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TESI DOCTORAL - La Salle

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6.3. Voting based consensus functions<br />

Sλ1 ,λ = Iλ1 2 Iλ2<br />

T<br />

=<br />

⎛<br />

1 0<br />

⎞<br />

0<br />

⎛<br />

0<br />

⎝1<br />

0<br />

0<br />

1<br />

0<br />

0<br />

1<br />

0<br />

1<br />

0<br />

0<br />

1<br />

0<br />

0<br />

1<br />

0<br />

0<br />

0<br />

0<br />

1<br />

0<br />

0<br />

1<br />

⎜<br />

1<br />

⎜<br />

⎞ ⎜<br />

0<br />

0 ⎜<br />

⎜0<br />

0⎠<br />

⎜<br />

⎜0<br />

1 ⎜<br />

⎜0<br />

⎜<br />

⎜0<br />

⎝0<br />

0<br />

0<br />

0<br />

0<br />

0<br />

0<br />

1<br />

0 ⎟<br />

1 ⎟ ⎛<br />

1 ⎟ 0<br />

1 ⎟ = ⎝2<br />

1 ⎟ 0<br />

1 ⎟<br />

0⎠<br />

0<br />

0<br />

2<br />

⎞<br />

3<br />

1⎠<br />

1<br />

(6.18)<br />

0 1 0<br />

Firstly, notice that S λ1 ,λ 2 is not a symmetric matrix (as object co-association matrices<br />

are), due to the fact that its rows and columns correspond to different entities. In fact,<br />

the (i,j)th element of S λ1 ,λ 2 is equal to the number of objects that are assigned to the ith<br />

cluster of λ1 and to the jth cluster of λ2, thus clearly indicating the degree of resemblance of<br />

these clusters. Deriving a cluster dissimilarity matrix from S λ1 ,λ 2 is pretty straightforward,<br />

provided that the implementation of the Hungarian method employed in this work does not<br />

require that the cluster dissimilarity measures verify any special property as regards their<br />

scale. The result of the cluster disambiguation method applied on this toy example is the<br />

cluster correspondence vector π λ1 ,λ 2 presented in equation (6.19).<br />

π λ1 ,λ 2 = [3 1 2] (6.19)<br />

The interpretation of the cluster correspondence vector πλ1 ,λ is that the cluster iden-<br />

2<br />

tified with the ‘1’ label in λ1 corresponds to the cluster with label ‘3’ of λ2, the cluster<br />

labeled as ‘2’ in λ1 must be aligned with the cluster with label ‘1’ of λ2, and the cluster ‘3’<br />

of λ1 is equivalent to cluster with label ‘2’ of λ2.<br />

The most usual way of representing the information contained in the cluster correspondence<br />

vector πλ1 ,λ is by means of a cluster permutation matrix P 2 λ1 ,λ . In general, P 2 λ1 ,λ is 2<br />

a k × k matrix whose entries are all zero except that the πλ1 ,λ (i)-th entry of the ith row is<br />

2<br />

equal to 1. The cluster permutation matrix corresponding to our toy example is presented<br />

in equation (6.20). Notice how all of its entries are zero except for the third entry of the<br />

first row (as πλ1 ,λ (1) = 3), the first entry of the second row (as π 2 λ1 ,λ (2) = 1) and the<br />

2<br />

second entry of the third row (as πλ1 ,λ (3) = 2).<br />

2<br />

P λ1 ,λ 2 =<br />

⎛<br />

0 0<br />

⎞<br />

1<br />

⎝1<br />

0 0⎠<br />

(6.20)<br />

0 1 0<br />

In order to obtain the cluster permuted version of the clustering λ1, it is necessary to<br />

multiply the transpose of the cluster permutation matrix Pλ1 ,λ by the incidence matrix<br />

2<br />

associated to this clustering, Iλ1 , which yields the cluster permuted incidence matrix I πλ1 ,λ2 λ , 1<br />

as indicated in equation (6.21).<br />

I πλ 1 ,λ 2<br />

λ 1<br />

T<br />

= Pλ1 ,λ Iλ1<br />

2 ,λ2 In our example, the cluster permuted incidence matrix is:<br />

174<br />

(6.21)

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