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Propp-Wilson Algorithm;
Coupling from the Past
- Recall that
- the procedure of coupling to the future discussed in
Section 3.5.1 starts at a deterministic time 0
whereas the final state, i.e. the coupling time
of the
simulation is random.
- Moreover, the state distribution of the Markov chain
at the coupling time
is in general not equal to the
stationary limit distribution
.
- Therefore, we will now consider a different coupling method,
- which is called Coupling from the Past (CFTP).
- It was developed in the mid 90s by Propp and Wilson at the Massachusetts Institute of Technology (MIT).
- The procedure is similar to coupling to the future (see
Section 3.5.1) but now the initial ,,time'' of the
simulation will be chosen randomly whereas the final
,,time'' is deterministic.
- In other words, the Markov chains
are not started at
,,time'' 0,
- but sufficiently far away in the ,,past'' such that by time 0 at
the latest all paths will have merged.
For the precise mathematical modeling of this procedure we need the
following notation.
- Definition
The random variable
is called CFTP coupling time where we define
if there is no
integer
such that
.
Theorem 3.23

Let

.
Then, for all

,
Moreover, for arbitrary

and

,
- Proof
-
- Remarks
-
- If the number
of elements in the state space
is large,
- the MCMC simulation of
based on the CFTP algorithm by Propp
and Wilson can be computationally inefficient
- as for every initial state
a complete
path needs to be generated.
- However, in some cases the computational complexity can be
reduced. Examples will be discussed in Sections 3.5.3
and 3.5.4.
- In these special situations the state space
and the update function
possess certain monotonicity
properties.
- As a consequence it suffices to consider a single sequence
of independent and
-uniformly distributed innovations.
- Moreover, only two different paths need to be generated.
Next: Monotone Coupling Algorithms
Up: Coupling Algorithms; Perfect MCMC
Previous: Coupling to the Future;
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Ursa Pantle
2006-07-20