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126 7 Local Alignment Statistics<br />

Because the mean step size is negative, the distribution function<br />

is finite. Moreover, it satisfies the renewal equation<br />

S(y)<br />

for any 0 ≤ y < ∞. Define<br />

S(y)=Pr[max<br />

k≥0 S k ≤ y] (7.19)<br />

= S(−1)+(S(y) − S(−1))<br />

= ( 1 − Pr[t + < ∞] ) +<br />

V (y) satisfies the renewal equation<br />

y<br />

∑<br />

k=0<br />

V (y)= ( Pr[t + < ∞] − Pr[Z + ≤ y] ) e λy +<br />

Pr[Z + = k]S(y − k) (7.20)<br />

V (y)=(1 − S(y))e λy . (7.21)<br />

y<br />

∑<br />

k=0<br />

e λk Pr[Z + = k]V (y − k). (7.22)<br />

By equation (7.18), e λk Pr[Z + = k] is a probability distribution. Using the Renewal<br />

Theorem in Section B.8, we have that<br />

lim V (y)<br />

y→∞<br />

= ∑∞ y=0 eλy (Pr[t + < ∞] − Pr[Z + ≤ y])<br />

E ( Z + e λZ+ ; t + < ∞ ) .<br />

By (7.18), multiplying the numerator by e λ − 1 yields 1 − Pr[t + < ∞] because the<br />

step sizes that have nonzero probability have 1 as their greatest common divisor.<br />

Hence,<br />

lim V (y)<br />

y→∞<br />

1 − Pr[t + < ∞]<br />

= (<br />

e λ − 1 ) E ( Z + e λZ+ ; t + < ∞ ).<br />

Recall that Q 1 = max 0≤k

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