Maneuvering Target Tracking in the Presence of Glint using the Nonlinear Gaussian Mixture Kalman Fil-xq4.pdf

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I. INTRODUCTION
Maneuvering Target Tracking in
thePresenceofGlintusingthe
Nonlinear Gaussian Mixture
Kalman Filter
Target tracking is a basic problem in radar, sonar,
and infrared applications. Since 1960 several methods
[1—2] have been proposed to solve the tracking
problem. The dynamic state-space (DSS) modeling
approach is widely used in radar target tracking. In
the DSS approach, the time-varying dynamics of
an unobserved state are characterized by the state
vector. It is usually assumed that the system state
is a first-order Markov process [3]. The Bayesian
approach provides a general framework for dynamic
state estimation. The Kalman filter (KF), which is
optimal in the minimum-mean-square error (MMSE)
sense for linear, Gaussian systems, is the most popular
tracking algorithm [4, 5].
Target tracking in practical radar systems is
nonlinear and non-Gaussian. The nonlinearity
behavior is due to the fact that the target dynamics
are usually modeled in Cartesian coordinates, while
the observation model is in polar coordinates.
There is no general analytic expression for the
posterior probability density function (pdf) in
nonlinear problems, and only approximated estimation
algorithms have been studied [6]. The extended
Kalman filter (EKF) is the most popular approach
for recursive nonlinear estimation [4, 7]. The main
idea of the EKF is based on a first-order linearization
of the model where the posterior pdf and the system
and measurement noises are assumed to be Gaussian.
The nonlinearity of the measurement model leads
to a non-Gaussian, multi-modal pdf of the system
state even when the system and the measurement
noise are Gaussian. The Gaussian approximation of
this multi-modal distribution leads to poor tracking
performance. The unscented Kalman filter (UKF)
approximates the pdf at the output of the nonlinear
transformation using deterministic sampling [8—10].
The advantage of the UKF over the EKF stems from
the fact that it does not involve approximation of the
nonlinear model per se [11, 12]. The UKF provides
an unbiased estimate; however, its convergence is
slow [12].
The Singer model [13] is widely used in
maneuvering target tracking applications. In this
model, the target acceleration is assumed to be a
zero-mean, first-order Markov process. Maneuvering
targets are characterized by changes of acceleration
due to sudden breaking or steering [14]. Usually, a
heavy-tailed distribution is used to model the abrupt
changes of the system state in maneuvering target
tracking applications [14].
In radar systems, changes in the target aspect
toward the radar may cause irregular electromagnetic
wave reflections, resulting in significant variations
of radar reflections [15]. This phenomenon gives
rise to outliers in angle tracking, and it is referred
to as target glint. The concept of angular glint was
I. BILIK, Member, IEEE
University of Massachusetts, Dartmouth
J. TABRIKIAN, Senior Member, IEEE
Ben-Gurion University of the Negev
Beer-Sheva, Israel
The problem of maneuvering target tracking in the presence
of glint noise is addressed in this work. The main challenge in this
problem stems from its nonlinearity and non-Gaussianity. A new
estimator, named as nonlinear Gaussian mixture Kalman filter
(NL-GMKF) is derived based on the minimum-mean-square error
(MMSE) criterion and applied to the problem of maneuvering
target tracking in the presence of glint. The tracking performance
of the NL-GMKF is evaluated and compared with the interacting
multiple modeling (IMM) implemented with extended Kalman
filter (EKF), unscented Kalman filter (UKF), particle filter
(PF) and the Gaussian sum PF (GSPF). It is shown that the
NL-GMKF outperforms these algorithms in several examples with
maneuvering target and/or glint noise measurements.
Manuscript received December 20, 2006; revised January 30, May
16, August 8, and September 10, 2008; released for publication
October 3, 2008.
IEEE Log No. T-AES/46/1/935940.
Refereeing of this contribution was handled by W. Koch.
Author’s addresses: I. Bilik, Dept. of Electrical and Computer
Engineering, University of Massachusetts, Dartmouth, MA;
J. Tabrikian, Dept. of ECE, Ben-Gurion University of the Negev,
ECE, Beer-Sheva, 84105, Israel, E-mail: (joseph@ee.bgu.ac.il).
