 Research Article
 Open Access
 Published:
Sequential Monte Carlo Methods for Joint Detection and Tracking of Multiaspect Targets in Infrared Radar Images
EURASIP Journal on Advances in Signal Processing volume 2008, Article number: 217373 (2007)
Abstract
We present in this paper a sequential Monte Carlo methodology for joint detection and tracking of a multiaspect target in image sequences. Unlike the traditional contact/association approach found in the literature, the proposed methodology enables integrated, multiframe target detection and tracking incorporating the statistical models for target aspect, target motion, and background clutter. Two implementations of the proposed algorithm are discussed using, respectively, a resamplemove (RS) particle filter and an auxiliary particle filter (APF). Our simulation results suggest that the APF configuration outperforms slightly the RS filter in scenarios of stealthy targets.
1. Introduction
This paper investigates the use of sequential Monte Carlo filters [1] for joint multiframe detection and tracking of randomly changing multiaspect targets in a sequence of heavily cluttered remote sensing images generated by an infrared airborne radar (IRAR) [2]. For simplicity, we restrict the discussion primarily to a single target scenario and indicate briefly how the proposed algorithms could be modified for multiobject tracking.
Most conventional approaches to target tracking in images [3] are based on suboptimal decoupling of the detection and tracking tasks. Given a reference target template, a twodimensional (2D) spatial matched filter is applied to a singleframe of the image sequence. The pixel locations where the output of the matched filter exceeds a prespecified threshold are treated then as initial estimates of the true position of detected targets. Those preliminary position estimates are subsequently assimilated into a multiframe tracking algorithm, usually a linearized Kalman filter, or alternatively discarded as false alarms originating from clutter.
Depending on its level of sophistication, the spatial matched filter design might or might not take into account the spatial correlation of the background clutter and random distortions of the true target aspect compared to the reference template. In any case, however, in a scenario with dim targets in heavily cluttered environments, the suboptimal association of a singleframe matched filter detector and a multiframe linearized tracking filter is bound to perform poorly [4].
As an alternative to the conventional approaches, we introduced in [5, 6] a Bayesian algorithm for joint multiframe detection and tracking of known targets, fully incorporating the statistical models for target motion and background clutter and overcoming the limitations of the usual association of singleframe correlation detectors and Kalman filter trackers in scenarios of stealthy targets. An improved version of the algorithm in [5, 6] was later introduced in [7] to enable joint detection and tracking of targets with unknown and randomly changing aspect. The algorithms in [5–7] were however limited by the need to use discretevalued stochastic models for both target motion and target aspect changes, with the "absent target" hypothesis treated as an additional dummy aspect state. A conventional hidden Markov model (HMM) filter was used then to perform joint minimum probability of error multiframe detection and maximum a posteriori (MAP) tracking for targets that were declared present in each frame. A smoothing version of the joint multiframe HMM detector/tracker, based essentially on a 2D version of the forwardbackward (BaumWelch) algorithm, was later proposed in [4]. Furthermore, we also proposed in [4] an alternative tracker based on particle filtering [1, 8] which, contrary to the original HMM tracker in [7], assumed a continuousvalued kinematic (position and velocity) state and a discretevalued target aspect state. However, the particle filter algorithm in [4] enabled tracking only (assuming that the target was always present in all frames) and used decoupled statistically independent models for target motion and target aspect.
To better capture target motion, we drop in this paper the previous constraint in [5–7] and, as in the later sections of [4], allow the unknown 2D position and velocity of the target to be continuousvalued random variables. The unknown target aspect is still modeled however as a discrete random variable defined on a finite set , where each symbol is a pointer to a possibly rotated, scaled, and/or sheared version of the target's reference template. In order to integrate detection and tracking, building on our previous HMM work in [7], we extend the set to include an additional dummy state that represents the absence of a target of interest in the scene. The evolution over time of the target's kinematic and aspect states is described then by a coupled stochastic dynamic model where the sequences of target positions, velocities, and aspects are mutually dependent.
