Page 227 - Applied Probability
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10. Molecular Phylogeny
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                              satisfying p AG(0) = 0.
                                This analysis has produced the probabilities p AA (t), p AG (t), and q AY (t)
                              of being in A, G, or either pyrimidine at time t starting from A at time
                              0. To decompose q AY (t) into its two constituent probabilities p AC (t) and
                              p AT (t), define q UU (t) to be the probability that the chain is in either purine
                              at time t given that it starts in either purine at time 0. Likewise, define
                              q UC (t) to be the probability that the chain is in the pyrimidine C at time t
                              given that it starts in either purine at time 0. Because of the symmetry of
                              the transition rates, q UU (t) makes sense, and q UC (t)= p AC (t)= p GC (t).
                              From q AY (t) and p AC (t), we calculate p AT (t)= q AY (t) − p AC (t).
                                To derive a differential equation for q UU (t), note the approximation
                                      q UU (t + h)= q UU (t)(1 − γh − λh)+ q UC (t)(δ + κ)h
                                                     +[1 − q UU (t) − q UC (t)](δ + κ)h + o(h),
                              where 1 − q UU (t) − q UC (t) is the probability of being in T at time t. This
                              approximation leads to
                                                  q    (t)  = −c 1 q UU (t)+ c 5 ,
                                                   UU
                              where c 1 was defined previously and
                                                            = δ + κ.
                                                         c 5
                              Again, the solution
                                                            c 5 +(c 1 − c 5 )e −c 1 t
                                                 q UU (t)=                               (10.14)
                                                                    c 1
                              satisfying q UU (0) = 1 follows directly.
                                The approximation for q UC (t),
                                       q UC (t + h)= q UC (t)(1 − δh − κh − βh)+ q UU (t)γh
                                                      +[1 − q UU (t) − q UC (t)]σh + o(h),
                              yields the differential equation

                                              q UC (t)  = −c 6 q UC (t)+ c 7 q UU (t)+ σ,

                              where

                                                     c 6  = δ + κ + σ + β
                                                     c 7  = γ − σ.
                              In view of equation (10.14) and the initial condition q UC (0) = 0, the solu-
                              tion for q UC (t)is

                                                       c 5 c 7 + σc 1  (c 1 − c 5 )c 7 −c 1 t
                                           q UC (t)  =          +           e
                                                         c 1 c 6   c 1 (c 6 − c 1 )
                                                         c 7 (c 6 − c 5 )+ σ(c 6 − c 1 )  −c 6 t
                                                       −                     e    .      (10.15)
                                                              c 6 (c 6 − c 1 )
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