0018-9251/10/$26.00 ° 2010 IEEE
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initially proposed in [16] and was explained as the tilt
of wave-front normal, resulting from the distortion of
target echo signal phase. It was found that glint has a
long-tailed pdf [15]. The statistical characteristics of
the glint noise and its mathematical models have been
studied in [15], [17], and [18]. The glint has been
modeled by the student’s t distribution in [18], based
on theoretical studies. In [17], the glint noise was
alternatively modeled by a mixture of a zero-mean,
small-variance Gaussian and a heavy-tailed Laplacian.
The Gaussian mixture model (GMM) with two
mixture components is widely used in the literature
for heavy-tailed, non-Gaussian pdfs. This model
consists of one small-variance Gaussian with high
probability and one large-variance Gaussian with low
probability of occurrence. The GMM is commonly
used to cope with abrupt changes of the system state
and glint noise modeling [15, 19].
Many researchers have addressed the problem
of filtering in non-Gaussian models. One of the
effective algorithms in the non-Gaussian problems is
the Masreliez filter [20, 21] that employs a nonlinear
“score-function,” calculated from known a priori
noise statistics. The score-function is customized for
the noise statistics and has to be redesigned for each
application. The main disadvantage of this approach
is that it involves a computationally expensive score
function calculation [17]. In [22], the Masreliez filter
was used in the target tracking problem with glint
noise.
Recently, a few filtering approaches have been
proposed. One of them is the multiple modeling
(MM) approach, in which the time-varying motion
of the maneuvering target is described by multiple
models [23]. In this approach, the non-Gaussian
system is represented by a mixture of parallel
Gaussian-distributed modes [4]. Using the Bayesian
framework, the posterior pdf of the system state
is obtained as a mixture of conditional estimates
with a priori probabilities of each mode [1].
Various filters are used for mode-conditioned state
estimation. For example, the Gaussian sum filter
(GSF) was implemented in [4], [24] using a bank
of KFs. The EKF and Masreliez filters were used as
mode-conditioned filters for the nonlinear problems of
target tracking in [17], [22], [25]. The main drawback
of the MM approach is the exponential growth of the
number of the modes, and exponentially increasing
number of mode-conditioned filters [1, 26]. Therefore,
optimal algorithms such as the GSF are impractical.
Suboptimal techniques for model order reduction
based on merging and pruning were summarized
in [26]. The generalized pseudo-Bayesian (GPB)
merging algorithm combines modes with similar
recent histories that differ mainly in old time instances
[1, 27]. A suboptimal, computationally-efficient
interacting MM (IMM) algorithm was successfully
applied to the maneuvering target tracking problem
[1, 28, 29]. In [19], [22], [25] the IMM algorithm
with EKFs and Masreliez filters were implemented for
maneuvering target tracking in the presence of glint
noise. The IMM algorithm with a greater number of
modes was proposed in [30] for non-Gaussian system
and measurement noises.
Another class of filtering algorithms is based
on the sequential Monte Carlo (MC) approach. The
sequential importance sampling technique forms
the basis for most MC techniques [31], in which
the filtering is performed recursively generating
MC samples of the state variables. These methods
are often very flexible in non-Gaussian problems
due to the nature of the MC simulations [32]. One
of the popular techniques of this approach is the
particle filter (PF), which is a suboptimal estimator
that approximates the posterior distribution by a
set of random samples with associated weights.
The PF models the state posterior distribution
using discrete random samples rather than using an
analytic model [33]. The Gaussian sum particle filter
(GSPF) [34] implements the PF assuming Gaussian
mixture distributions for the system noise. The GSPF
introduces a new model order reduction method based
on the importance resampling method. Thus, the
model order of the state vector posterior pdf remains
constant over iterations, discarding mixands with
small weights.
The PF has been extensively used for maneuvering
target tracking (e.g., [14]). In [35] the PF was applied
to the problem of tracking in glint noise environment.
As shown in [36] and [37], the PF outperforms the
IMM algorithm when the likelihood function is
multi-modal. Different application-driven PFs are
presented in the literature, but there is no precise
rule about which type of PF should be used in each
application. This implies that no rigorous PF exists,
which is one of the disadvantages of the PF approach.