Contrary to alternative featurebased trackers in the literature, the proposed algorithm in this paper detects and tracks the target directly from the raw sensor images, processing pixel intensities only. The clutterfree target image is modeled by a nonlinear function that maps a given target centroid position into a spatial distribution of pixels centered around the (quantized) centroid position, with shape and intensity being dependent on the current target aspect. Finally, the target is superimposed to a structured background whose spatial correlation is captured by a noncausal GaussMarkov random field (GMRf) model [9–11]. The GMRf model parameters are adaptively estimated from the observed data using an approximate maximum likelihood (AML) algorithm [12].
Given the problem setup described in the previous pa ragraph, the optimal solution to the integrated detection/ tracking problem requires the recursive computation at each frame of the joint posterior distribution of the target's kinematic and aspect states conditioned on all observed frames from instant up to instant . Given, however, the inherent nonlinearity of the observation and (possibly) motion models, the exact computation of that posterior distribution is generally not possible. We resort then to mixedstate particle filtering [13] to represent the joint posterior by a set of weighted samples (or particles) such that, as the number of particles goes to infinity, their weighted average converges (in some statistical sense) to the desired minimum meansquare error (MMSE) estimate of the hidden states. Following a sequential importance sampling (SIS) [14] approach, the particles may be drawn recursively from the coupled prior statistical model for target motion and aspect, while their respective weights may be updated recursively using a likelihood function that takes into account the models for the target's signature and for the background clutter.
We propose two different implementations for the mixedstate particle filter detector/tracker. The first implementation, which was previously discussed in a conference paper (see [15]) is a resamplemove (RS) filter [16] that uses particle resampling [17] followed by a MetropolisHastings move step [18] to combat both particle degeneracy and particle impoverishment (see [8]). The second implementation, which was not included in [15], is an auxiliary particle filter (APF) [19] that uses the current observed frame at instant to preselect those particles at instant which, when propagated through the prior dynamic model, are more likely to generate new samples with high likelihood. Both algorithms are original with respect to the previous particle filteringbased tracking algorithm that we proposed in [4], where the problem of joint detection and tracking with coupled motion and aspect models was not considered.
Related Work and Different Approaches in the Literature
Following the seminal work by Isard and Blake [20], particle filters have been extensively applied to the solution of visual tracking problems. In [21], a sequential Monte Carlo algorithm is proposed to track an object in video subject to model uncertainty. The target's aspect, although unknown, is assumed, however, to be fixed in [21], with no dynamic aspect change. On the other hand, in [22], an adaptive appearance model is used to specify a timevarying likelihood function expressed as a Gaussian mixture whose parameters are updated using the EM [23] algorithm. As in our work, the algorithm in [22] also processes image intensities directly, but, unlike our problem setup, the observation model in [22] does not incorporate any information about spatial correlation of image pixels, treating instead each pixel as independent observations. A different Bayesian algorithm for tracking nonrigid (randomly deformable) objects in threedimensional images using multiple conditionally independent cues is presented in [24]. Dynamic object appearance changes are captured by a mixedstate shape model [13] consisting of a discretevalued cluster membership parameter and a continuousvalued weight parameter. A separate kinematic model is used in turn to describe the temporal evolution of the object's position and velocity. Unlike our work, the kinematic model in [24] is assumed statistically independent of the aspect to model.
Rather than investigating solutions to the problem of multiaspect tracking of a single target, several recent references, for example, [25, 26], use mixture particle filters to tackle the different but related problem of detecting and tracking an unknown number of multiple objects with different but fixed appearance. The number of terms in the nonparametric mixture model, that represents the posterior of the unknowns, is adaptively changed as new objects are detected in the scene and initialized with a new associated observation model. Likewise, the mixture weights are also recursively updated from frame to frame in the image sequence.
Organization of the Paper
