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Maximize the
product of the probabilities that the
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Boltzmann
machine assigns to the vectors in the
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training set.
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This
is equivalent to maximizing the sum of
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the
log probabilities of the training vectors.
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It
is also equivalent to maximizing the
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probabilities
that we will observe those
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vectors
on the visible units if we take random
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samples
after the whole network has reached
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thermal
equilibrium with no external input.
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