A recursive estimator, denoted as Gaussian mixture
KF (GMKF), for linear non-Gaussian problems was
derived in [38], [39]. The main idea of the GMKF
is that any pdf can be closely approximated by a
mixture of a finite number of Gaussians [40]. The
GMKF is based on the GSF, where the problem of
exponential model order growth was solved using
a greedy expectation-maximization (EM)-based
method. In [38], [39], it was shown that the GMKF
outperforms the PF, the IMM-KF, and the GSPF in
linear non-Gaussian problems.
This work addresses the nonlinear and
non-Gaussian problem of maneuvering target tracking
in the presence of non-Gaussian glint noise. A
recursive algorithm named as nonlinear GMKF
(NL-GMKF), which extends the GMKF to nonlinear
models, is derived based on the MMSE criterion.
The proposed NL-GMKF considers the case of
non-Gaussian system and measurement noises as
well as the non-Gaussian posterior pdf of the state
BILIK & TABRIKIAN: MANEUVERING TARGET TRACKING IN THE PRESENCE OF GLINT
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vector. The NL-GMKF differs from the GSPF [34]
and the mixture Kalman filter (MKF) [32] in the
following aspects. First, the NL-GMKF assumes
general non-Gaussian distributions for the system and
measurement noises, rather than GMM distributions.
Second, in the NL-GMKF, the posterior distribution
of the state vector is modeled by GMM whose
parameters are determined to minimize its estimated
Kullback-Leibler divergence (KLD) from the “true”
distribution, while in the GSPF and the MKF, the
GMM parameters are determined by resampling,
which throws out mixands with insignificant weights.
Usually, the parameters of the mixture model are
estimated via the EM algorithm. The performance
of this algorithm depends on its initialization, due
to its tendency to converge to local maxima. An
elegant solution for the initialization problem is
provided by the greedy learning of GMM [41], which
is implemented in this work.
The expected significance of the proposed
NL-GMKF is in practical applications of low
to moderate maneuvering target tracking, when
maneuver detection is difficult. The advantage
of the NL-GMKF over other tracking algorithms
is significant especially in the presence of glint
measurement noise with small probability of detection
and high significance. The correlation between
the statistics of glint noise and maneuver (that
characterizes a maneuvering target consisting of
multiple scattering centers) makes the problem
of maneuvering target tracking in the presence
of glint noise extremely challenging due to the
difficulty of maneuver and glint detection and filtering
simultaneously. The proposed NL-GMKF does not
require prior knowledge of the target dynamics
such as coordinated turn model; therefore, it might
be useful when tracking targets with complicated
maneuvering profile that cannot be modeled by a
finite set of simple dynamic models.
The paper is organized as follows: The NL-GMKF
is derived in Section II. The NL-GMKF computational
complexity is analyzed in Section III. The DSS
model for radar target tracking is stated in Section IV.
Estimation performances of the NL-GMKF for various
target tracking cases are evaluated in Section V. Our
conclusions are summarized in Section VI.
where the nonlinear transition function a ( ¢ , ¢ )and
the observation function h ( ¢ , ¢ )areassumedtobe
known. The system and measurement noises are
non-Gaussian with known pdfs. The driving noise
u [ n ] and the measurement noise w [ n ] are temporally
independent, i.e., u [ n ]and u [ n 0 ], and w [ n ]and w [ n 0 ]
are mutually independent for any time instances
n =0,1,2, ::: ; n 0 =0,1,2, ::: ; n6 = n 0 . The initial state
s [ ¡ 1], the driving noise u [ n ], and the measurement
noise w [ n ] are statistically independent. The initial
state distribution is modeled by
s [ ¡ 1] » GMM( ® s l [ ¡ 1], ¹ s l [ ¡ 1], ¡ s l [ ¡ 1]; l =1, ::: , L )
(3)
where GMM( ® y j , ¹ y j , ¡ y j , j =1, ::: , J ) denotes
a J th-order proper complex Gaussian mixture
distribution whose density function is given by
X
J
f y ( y )=
® y j © ( y ; ° y j )
( 4 )
j =1
where ® y j is the mixture weight, © ( y ; ° y j )isthe
j th mixture component, and ° y j contains the mean
vector ¹ y j , and the covariance matrix ¡ y j of the j th
Gaussian.