The paper is divided into 6 sections. Section 1 is this introduction. In Section 2, we present the coupled model for target aspect and motion and review the observation and clutter models focusing on the GMRf representation of the background and the derivation of the associated likelihood function for the observed (target + clutter) image. In Section 3, we detail the proposed detector/tracker in the RS and APF configurations. The performance of the two filters is discussed in Section 4 using simulated infrared airborne radar (IRAR) data. A preliminary discussion on multitarget tracking is found in Section 5, followed by an illustrative example with two targets. Finally, we present in Section 6 the conclusions of our work.
2. The Model
In the sequel, we present the target and clutter models that are used in this paper. We use lowercase letters to denote both random variables/vectors and realizations (samples) of random variables/vectors; the proper interpretation is implied in context. We use lowercase to denote probability density functions (pdfs) and uppercase to denote the probability mass functions (pmfs) of discrete random variables. The symbol is used to denote the probability of an event in the algebra of the sample space.
State Variables
Let be a nonnegative integer number and let superscript denote the transpose of a vector or matrix. The kinematic state of the target at frame is defined as the fourdimensional continuous (realvalued) random vector that collects the positions, and , and the velocities, and , of the target's centroid in a system of 2D Cartesian coordinates . On the other hand, the target's aspect state at frame , denoted by , is assumed to be a discrete random variable that takes values in the finite set where the symbol "" is a dummy state that denotes that the target is absent at frame , and each symbol , , is in turn a pointer to one possibly rotated, scaled, and/or sheared version of the target's reference template.
2.1. Target Motion and Aspect Models
The random sequence , is modeled as firstorder Markov process specified by the pdf of the initial kinematic state , the transition pdf , the transition probabilities , , and the initial probabilities , .
Aspect Change Model
Assume that, at any given frame, for any aspect state , the clutterfree target image lies within a bounded rectangle of size . In this notation, and denote the maximum pixel distances in the target image when we move away, respectively, up and down, from the target centroid. Analogously, and are the maximum horizontal pixel distances in the target image when we move away, respectively, left and right, from the target centroid.
Assume also that each image frame has the size of pixels. We introduce next the extended grid that contains all possible target centroid locations for which at least one target pixel still lies in the sensor image. Next, let be a matrix of size such that for any and
Assuming that a transition from a "present target" state to the "absent target" state can only occur when the target moves out of the image, we model the probability of a change in the target's aspect from the state to the state , , as
where the twodimensional vector denotes the quantized target centroid position defined on the extended image grid and obtained from the fourdimensional continuous kinematic state by making
where and are the spatial resolutions of the image, respectively, in the directions and . The parameter in (2) denotes in turn the probability of a new target entering the image once the previous target became absent. For simplicity, we restrict the discussion in this paper to the situation where there is at most one single target of interest present in the scene at each image frame. The specification , , corresponds to assuming the worstcase scenario where, given that a new target entered the scene, there is a uniform probability that the target will take any of the possible aspect states. Finally, the term in (2) is the probability of a target moving out of the image at frame given its kinematic and aspect states at frame .
Motion Model
For simplicity, we assume that, except in the situation where there is a transition from the "absent target" state to the "present target" state, the conditional pdf is independent of the current and previous aspect states, respectively, and . In other words, unless and , we make
where is an arbitrary pdf (not necessarily Gaussian) that models the target motion. Otherwise, if and , we reset the target's position and make
where is typically a noninformative (e.g., uniform) prior pdf defined in a certain region (e.g., upperleft corner) of the image grid. Given the independence assumption in (4), it follows that, for any
2.2. Observation Model and Likelihood Function
Next, we discuss the target observation model. Previous references mentioned in Section 1, for example, [21, 22, 24–26], are concerned mostly with video surveillance of near objects (e.g., pedestrian or vehicle tracking), or other similar applications (e.g., face tracking in video). For that class of applications, effects such as object occlusion are important and must be explicitly incorporated into the target observation model. In this paper by contrast, the emphasis is on a different application, namely, detection and tracking of small, quasipoint targets that are observed by remote sensors (usually midto highaltitude airborne platforms) and move in highly structured, generally smooth backgrounds (e.g., deserts, snowcovered fields, or other forms of terrain). Rather than modeling occlusion, our emphasis is instead on additive natural clutter.
