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Military Communications and Information Technology: A Trusted ...

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Chapter 3: <strong>Information</strong> <strong>Technology</strong> for Interoperability <strong>and</strong> Decision...<br />

285<br />

tion. In addition, ASDs fully describe the correlations between the state estimates<br />

at different instants of time.<br />

All information on the target states accumulated over a time window<br />

tk, tk , , tn<br />

of length kn<br />

1,<br />

xkn ( xk, , xn)<br />

(10)<br />

that can be extracted from the time series of accumulated sensor data up to<br />

k<br />

<strong>and</strong> including time is contained in a joint density function p( x<br />

kn| Z ), which<br />

is called a ASD.<br />

Iterative ASD<br />

ASD posterior<br />

z z z z z z z z z<br />

0<br />

time t<br />

Figure 2. Schematic illustration of an iterative ASD filter <strong>and</strong> the ASD posterior. The iterative filtering<br />

scheme includes the calculation of a prior ASD density using a fixed window size. It is based<br />

on an ASD posterior, which yields the joint density conditioned on the entire set of measurements<br />

Given the full posterior ASD [2], one can calculate the exact cross-covariance<br />

to timely delayed measurements. To this end, let us consider a measurement<br />

produced at time with t n<br />

m t k<br />

i.e. possibly before the `present’ time<br />

where the time series is available <strong>and</strong> has been exploited. We would like to<br />

underst<strong>and</strong> the impact this new, but late sensor information has on the present<br />

<strong>and</strong> the past target states xl , l n, , k,<br />

i.e. on the accumulated state x<br />

kn<br />

Let<br />

be a measurement of the observed object state at time characterized by<br />

a Gaussian likelihood function, which is defined by a measurement matrix <strong>and</strong><br />

a corresponding measurement error covariance matrix We further renumber<br />

the target states xk, , xn<br />

such that xk, , xm, , xn : xkmn<br />

: :<br />

are consistent with<br />

their time stamps ( tl) lk, , m, ,<br />

n.<br />

By an application of continuous time retrodiction (see [3], e.g., for a detailed<br />

discussion), it is well possible to extend the posterior density of the state x<br />

kn<br />

to<br />

a prior density of the extended state x<br />

kmn : :<br />

[4]. One obtains a single Gaussian density<br />

with a joint expectation vector including the estimates for all single states:<br />

k<br />

px ( | Z) N ( x ; x , P ),<br />

(11)<br />

kmn : : kmn : : kmnk : : | kmnk : : |<br />

where the expectation vector accumulates the target estimates for each state within<br />

the time window:<br />

x ( x , , x , , x ).<br />

(12)<br />

k: mnk : | kk | mk | nk |

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