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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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