Image Frame Model
Assuming a single target scenario, the th frame in the image sequence is modeled as the matrix:
where the matrix represents the background clutter and is a nonlinear function that maps the quantized target centroid position, , (see (3)) into a spatial distribution of pixels centered at and specified by a set of deterministic and known target signature coefficients dependent on the aspect state . Specifically, we make [4]
where is an matrix whose entries are all equal to zero, except for the element which is equal to 1.
For a given fixed template model , the coefficients in (8) are the target signature coefficients responding to that particular template. The signature coefficients are the product of a binary parameter , that defines the target shape for each aspect state, and a real coefficient , that specifies the pixel intensities of the target, again for the various states in the alphabet . For simplicity, we assume that the pixel intensities and shapes are deterministic and known at each frame for each possible value of . In particular, if takes the value denoting absence of target, then the function in (7) reduces to the identically zero matrix, indicating that sensor observations consist of clutter only.
Remark. Equation (8) assumes that the target's template is entirely located within the sensor image grid. Otherwise, for targets that are close to the image borders, the summation limits in (8) must be changed accordingly to take into account portions of the target that are no longer visible.
Clutter Model
In order to describe the spatial correlation of the background clutter, we assume that, after suitable preprocessing to remove the local means, the random field , , , is modeled as a firstorder noncausal GaussMarkov random field (GMrf) described by the finite difference equation [9]
where , with if and zero otherwise. The symbol denotes here the expectation (or expected value) of a random variable/vector.
Likelihood Function Model
Let , , and be the onedimensional equivalent representations, respectively, of , and in (7), obtained by rowlexicographic ordering. Let also denote the covariance matrix associated with the random vector , assumed to have zero mean after appropriate preprocessing. For a GMrf model as in (9), the corresponding likelihood function for a fixed aspect state , , is given by [4]
where
is referred to in our work as the data term and
is called the energy term. On the other hand, for , reduces to the likelihood of the absent target state, which corresponds to the probability density function of assuming that the observation consists of clutter only, that is,
Writing the difference equation (9) in compact matrix notation, it can be shown [9–11] by the application of the principle of orthogonality that has a blocktridiagonal structure of the form
where denotes the Kronecker product, is identity matrix, and is a matrix whose entries if and are equal to zero otherwise.
Using the blockbanded structure of in (14), it can be further shown that may be evaluated as the output of a modified 2D spatial matched filter using the expression
where , , are obtained, from (3), and is the output of a 2D differential operator
with Dirichlet (identically zero) boundary conditions.
Similarly, the energy term can be also efficiently computed by exploring the blockbanded structure of . The resulting expression is the difference between the autocorrelation of the signature coefficients and their lagone crosscorrelations weighted by the respective GMrf model parameters or . Before we leave this section, we make two additional remarks.
Remark 2.
As before, (15) is valid for and . For centroid positions close to the image borders, the summation limits in (15) must be varied accordingly (see [6] for details).
Remark 3.
Within our framework, a crude nonBayesian single frame maximum likelihood target detector could be built by simply evaluating the likelihood map for each aspect state and finding the maximum over the image grid of the sum of likelihood maps weighted by the a priori probability for each state (usually assumed to be identical). A target would be considered present then if the weighted likelihood peak exceeded a certain threshold. In that case, the likelihood peak would also provide an estimate for the target location. The integrated joint detector/tracker presented in Section 3 outperforms, however, the decoupled singleframe detector discussed in this remark by fully incorporating the dynamic motion and aspect motion into the detection process and enabling multiframe detection within the context of a trackbeforedetect philosophy.
3. Particle Filter Detector/Tracker
3.1. Sequential Importance Sampling
Given a sequence of observed frames , our goal is to generate, at each instant , a properly weighted set of samples (or particles) , , with associated weights such that, according to some statistical criterion, as goes to infinity,
A possible mixedstate sequential importance sampling (SIS) strategy (see [4, 13]) for the recursive generation of the particles and their proper weights is described in the algorithm below.

