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Unit 12: Design and Evaluation of Simulation Experiments (II)
Poisson’s Equation Notes
For that purpose, it is useful to introduce Poisson’s equation. The stationary probability vector
and the fundamental matrix Z can be viewed as solutions x to Poisson’s equation
xQ = y ;
for appropriate (row) vectors y. It can be shown that Poisson’s equation has a solution x if and
T
only if ye = 0, where e is the row vector of 1’s and e is its transpose. Then all solutions are of the
T
form
x = –yZ + (xe ) .
T
For example, is obtained by solving Poisson’s equation when y is the zero vector (and
normalizing by requiring that xe = 1). Then elements of Z can be obtained by choosing other
T
vectors y, requiring that xe = 0.
T
In passing, we remark that there also is an alternate column-vector form of Poisson’s equation,
namely,
T
Qx = y ,
T
T
which has a solution if and only if y = 0. Then all solutions are of the form
T
T
x = —Zy + (x )e .
T
T
It is significant that, for a CTMC, the asymptotic bias defined in (2) and the asymptotic
2
variance defined in (3) can be expressed directly in terms of , Z, the function f and (for ) the
initial probability vector, say , i.e.,
m m
( ) Zf i Z f j
, i j
i 0 j 0
and
m m
2
2( f )Zf 2 f i Z , i j j . f
i
i 0 j 0
Moreover, the asymptotic parameters ( ) and are themselves directly solutions to Poisson’s
2
equation. In particular,
( ) xf T ,
T
where x is the unique solution to Poisson’s equation for y = — + with xe = 0. Similarly,
2
2xf T ,
where x is the unique solution to Poisson’s equation for y = –¡(f — ) with xe = 0.
T
i i i
Birth-and-Death Processes
Birth-and-death (BD) processes are special cases of CTMC’s in which Q = 0 when |i—j| > 1; then
i,j
we often use the notation Q and Q —1 , and refer to as the birth rates and as the
i,i+1 i i,i i i i
death rates. For BD processes and skip-free CTMC’s (which in one direction can go at most one
step), Poisson’s equation can be efficiently solved recursively.
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