Let ˆ s [ njp ] denote the MMSE estimator of s [ n ]
from X [ p ] =( x T [0], x T [1], ::: , x T [ p ]) T . The notation
ˆ s [ njn¡ 1] stands for one-step prediction of the state
vector s [ n ] from data X [ 1]. The objective of this
paper is to derive a recursive method for estimation
of s [ n ] from the observed data X [ n ]. To this end, the
MMSE criterion resulting in the conditional mean
estimator
ˆ s [ njn ] = E [ s [ n ] jX [ n ]]
(5)
is employed.
B. NL-GMKF Derivation
In this section, the recursive NL-GMKF is derived
based on the MMSE criterion. Let x [ njn¡ 1] denote
the MMSE estimator of x [ n ]from X [ 1] using (2).
Then x [ njn¡ 1] is given by
x [ njn¡ 1]= E ( x [ n ] jX [ 1])
II. NL-GMKF
= E ( h ( s [ n ], w [ n ]) jX [ 1]) (6)
A. DSS Model
and the innovation process defined as x [ n ]isgivenby
The DSS model is widely used for maneuvering
target tracking problems where the system state and
observation vectors f s [ n ], x [ n ], n =0,1,2, :::g are
described by the following nonlinear, non-Gaussian
DSS model:
x [ n ]= x [ n ] ¡ x [ njn¡ 1]
= h ( s [ n ], w [ n ]) ¡ x [ njn¡ 1] : (7)
If the transformation X [ n ] $ [ X T [ 1], x T [ n ]] T
is one-to-one, then the conditional distribution of
s [ n ] jX [ n ] is identical to the conditional distribution
of s [ n ] jX [ 1], x [ n ]. Since s [ n ]and x [ n ]given
X [ 1] are assumed to be jointly GMM of order
s [ n ]= a ( s [ 1], u [ n ])
(1)
x [ n ]= h ( s [ n ], w [ n ])
(2)
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L , the conditional distribution of s [ n ] j x [ n ], X [ 1]
given the random mixture indicator ´ l [ n ] [42] is
Gaussian. Therefore, the conditional distribution of
s [ n ] jX [ n ] is GMM of order L :
In the following, the parameters required in (14)
and (15) are obtained. Let
·
¸
·
¸
s [ n ]
x [ n ]
s [ n ]
x [ n ]
y [ n ]=
and y [ n ] =
:
s [ n ] jX [ n ] » GMM( ® s [ njn , ´ l [ n ]], ¹ s [ njn , ´ l [ n ]],
¡ s [ njn , ´ l [ n ]]; l =1, ::: , L ) :
Then using (1), (2), and (7) one obtains
0
2
4 s [ 1]
3
1
·
¸
a ( s [ 1], u [ n ])
h ( a ( s [ 1], u [ n ]), w [ n ])
@
5
A
(8)
y [ n ]=
= G
u [ n ]
w [ n ]
In the following, the parameters of this conditional
distribution às [ njn ]where
(16)
and
·
¸
à s [ njn ]= s [ njn , ´ l [ n ]], ¹ s [ njn , ´ l [ n ]],
¡ s [ njn , ´ l [ n ]] g l =1
0
x [ njn¡ 1]
y [ n ]= y [ n ] ¡
(9)
2
4 s [ 1]
3
5
1
A
are derived.