(1)
Initialization For

(i)
Draw , and .

(ii)
Make and .

(i)

(2)
Importance Sampling For

(i)
Draw according to (2).

(ii)
Draw according to (4) or (5).

(iii)
Update the importance weights
(18)
using the likelihood function in Section 2.2.

(i)
EndFor

(i)
Normalize the weights such that .

(ii)
For , make , , and .

(iii)
Make and go back to step 2.
3.2. ResampleMove Filter
The sequential importance sampling algorithm in Section 3.1 is guaranteed to converge asymptotically with probability one; see [27]. However, due to the increase in the variance of the importance weights, the raw SIS algorithm suffers from the "particle degeneracy" phenomenon [8, 14, 17]; that is, after a few steps, only a small number of particles will have normalized weights close to one, whereas the majority of the particles will have negligible weight. As a result of particle degeneracy, the SIS algorithm is inefficient, requiring the use of a large number of particles to achieve adequate performance.
Resampling Step
A possible approach to mitigate degeneracy is [17] to resample from the existing particle population with replacement according to the particle weights. Formally, after the normalization of importance weights , we draw with , and build a new particle set , , such that After the resampling step, the new selected trajectories are approximately distributed (see, e.g., [28]) according to the mixed posterior pdf so that we can reset all particle weights to .
Move Step
Although particle resampling according to the weights reduces particle degeneracy, it also introduces an undesirable side effect, namely, loss of diversity in the particle population as the resampling processes generate multiple copies of a small number or, in the extreme case, only one highweight particle. A possible solution, see [16], to restore sample diversity without altering the sample statistics is to move the current particles to new locations using a Markov chain transition kernel , that is, invariant to the conditional mixture pdf . Provided that the invariance condition is satisfied, the new particle trajectories remain distributed according to and the associated particle weights may be kept equal to . A Markov chain that satisfies the desired invariance condition can be built using the following MetropolisHastings strategy [15, 18].
For , the following algorithm holds.

(i)
Draw according to (2).

(ii)
Draw according to (4) or (5).

(iii)
Draw If
(19)then
(20)Else,
(21) 
(iv)
Reset .
EndFor.
3.3. Auxiliary Particle Filter
An alternative to the resamplemove filter in Section 3.2 is to use the current observation to preselect at instant a set of particles that, when propagated to instant according to the system dynamics, is more likely to generate samples with high likelihood. That can be done using an auxiliary particle filter (APF) [19] which samples in two steps from a mixed importance function:
where and are drawn according to the mixed prior . The proposed algorithm is summarized into the following steps.

(1)
Presampling Selection Step For

(i)
Draw according to (2).

(ii)
Draw according to (4) or (5).

(iii)
Compute the firststage importance weights
(23)
using the likelihood function model in Section 2.2.

(i)
EndFor

(2)
Importance Sampling with Auxiliary Particles For

(i)
Sample with .

(ii)
Sample according to (2).

(iii)
Sample according to (4) or (5).

(iv)
Compute the secondstage importance weights
(24)EndFor.

(v)
Normalize the weights such that .

(i)

(3)
Postsampling Selection Step For

(i)
Draw with .

(ii)
Make and .
EndFor.

(iii)
Make and go back to step 1.

