moving at different velocities by integrating (1) over every possible Doppler phase shift (note that integration here represents the inclusion of received signal components over all values of θ and hence is not performed on the noise term). The λth sample of the total received signal is then
Although (2) is continuous in θ, it can be approximated by
where
and K is arbitrarily large, such that (3) is a good approximation of (2). For notational simplicity, we denote x(λ,θk)□xk(λ). By rearranging terms, (3) can be expressed as
where
{tilde over (s)}k=s∘e(θk) (6)
is a Doppler phase shifted version of the transmitted waveform. The collection of N contiguous samples of the received return signal y(λ)=[y(λ)y(λ+1) . . . y(λ+N−1)]T can therefore be expressed as
where
As shown by (7), the radar return can be viewed as the summation of the returns from K distinct range profiles, each illuminated by a unique waveform. The monostatic formulation given above is mathematically identical to the MAPC formulation. Hence, using the MAPC formulation and solution, the SPI algorithm is above to accurately estimate each of the “range profiles”, thereby producing an estimate of the two-dimensional range-Doppler profile. By measuring both range and Doppler information of multiple targets using a single pulse, it is possible to produce focused radar images without the use of complicated motion compensation techniques. Note, however, that the Doppler resolution is limited by the length of the pulse and therefore SPI is intended for fast-moving targets such as aircraft or missles, e.g. for targets moving at speeds above Mach 2 for a W-band radar.
The initial processing stage for the SPI algorithm consists of a bank of Doppler phase-shifted versions of the standard matched filter. The phase shifted versions of the matched filter partitions the Doppler space such that regardless of the Doppler shift induced by target motion, the radar return will match closely to at least one of the waveforms in the receiver. In order to facilitate the greatest Doppler resolution, a waveform with a thumbtack type ambiguity function is used for the transmitted waveform. A thumbtack ambiguity diagram is shown in
Were one to use standard matched filtering alone, the range profile for the kth Doppler shift could be estimated as
{circumflex over (x)}MF,k(λ.)={tilde over (s)}kHy(λ). (9)
where (□)H is the Hermitian operation (note that this is also the first stage of the SPI algorithm). In addition to the problems due to high range sidelobes, the matched filters are unable to accurately distinguish between targets based on their Doppler shifts, as will be shown below. To overcome the issues associated with traditional matched filtering, in subsequent stages of the SPI algorithm the bank of matched filters, sk in (9), is replaced by a bank of range/Doppler-dependent adaptive RMMSE-based filters. To produce an estimate of the received range profile associated with Doppler, an MMSE cost function is minimized for each range/Doppler cell as
Jk(λ)=E[|xk(λ)−wkH(λ)y(λ)|2]. (10)
where wk(λ) is the APC weight vector for the λth range cell in the range profile with Doppler phase shift θk, and E[□] is the expectation operator. The solution to (10) takes the form
where {circumflex over (ρ)}k(λ)=|{circumflex over (x)}k(λ)|2 is the estimated power of xk(λ), R=E[v(λ)v(λ)H] is the noise covariance matrix, and the matrix
where
Estimates of the K Doppler-shifted range profiles, as well as knowledge of the noise covariance matrix R are required to form the APC weight vectors. Assuming the noise covariance is white Gaussian, R simplifies to σv2 IN, where σv2 is the noise power, and IN is the N×N identity matrix.
