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Solution to selected problems.

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31. Let T be an arbitrary F µ s<strong>to</strong>pping time and Λ = {ω : X T (ω) ≠ X T − (ω)}. Then by<br />

Meyer’s theorem, T = T Λ ∧ T Λ c where T Λ is <strong>to</strong>tally inaccessible time and TΛ c is predictable time.<br />

By continuity of X, Λ = ∅ and T Λ = ∞. Therefore T = T Λ c. It follows that all s<strong>to</strong>pping times are<br />

predictable and there is no <strong>to</strong>tally inaccessible s<strong>to</strong>pping time.<br />

32. By exercise 31, the standard Brownian space supports only predictable time since Brownian<br />

motion is clearly a strong Markov Feller process. Since O = σ([S, T [: S, T are s<strong>to</strong>pping time and S ≤<br />

T ) and P = σ([S, T [: S, T are predictable times and S ≤ T ), if all s<strong>to</strong>pping times are predictable<br />

O = P.<br />

35. E(M t ) ≥ 0 and E(M t ) = exp [B τ t − 1/2(t ∧ τ)] ≤ e. So it is a bounded local martingale and<br />

hence martingale. If E(−M) is a uniformly integrable martingale, there exists E(−M ∞ ) such that<br />

E[E(−M ∞ )] = 1. By the law of iterated logarithm, exp(B τ − 1/2τ)1 {τ=∞} = 0 a.s. Then<br />

[ (<br />

E[E(−M ∞ )] = E exp −1 − τ ) ]<br />

1<br />

2 {τ

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