(i)
3.4. Multiframe Detector/Tracker
The final result at instant of either the RS algorithm in Section 3.2 or the APF algorithm in Section 3.3 is a set of equally weighted samples that are approximately distributed according to the mixed posterior . Next, let denote the hypothesis that the target of interest is present in the scene at frame . Conversely, let denote the hypothesis that the target is absent. Given the equally weighted set , we compute then the Monte Carlo estimate, , of the posterior probability of target absence by dividing the number of particles for which by the total number of particles . The minimum probability of error test to decide between hypotheses and at frame is approximated then by the decision rule
or, equivalently,
Finally, if is accepted, the estimate of the target's kinematic state at instant is obtained from the Monte Carlo approximation of , which is computed by averaging out the particles such that .
4. Simulation Results
In this section, we quantify the performance of the proposed sequential Monte Carlo detector/tracker, both in the RS and APF configurations, using simulated infrared airborne radar (IRAR) data. The background clutter is simulated from real IRAR images from the MIT Lincoln Laboratory database, available at the CIS website, at Johns Hopkins University. An artificial target template representing a military vehicle is added to the simulated image sequence. The simulated target's centroid moves in the image from frame to frame according to the simple whitenoise acceleration model in [3, 4] with parameters and second. A total of four rotated, scaled, or sheared versions of the reference template is used in the simulation.
The target's aspect changes from frame to frame following a known discretevalued hidden Markov chain model where the probability of a transition to an adjacent aspect state is equal to 40%. In the notation of Section 2.1, that specification corresponds to setting , , if , and otherwise. All four templates are equally likely at frame zero, that is, for . The initial and positions of the target's centroid at instant zero are assumed to be uniformly distributed, respectively, between pixels 50 and 70 in the coordinate and pixels 10 and 20 in the coordinate. The initial velocities and are in turn Gaussiandistributed with identical means ( or pixels/frame) and a small standard deviation ().
Finally, the background clutter for the moving target sequence was simulated by adding a sequence of synthetic GMrf samples to a matrix of previously stored local means extracted from the database imagery. The GMrf samples were synthetized using correlation and prediction error variance parameters estimated from real data using the algorithms developed in [11, 12] see [4] for a detailed pseudocode.
Two video demonstrations of the operation of the proposed detector/tracker are available for visualization by clicking on the links in [29]. The first video (peak targettoclutter ratio, or PTCR ≈ 10 dB) illustrates the performance over 50 frames of an 8 000particle RS detector/tracker implemented as in Section 3.2, whereas the second video (PTCR ≈ 6.5 dB) demonstrates the operation over 60 frames of a 5 000particle APF detector/tracker implemented as in Section 3.3. Both video sequences show a target of interest that is tracked inside the image grid until it disappears from the scene; the algorithm then detects that the target is absent and correctly indicates that no target is present. Next, once a new target enters the scene, that target is acquired and tracked accurately until, in the case of the APF demonstration, it leaves the scene and no target detection is once again correctly indicated.
Both video demos show the ability of the proposed algorithms to (1) detect and track a present target both inside the image grid and near its borders, (2) detect when a target leaves the image and indicate that there is no target present until a new target appears and (3), when a new target enters the scene, correctly detect that the target is present and track it accurately. In the sequel, for illustrative purposes only, we show in the paper the detection/tracking results for a few selected frames using the RS algorithm and a dataset that is different from the one shown in the video demos.
Figure 1(a) shows the initial frame of the sequence with the target centered in the (quantized) coordinates and superimposed on clutter. The clutterfree target template, centered at the same pixel location, is shown as a binary image in Figure 1(b). The simulated PTCR in Figure 1(b) is 10.6 dB.
Next, Figure 2(a) shows the tenth frame in the image sequence. Once again, we show in Figure 2(b) the corresponding clutterfree target image as a binary image. Note that the target from frame 1 has now undergone a random change in aspect in addition to translational motion.
The tracking results corresponding to frames 1 and 10 are shown, respectively, in Figures 3(a) and 3(b). The actual target positions are indicated by a cross sign ('+'), while the estimated positions are indicated by a circle ('o'). Note that the axes in Figures 1(a) and 1(b) and Figures 2(a) and 2(b) represent integer pixel locations, while the axes in Figures 3(a) and 3(b) represent realvalued and , coordinates assuming spatial resolutions of meters/pixel such that the pixel range in the axes of Figures 1(a) and 1(b) and Figures 2(a) and 2(b) corresponds to a meter range in the axes of Figures 3(a) and 3(b).