Since the conditional distribution of s [ n ], x [ n ]
given the random mixture indicator ´ l [ n ], is jointly
Gaussian, then the mean vector ¹ s [ njn , ´ l [ n ]] and
covariance matrix ¡ s [ njn , ´ l [ n ]] can be obtained as
¹ s [ njn , ´ l [ n ]]= E [ s [ n ] j x [ n ], X [ 1], ´ l [ n ]]
= E [ s [ n ] jX [ 1], ´ l [ n ]]
+ ¡ sx [ njn¡ 1, ´ l [ n ]] ¡ ¡ 1
·
0
x [ njn¡ 1]
¸
= G
u [ n ]
w [ n ]
¡
: (17)
Since y [ n ], is a linear transformation of y [ n ], then
the vectors s [ n ]and x [ n ]given X [ 1] are jointly
GMM of order L , that is, the conditional distribution
of y [ n ]given X [ 1] can be modeled by an L th
order GMM with parameters:
x
à y [ njn¡ 1]= y [ njn¡ 1, ´ l [ n ]], ¹ y [ njn¡ 1, ´ l [ n ]],
¡ y [ njn¡ 1, ´ l [ n ]] g l =1
£ [ njn¡ 1, ´ l [ n ]]
£ ( x [ n ] ¡¹ x [ njn¡ 1, ´ l [ n ]]) (10)
¡ s [ njn , ´ l [ n ]]=cov( s [ n ] j x [ n ], X [ 1], ´ l [ n ])
=cov( s [ n ] jX [ 1], ´ l [ n ])
¡¡ sx [ njn¡ 1, ´ l [ n ]] ¡ ¡ 1
(18)
where
¹ y [ njn¡ 1, ´ l [ n ]]
·
¸
¹ s [ njn¡ 1, ´ l [ n ]]
¹ x [ njn¡ 1, ´ l [ n ]]
=
(19)
x
£ [ njn¡ 1, ´ l [ n ]] ¡ sx [ njn¡ 1, ´ l [ n ]]
(11)
¡ y [ njn¡ 1, ´ l [ n ]]
·
¸
¡ s [ njn¡ 1, ´ l [ n ]] ¡ sx [ njn¡ 1, ´ l [ n ]]
¡ sx [ njn¡ 1, ´ l [ n ]] ¡ x [ njn¡ 1, ´ l [ n ]]
¢
=
:
where
¹ x [ njn¡ 1, ´ l [ n ]]= E [ x [ n ] jX [ 1], ´ l [ n ]]
¡ x [ njn¡ 1, ´ l [ n ]]=cov( x [ n ] jX [ 1], ´ l [ n ])
¡ sx [ njn¡ 1, ´ l [ n ]]=cov( s [ n ], x [ n ] jX [ 1], ´ l [ n ]) :
(20)
(12)
Using the properties of the jointly
GMM-distributed random processes, s [ n ] jX [ 1]
and x [ n ] jX [ 1], the mixture weights can be
obtained as
Following the conventions of the KF, the l th Kalman
gain corresponding to the l th mixture component is
defined as
® s [ njn , ´ l [ n ]]
® y [ njn¡ 1, ´ l [ n ]] © ( x [ n ]; ° x l [ njn¡ 1])
=
P
L
K l [ n ] = ¡ sx [ njn¡ 1, ´ l [ n ]] ¡ ¡ 1
x [ njn¡ 1, ´ l [ n ]] :
l 0 =1 ® y [ njn¡ 1, ´ l 0 [ n ]] © ( x [ n ]; ° x l 0 [ njn¡ 1])
(21)
(13)
Using (13), (10) and (11) can be rewritten as
where
° x l [ njn¡ 1]= x [ njn¡ 1, ´ l [ n ]], ¡ x [ njn¡ 1, ´ l [ n ]] g:
(22)
¹ s [ njn , ´ l [ n ]]
= ¹ s [ njn¡ 1, ´ l [ n ]]+ K l [ n ]( x [ n ] ¡¹ x [ njn¡ 1, ´ l [ n ]])
(14)
Therefore, one can calculate the pdf parameters of
s [ n ] jX [ n ] given in (14), (15), and (21) using the
parameters of the distribution y [ n ] jX [ 1] obtained
in the following.
¡ s [ njn , ´ l [ n ]]
= ¡ s [ njn¡ 1, ´ l [ n ]] ¡ K l [ n ] ¡ xs [ njn¡ 1, ´ l [ n ]] : (15)
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0
@
641081676.002.png
The conditional pdf of y [ n ] jX [ 1] is modeled
by GMM of order L with parameters
The measurement prediction is calculated as a
conditional mean estimator of x [ n ]given X [ 1],
using parameters obtained in (24) and (25) as follows
à y [ njn¡ 1]= y [ njn¡ 1, ´ l [ n ]], ¹ y [ njn¡ 1, ´ l [ n ]],
¡ y [ njn¡ 1, ´ l [ n ]] g l =1
X
x [ njn¡ 1]=
® y [ njn¡ 1, ´ l [ n ]] ¹ x [ njn¡ 1, ´ l [ n ]] :
(23)
l =1
where
(30)
The MMSE estimator in (5) is obtained using (14)
and (21) as follows:
·
¹ s [ njn¡ 1, ´ l [ n ]]
¹ x [ njn¡ 1, ´ l [ n ]]
¸
¹ y [ njn¡ 1, ´ l [ n ]]=
(24)
and
X
L
ˆ s [ njn ]=
® s [ njn , ´ l [ n ]] ¹ s [ njn , ´ l [ n ]] : (31)
¡ y [ njn¡ 1, ´ l [ n ]]
·
¸
l =1
¡ s [ njn¡ 1, ´ l [ n ]] ¡ sx [ njn¡ 1, ´ l [ n ]]
¡ sx [ njn¡ 1, ´ l [ n ]] ¡ x [ njn¡ 1, ´ l [ n ]]
This completes the derivation of the NL-GMKF.
