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Bernal S D_2010.pdf - University of Plymouth

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4.4. FEEDFORWARD PROCESSING<br />

(he simultaneous coincidence <strong>of</strong> the features in the afferent nodes, as proposed by George and<br />

Hawkins (2009). Finally, the weight matrix for each S2 prototype is approximated by the CPT<br />

p{a\s2).<br />

S2b>n^n^szJ'si=^^V {-P - ||C1{6„.„,.,1 - n«||^)<br />

fc,j,,.V, k,<br />

where the indices are given by Equations (4.3) to (4.5),<br />

Similarly, the invariance operation in HMAX i.s approximated u.sing belief propagation as shown<br />

in liquation 4.9. The approximation to ihe max operation is emiwdded in the ^i(52) output<br />

messages to S2 generated using the weights in the CPT P{C\\S2), which sum over the CI<br />

features <strong>of</strong> the same group. In order to make this possible, the most common SI states and<br />

locations have previously been combined in the CI node states through the CPT /^(Sl|Cl) (see<br />

r'igures 4.7 and 4.9). In this sense it can be argued that both the selectivity operation and<br />

the invariance operation are actually implemenled using the weights in P{C\\S2), whereas the<br />

weights in P(i'l |C1) implement a necessary pre-processing step.<br />

4.4.2 Dealing with large-scale Bayeslan networks<br />

Due to the large fan-in in the network and the large number <strong>of</strong> stales, calculating the A function<br />

<strong>of</strong> a node requires multiplying a high number <strong>of</strong> polL'ntially very low probability values. For<br />

example, a CI node in band 8 receives input from 96S (22 x 22 locations x 2 bands) SI nodes,<br />

meaning that it is necessary to obtain the product <strong>of</strong> 968 probability disiribuiions. The result<br />

172<br />

(4.9)

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