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The decomposition of histories can now be simulated on a computer in order to actually
solve the Master equation. Here, we only describe the simplest version (spontaneous
emission, no driving field), starting from a
pure state
of the total system. For more details, see Carmichael or Plenio/Knight.
Step 1: Fix a time step
. Calculate the probability
of photon emission;
 |
|
|
(147) |
Step 2: Compare
with a random number
Step 3: Go back to Step 1.
This procedure (performed with small time-steps
up to a final time
)
yields a `curve' of simulated states
,
in the
system Hilbert space
. The procedure is then repeated many times in order to
obtain time-dependent averages
of observables
.
The entire procedure yields a density operator
that solves the original Master equation,
Eq.(7.143): in one time step
, we have
Remarks:
- The splitting of
as
is not unique, there
are ususally several ways of how to `unravel' the Master equation.
- For more complicated Master equations, one has to extend and modify the above procedure.
Next: Feynman-Vernon Influence Functional Theories
Up: Unravelling and Decomposition into
Previous: Decomposition into Histories
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Tobias Brandes
2004-02-18