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ypy ( ,0,0) = θ py ( − 1,0,0) y1 ≥ 1<br />

1 1 1 1<br />

yp(0, y,0) = θ p(0, y− 1,0) y2 ≥ 1<br />

(5.11)<br />

2 2 2 2<br />

yp(0,0, y) = θ p(0,0, y− 1) y3 ≥ 1<br />

3 3 3 3<br />

p(0,0,0) = exp( − ( θ + θ + θ + θ + θ + θ )) . (5.12)<br />

1 2 3 12 13 23<br />

The above mentioned recurrence relations and the Flat algorithm (Tsiamyrtzis and<br />

Karlis, 2004) are used to calculate the probabilities <strong>of</strong> the restricted covariance trivariate<br />

Poisson model.<br />

5.2.3 The Flat algorithm<br />

Using the Flat Algorithm the calculation <strong>of</strong> py (<br />

1, y2, y<br />

3)<br />

can be done in two stages. In<br />

the first stage, one can move from ( y1, y2, y<br />

3)<br />

to the closest hyperplane using only one<br />

<strong>of</strong> the recurrence relationships (5.7), and in the second stage, he can move down to the 0<br />

point by the simplified recurrence relationships (5.10) and (5.11). Thus, starting from<br />

( y1, y2, y<br />

3)<br />

and applying the recurrence relationship, we get three new points<br />

( y1− 1, y2, y3)<br />

, ( y1−1, y2− 1, y3)<br />

and ( y 1<br />

−1, y 2<br />

−1, y 3<br />

− 1) . Applying the same recurrence<br />

relationship to these three points we get another six new points: ( y 1<br />

− 2, y 2<br />

, y 3<br />

),<br />

( y1−2, y2− 1, y3)<br />

, ( y1−2, y2, y3− 1) , ( y1− 2, y2− 2, y3)<br />

, ( y1−2, y2−1, y3− 1) and<br />

( y −2, y , y − 2) . Figure 5.1 illustrates how coordinates can move to the closer plane<br />

1 2 3<br />

using the recurrence relationship (5.7) <strong>for</strong> the case y1 ≤ y2 ≤ y3<br />

.<br />

75

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