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(1)Stochastic Mechanics 6 CFU Part II 12.6.2012 Exercise 1 Let Wt be a Brownian motion

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Stochastic Mechanics 6 CFU Part II 12.6.2012

Exercise 1 Let Wt be a Brownian motion.

a llustrate Ito’s formula and use it to calculate d(eσWt2)

b Let H ∈ L2(0, T ) be a step process with partition P = {0 = t0 <

t1 < · · · < tn = T }. Define the (Ito) Riemann sums of H with respect to the Brownian motion Wt for this partition P , by

S(H, P ) =

n−1

X

i=0

Hti(Wti+1− Wti) Calculate the mean and the variance of S(H, P ).

Exercise 2

a Let g = g(y) be a given function of y, and suppose that y = f (w) is a solution of the ODE

dy = g(y)dw,

that is, f0(w) = g(f (w)). Show that Xt = f (Wt) then is a solution of the SDE:

dXt= 1

2g(Xt)g0(Xt)dt + g(Xt)dWt b Use point a above to solve the SDE

dXt= σ2

4 dt + σp XtdWt with X0 ≥ 0. (Hint: Take g(x) = σ√

x).

Exercise 3 Consider the boundary value problem for the backwards heat equation with a drift term (a being a constant):

( ∂u

∂s +12∂x2u2 + a∂u∂x = 0, x ∈ R, s < T u(x, T ) = e2x

a Write the solution of the associated SDE and calculate its transition probability density.

b Use Feynman-Kac formula to solve it.

Exercise 4 Given the SDE

( dXt= (2 − Xt)dt +√ 2dWt X0 = 1

a Solve the equation and calculate E(Xt) and V ar(Xt).

b Calculate the transition probability density of Xt.

c Write the Kolmogorov forward equation for the process and find its stationary solution.

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