In this particular example, the target leaves the scene at frame 31 and no target reappears until frame 37. The SMC tracker accurately detects the instant when the target disappears and shows no false alarms over the 6 absent target frames as illustrated in Figures 4(a) and 4(b) where we show, respectively, the clutter+backgroundonly thirtysixth frame and the corresponding tracking results indicating in this case that no target has been detected. Finally, when a new target reappears, it is accurately acquired by the SMC algorithm. The final simulated frame with the new target at position is shown for illustration purposes in Figure 5(a). Figure 5(b) shows the corresponding tracking results for the same frame.
In order to obtain a quantitative assessment of tracking performance, we ran 100 independent Monte Carlo simulations using, respectively, the 5000particle APF detector/tracker and the 8000particle RS detector/tracker. Both algorithms correctly detected the presence of the target over a sequence of 20 simulated frames in all 100 Monte Carlo runs. However, with PTCR = 6.5 dB, the 5000particle APF tracker diverged (i.e., failed to estimate the correct target trajectory) in 3 out of the 100 Monte Carlo trials, whereas the RS tracker diverged in 5 out of 100 runs. When we increased the PTCR to 8.1 dB, the divergence rates fell to 2 out of 100 for the APF, and 3 out of 100 for the RS filter. Figures 6(a) and 6(b) show, in the case of PTCR = 6.5 dB, the root mean square (RMS) error curves (in number of pixels) for the target's position estimates, respectively, in coordinates and generated by both the APF and the RS trackers. The RMS error curves in Figure 6 were computed from the estimation errors recorded in each of the 100 Monte Carlo trials, excluding the divergent realizations. Our simulation results suggest that, despite the reduction in the number of particles from 8000 to 5000, the APF tracker still outperforms the RS tracker, showing similar RMS error performance with a slightly lower divergence rate. For both filters, in the nondivergent realizations, the estimation error is higher in the initial frames and decreases over time as the target is acquired and new images are processed.
5. Preliminary Discussion on Multitarget Tracking
We have considered so far a single target with uncertain aspect (e.g., random orientation or scale). In theory, however, the same modeling framework could be adapted to a scenario where we consider multiple targets with known (fixed) aspect. In that case, the discrete state , rather than representing a possible target model, could denote instead a possible multitarget configuration hypothesis. For example, if we knew a priori that there is a maximum of targets in the field of view of the sensor at each time instant, then would take possible values corresponding to the hypotheses ranging from "no target present" to "all targets present" in the image frame at instant . The kinematic state , on the other hand, would have variable dimension depending on the value assumed by , as it would collect the centroid locations of all targets that are present in the image given a certain target configuration hypothesis. Different targets could be assumed to move independently of each other when present and to disappear only when they move out of the target grid as discussed in Section 2. Likewise, a change in target configuration hypotheses would result in new targets appearing in uniformly random locations as in (5).
The main difficulty associated with the approach described in the previous paragraph is however that, as the number of targets increases, the corresponding growth in the dimension of the state space is likely to exacerbate particle depletion, thus causing the detection/tracking filters to diverge if the number of particles is kept constant. That may render the direct application of the joint detection/tracking algorithms in this paper unfeasible in a multitarget scenario. The basic tracking routines discussed in the paper may be still viable though when used in conjunction with more conventional algorithms for target detection/acquisition and data association. For a review of alternative approaches to multitarget tracking, mostly for video applications, we refer the reader to [30–33].
5.1. Likelihood Function Modification in a Multitarget Scenario
In the alternative scenario with multiple (at most ) targets, where represents one of possible target configurations, the likelihood function model in (10) depends instead on a sum of data terms
and a sum of energy terms
where is the longvector representation of the clutterfree image of the th target under the target configuration hypothesis , assumed to be identically zero for target configurations under which the th target is not present. The sum of the data terms corresponds to the sum of the outputs of different correlation filters matched to each of the possible (fixed) target templates taking into account the spatial correlation of the clutter background. The energy terms, , are on the other hand constant with for most possible locations of targets and on the image grid, except when either one of the two targets or both are close to the image borders. Finally, for , the energy terms are zero for present targets that are sufficiently apart from each other and, therefore, most of the time, they do not affect the computation of the likelihood function. The terms must be taken into account, however, for overlapping targets; in this case, they may be computed efficiently exploring the sparse structure of and . For details, we refer the reader to future work.
