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Workshop proceeding - final.pdf - Faculty of Information and ...

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( xˆ<br />

, m ˆ ) = argmax Γ ( x , m )<br />

(51)<br />

k k k k k<br />

xk,<br />

mk<br />

The previous states <strong>and</strong> modes are found by tracing backwards from ( xˆ<br />

, mˆ<br />

).<br />

k<br />

k<br />

6. Simulation <strong>and</strong> Results<br />

In our simulation, an approaching target, referring back to Fig. 2, travels at initial range r<br />

0<br />

= 300 km,<br />

with velocity v = 2.8 Mach, <strong>and</strong> headingα = 225 deg. Since the target is not travelling along the radial<br />

direction, the Doppler is inevitably time-varying. We set the Doppler rate increment variance<br />

2 2<br />

Q = (6Hz/s ) .Fig. 5 <strong>and</strong> Fig.6 show the trajectories <strong>of</strong> target range <strong>and</strong> Doppler, respectively. The<br />

target Doppler information is represented by the observed apparent Doppler <strong>and</strong> corresponding<br />

ambiguity number.<br />

Fig. 5. target range trajectory<br />

Fig. 6. target Doppler trajectory, represented by apparent Doppler trajectory <strong>and</strong> ambiguity number<br />

trajectory<br />

The ambiguity number transits for i to j = i − 1 when the guard condition is satisfied. To account for<br />

the r<strong>and</strong>om variations in Doppler increment, δ ij<br />

is modeled as a Gaussian distributed variable with<br />

20

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