Note that the GMM order of the conditional
distribution y [ n ] jX [ 1] might be obtained
using model order selection algorithms such as
the minimum description length (MDL) [43].
Alternatively, L can be set as an upper bound on the
number of mixture components in the conditional
pdf.
In this work, the vector parameter à y [ njn¡ 1]
is obtained from the data D 0 using the greedy EM
algorithm [44]. The greedy learning algorithm
controls the GMM order of the estimated pdf, which
varies over the iterations. In [41] it was shown
that the greedy EM algorithm is insensitive to the
initialization. The pdf estimation using the greedy EM
algorithm appears in [41], [44] and is summarized in
the Appendix.
=
:
(25)
Since x [ njn¡ 1] depends on X [ 1] only, then
from (17) we conclude that the conditional pdf of
y [ n ] jX [ 1] is shifted by
·
0
x [ njn¡ 1]
¸
compared to the conditional pdf of y [ n ] jX [ 1]:
·
0
x [ njn¡ 1]
¸
¹ y [ njn¡ 1, ´ l [ n ]]= ¹ y [ njn¡ 1, ´ l [ n ]] ¡
(26)
¡ y [ njn¡ 1, ´ l [ n ]]= ¡ y [ njn¡ 1, ´ l [ n ]]
(27)
® y [ njn¡ 1, ´ l [ n ]]= ® y [ njn¡ 1, ´ l [ n ]]
(28)
C. NL-GMKF Summary
and
This subsection summarizes the derived
NL-GMKF for recursive estimation of s [ n ] from X [ n ].
¹ x [ njn¡ 1, ´ l [ n ]]= ¹ x [ njn¡ 1, ´ l [ n ]] ¡ x [ njn¡ 1] :
(29)
Hence the mixture weights and covariance matrices
in à y [ njn¡ 1] and à y [ njn¡ 1] are identical and the
means are related in (29).
Since the function G ( ¢ ) is nonlinear, the parameters
of the conditional distribution of y [ n ] jX [ 1]
cannot be obtained analytically. Alternatively, the MC
approach can be implemented. Thus, an artificial data
set D is obtained from the conditional distribution of
2
4 s [ 1]
1) Initialization:
Initialize the L -order GMM parameters of the state
vector at time instance n = ¡ 1.
® s [ ¡ 1 1, ´ s l [ ¡ 1]]= ® s l [ ¡ 1]
¹ s [ ¡ 1 1, ´ s l [ ¡ 1]]= ¹ s l [ ¡ 1]
¡ s [ ¡ 1 1, ´ s l [ ¡ 1]]= ¡ s l [ ¡ 1] :
3
Set n =0.
2) Mixture parameters of the state and measurement
prediction:
Generate an artificial data set D from the
conditional distribution of
2
4 s [ 1]
u [ n ]
w [ n ]
5
given X [ 1]. Next, the nonlinear function G ( ¢ )is
applied on the data set D to obtain a new artificial
data set D 0 , which is used to obtain the pdf parameters
of y [ n ] jX [ 1], i.e., Ã y [ njn¡ 1]. The statistical
parameters required for calculation of (13), (14),
and (15) can be obtained from the parameters of
à y [ njn¡ 1] in (18).
u [ n ]
w [ n ]
3
5
given X [ 1], according to the pdf of s [ 1] j
X [ 1] from the previous step and pdfs of u [ n ]
and w [ n ].
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