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Clone Pair Overlap Score
Let Ca and Cb be two clones viewed as intervals of
lengths la and lb respectively. Without loss of
generality, assume
.
Define
=
and
.
The
overlap score uses the hybridization vectors
to produce a
vector probabilities for the overlap length
.
Figure 10.10:
Clone pair overlap
score
|
The relative position of Ca,Cb and
is
shown in figure 10.10.
We first calculate the probability
.
Let
,
,
and let
Ai,j be the number of occurrences of probe j in Ci. We
can thus write the following equation:
The calculation of the probabilities inside the summation is
straightforward using the statistical model. Since hybridization
is a virtual certainty if a probe occurs many times inside a
clone, we can limit the summation to small values of k (say
), thereby making feasible the score's computation
while introducing only a negligible error. Considering each probe
as an independent source of information, the conditional
probability of the vector pair
is:
![\begin{displaymath}Pr(\overrightarrow{B_{a}} ,\overrightarrow{B_{b}} \vert l_{\g...
...t)
= \prod_{j=1}^{n} Pr(B_{aj},B_{bj} \vert l_{\gamma} = t)
\end{displaymath}](img81.gif) |
(10.15) |
Assuming uniform parameters for the probes, the expression
inside the product is
independent of j. Therefore, we can define
Px,yt by
Px,yt = Pr(Ba,j = x, Bb,j = y | t). Denoting by
Sx,y(a,b) the set of probes
,
such that
Ba,j = x and
Bb,j = y, we can write:
![\begin{displaymath}Pr(\overrightarrow{B_{a}} ,\overrightarrow{B_{b}} \vert t)
...
...rod_{x=0}^{1}\prod_{y=0}^{1}P_{x,y}^{\vert S_{x,y}(a,b)\vert}
\end{displaymath}](img84.gif) |
(10.16) |
Having computed
we can use Bayes Theorem:
![\begin{displaymath}Pr(l_{\gamma} = t_{0} \vert
\overrightarrow{B_{a}} ,\overri...
...errightarrow{B_{b}} \vert l_{\gamma} = t)Pr(l_{\gamma}
=t)}
\end{displaymath}](img86.gif) |
(10.17) |
Next: Problem Statement
Up: Constructing Physical Maps from
Previous: The Statistical Model
Itshack Pe`er
1999-03-21