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Given the actual state of the quantum system, and the
configuration of the detectors
we
compute probabilities
for the
detector to flip. Then we select randomly, with the calculated
probability distribution, the flipping detector, and we implement
the jump by changing to
according to the
formula (), with
. The probabilities
are computed using the theory of piecewise deterministic
Markov processes applied to the case of quantum measurements  as
developed within EEQT.^{}According to EEQT the probabilities
are given by the formula:

(16) 
where is the normalizing constant. Using cyclic
permutation under the trace, as well as the fact that
we find, taking trace of both sides of the formula
(), that are proportional to
given by (), thus

(17) 
Note that, owing to the fact that
we
have
, as it should be.
Next: 3. The Five Platonic
Up: 2. The algorithm
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