5.2. Illustrative Example with Two Targets
We conclude this preliminary discussion on multitarget tracking with an illustrative example where we track two simulated targets moving on the same real clutter background from Section 4 for 22 consecutive frames. This example differs, however, from the simulations in Section 4 in the sense that, rather than performing joint detection and tracking of the two targets, the algorithm assumes a priori that two targets are always present in the scene and performs target tracking only. The two targets are preacquired (detected) in the initial frame such that their initial positions are known up only to a small uncertainty. For this particular simulation, with PTCR ≈ 12.5 dB, that preliminary acquisition was done by applying the differential filter in (16) to the initial frame, and then applying the output of the differential filter to a bank of two spatial matched filters as in (15), designed according to the signature coefficients, respectively, for targets 1 and 2. The outputs of the two matched filters minus the corresponding energy terms for targets 1 and 2, respectively, are finally added together and thresholded to provide the initial estimates of the location of the two targets. Note that the crossenergy terms discussed in Section 5.1 may be ignored in this case since we are assuming that the two targets are initially sufficiently far apart. Frames 1 and 10 of the simulated cluttered sequence with the two targets are shown in Figures 7(a) and 7(b) for illustration purposes.
Once the two targets are initially acquired, we track them jointly from the raw sensor images (i.e., without any other conventional decoupled data association/tracking method) using an auxiliary particle filter that assumes the modified likelihood function of Section 5.1 and two independent motion models, respectively, for targets 1 and 2. The tracking filter uses particles. Figure 8 shows the actual and estimated trajectories, respectively, for targets 1 and 2. As we can see from the plots, the experimental results are worse than those obtained in the single target, multiaspect case, but the filter was still capable of tracking the pixel locations of the centroids of the two targets fairly accurately with errors ranging from zero to two or three pixels at most and without using any ad hoc data association routine.
6. Conclusions and Future Work
We discussed in this paper a methodology for joint detection and tracking of multiaspect targets in remote sensing image sequences using sequential Monte Carlo (SMC) filters. The proposed algorithm enables integrated, multiframe target detection and tracking incorporating the statistical models for target motion, target aspect, and spatial correlation of the background clutter. Due to the nature of the application, the emphasis is on detecting and tracking small, remote targets under additive clutter, as opposed to tracking nearby objects possibly subject to occlusion.
Two different implementations of the SMC detector/tracker were presented using, respectively, a resamplemove (RS) particle filter and an auxiliary particle filter (APF). Simulation results show that, in scenarios with heavily obscured targets, the APF and RS configurations have similar tracking performance, but the APF algorithm has a slightly smaller percentage of divergent realizations. Both filters, on the other hand, were capable of correctly detecting the target in each frame, including accurately declaring absence of target when the target left the scene and, conversely, detecting a new target when it entered the image grid. The multiframe trackbeforedetect approach allowed for efficient detection of dim targets that may be near invisible in a singleframe but become detectable when seen across multiple frames.
The discussion in this paper was restricted to targets that assume only a finite number of possible aspect states defined on a library of target templates. As an alternative for future work, an appearance model similar to the one described in [24] could be used instead, allowing the discretevalued aspect states to denote different classes of continuousvalued target deformation models, as opposed to fixed target templates. Similarly, the framework in this paper could also be modified to allow for multiobject tracking as indicated in Section 5.
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Part of the material in this paper was presented at the 2005 IEEE Aerospace Conference.
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Bruno, M.G.S., Araújo, R.V. & Pavlov, A.G. Sequential Monte Carlo Methods for Joint Detection and Tracking of Multiaspect Targets in Infrared Radar Images. EURASIP J. Adv. Signal Process. 2008, 217373 (2007). https://doi.org/10.1155/2008/217373
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DOI: https://doi.org/10.1155/2008/217373
Keywords
 Target Motion
 Sequential Monte Carlo
 Background Clutter
 Joint Detection
 Image Grid