Initially, as no knowledge of the K range profiles is available, the estimated power can be set to unity, {circumflex over (ρ)}k(λ)=1, ∀k, λ, and the noise assumed to be negligible. Thus (11) and (12) reduce to
The filters of (13) are applied as in (9) with {tilde over (s)}k replaced by
from (11) in the following form
where α is a scalar, d is (N−1)×1, and Q is (N−1)×(N−1). From (12), the next contiguous range cell, the matrix
can be written as
where b is a scalar, g is (N−1)×1, and Q is the same matrix from (15). The similarity between (15) and (16) can be exploited as follows using the matrix inversion lemma. First, we apply the permutation matrix
in which IN−1 is the (N−1)×(N−1) identity matrix and 0N−1 is an (N−1)×1 vector of zeros, to obtain
If we define {tilde over (d)}T=[dT 0]T and {tilde over (g)}T=[gT 0]T, the matrix
can be written as
where eN=[0 . . . 0 1]T has length N. Given (19), it is straightforward to show using the matrix inversion lemma that
in which Γ=diag{1.1.(b−a)}, U=[({tilde over (g)}−{tilde over (d)}) eN eN], and V=[eN ({tilde over (g)}−{tilde over (d)}) eN]. Hence, given
computed at a given range cell.
for the next range cell can be efficiently determined without the need to re-compute the matrix inverse.
To discuss Doppler resolution we first introduce the term φ which represents the total Doppler phase shift over the length of the waveform (as opposed to the phase shift between successive received samples previously specified as θ). In terms of the bank of Doppler-shifted matched filters, it has been observed that two targets of equal power can be resolved on the basis of a single pulse when the phase difference over the length of the waveform (i.e. Δφ) between the two targets is 2π radians. In contrast, the Doppler resolution of the SPI algorithm under the same conditions has been found to be only π radians. Thus, SPI effectively achieves Doppler super-resolution that is a two-fold improvement over the nominal matched filter Doppler resolution. However, the trade-off for achieving this super-resolution as well as the suppression of range and Doppler sidelobes is that the approximation in (24) requires K to be sufficiently large to accurately represent all possible Doppler shifts present. Experimentation via simulation has shown that specifying the set of Doppler-shifted waveforms such that
between contiguous Doppler-shifted version of the transmit waveform provides sufficiently high representation in the Doppler domain. The need for Doppler over-sampling is a result of Doppler mismatch effects which, as discussed previously, fundamentally limit the suppression of sidelobes. Note, though, that large values of Δφ need not be included (relative to the particular application) as these may represent Doppler shifts which would not be expected to occur in practice.
Waveforms that produce “thumbtack” ambiguity function (see
The single pulse imaging (SPI) algorithm simultaneously measures the Doppler phase shifts of multiple moving targets while adaptively pulse compressing a received radar waveform on a single pulse basis. Multiple pulse imaging algorithms have problems accounting for scatterers moving out of their range cells during the imaging time, resulting in a smeared image. Because both range and Doppler measurements are made using only a single pulse, the need for complicated motion compensation algorithms to correct for blurring due to range migration and/or non-uniform rotation is mitigated. In addition, SPI has the ability to image very high speed targets. Unlike the MAPC algorithm referred to above SPI is applied monostatically, where Doppler-induced phase-shifted versions of the transmitted waveform are modeled as independent received waveforms. A unique range profile is estimated for each Doppler phase shift, resulting in a two-dimensional range-Doppler image. The use of APC techniques allow small scatterers to be identified, which would otherwise be masked by the sidelobes of nearby larger scatterers.
As an example, consider a simulated target scenario consisting of a large stationary scatterer surrounded by four smaller scatterers. Two of the smaller scatterers are stationary, located 7 range cells before and after the large scatterer. The other two small scatterers are in the same range cell as the large scatterer, but possess Doppler phase shifts over the length of the waveform of φ=±2.75π (analogous to a Mach 2 scatterer illuminated by a 3.5-μs pulse at W-band). The transmitted waveform is a length N=30 random phase waveform. The signal-to-noise ratio (SNR) of the large target is 60 dB, and the small targets are 20 dB lower than the large target. The Doppler shifts of the smaller targets are analogous to Mach 2 targets illuminated by a 3.5 μs pulse at W-band. The output of a bank of matched filters is shown in
Obviously many modifications and variations of the present invention are possible in the light of the above teachings. It is therefore to be understood that the scope of the invention should be determined by referring to the following appended claims.
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