Unformatted text preview: for a
set of parameters that cause the inputs to model the outputs. Function learning attempts to
nd the best parameter vector v; alignment attempts to nd the best transformation T . As
we did for function learning, we can draw an analogy with sample entropy. The log likelihood
of T is proportional to the conditional entropy of the image given the model,
1
log`T = , N havT X j uX ; T; ; q; F :
a 4.14 This is not the EMMA estimate of entropy, but the conditional entropy of v under the
assumption that v is conditionally Gaussian. For the problems described in Section 3.1 it
was possible to show that entropy optimization led to maximum mutual information solutions.
For this problem however, we cannot claim that maximizing log likelihood is equivalent to
maximizing the mutual information between v and u. The mutual information I vT X ; uX = hvT X , hvT X j uX ; T; ; q; F ; 4.15 includes both a conditioned and unconditioned entropy. For some types of transformations
hvT X may change as T is varied. In these cases minimizing conditional entropy is not
equivalent to maximizing mutual information. One must also maximize the unconditioned
entropy. In our simple example, where only translation is varied and the signals are periodic,
unconditioned entropy does not change as T is varied.
Returning to the rst synthetic example, we can plot C T from 4.12 versus translation. Figure 4.3 graphs C T for the two signals from Figure 4.1 we have assumed periodic
boundary conditions on the signals. We can see that the cost has a very strong minimum at
the true translation of 0 pixels.
81 Paul A. Viola CHAPTER 4. MATCHING AND ALIGNMENT
1400
u(x)
v(x) Difference Squared 1200 Intensity 1
0.5
0
0.5
1 1000
800
600
400
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0 0 100 200
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Position 400 150 75 0
Position 75 150 Figure 4.3: On the left is a plot of image and model that are identical except for noise. On
the right is a plot of C T versus translation. There is a signi cant minimum at the correct
aligning translation of 0 pixels.
u(x)
v(x) 1400 Difference Squared Intensity 1500
2
1.5
1
0.5
0
0.5
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Position 400 150 75 0
Position 75 150 Figure 4.4: On the left is a plot of image and model that are related nonlinearly. On the
right is a plot of C T versus translation. There is no minima at the aligning translation of
0 pixels. In fact minima exist at incorrect translations.
Correlation works very well at matching together u and v when the imaging model and
exogenous parameters are known. In many cases however we may be faced with a situation
where F and q are unknown. In some cases alignment problems can still be solved by
assuming that the imaging function is the identity function. This assumption is not e ective
when aligning the nonmonotonically related signals shown in Figure 4.2. Figure 4.4 graphs
C T versus translation for these two signals. Notice that each of the actual minima are at
incorrect translations.
In general C T cannot be used to align signals related by an unknown nonlinear transformations. C T can however be generalized to work with signals that have been transformed
linearly. Rather than minimize the squared di erence between signals, we can instead minimize the squared di erence between signals that have been normalized. A normalized signal
82 4.1. ALIGNMENT AITR 1548 4 u(x)
v(x) Intensity 2
0
2
4
6
0 100 200
300
Position 400 Figure 4.5: Graph of ux and vx = 3ux , 2 versus x.
is one with a mean of zero and a standard deviation of one and can be computed as E
b
ux = ux , XuX :
u 4.16 The normalized version of a signal is invariant to multiplicative and additive changes to the
original. The sum of the squared di erences between the normalized signals, NC T , can
be computed directly as one minus the Normalized correlation between the signals u and v.
Normalized cost is de ned as:
, u E
4.17
NC T = 1 , Ea uX vT X EavTXX a vT X :
au X a
As a shorthand we have abbreviated sums over the coordinates x as expectations and variances.
Normalized cost can be used on signals like the ones shown in Figure 4.5 F u = 3u , 2.
A plot of NC T versus translation is identical to Figure 4.3. In some cases, normalized cost
can be applied to signals transformed by nonlinear monotonic functions. Note however that
the two signals shown in Figure 4.2 are related by a nonmonotonic function and cannot be
accommodated in this way. In these examples translation does not e ect the mean or the
standard deviation of the signals. As a result, normalized cost will not produce a convincing
minimum where cost alone does not.
83 Paul A. Viola CHAPTER 4. MATCHING AND ALIGNMENT We may still wish to align models and images that are related by nonmonotonic functions.
In this case alignment can be performed by jointly searching over the space of possible imaging
functions, exogenous parameters and transformations. Probability can be used to m...
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 Spring '10
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 The Land, Probability distribution, Probability theory, probability density function, Mutual Information, Paul A. Viola

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