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Variational Principles in Conformation Dynamics - FU Berlin, FB MI

Variational Principles in Conformation Dynamics - FU Berlin, FB MI

Variational Principles in Conformation Dynamics - FU Berlin, FB MI

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A. AppendixA.1. Diffusion <strong>in</strong> a quadratic potentialLet us prove the properties of the diffusion <strong>in</strong> a quadratic potential as <strong>in</strong>troduced <strong>in</strong> sectionIII.4. First,letusderiveananalyticexpressionfortheproblem’ssolution.Onstochastic<strong>in</strong>tegrals and Ito’s formula, see [Evans, ch.4].Lemma A.1: If the process is <strong>in</strong>itially distributed accord<strong>in</strong>g to X 0 ,thenthedistributionattime t is given by the stochastic <strong>in</strong>tegralX t = e −θt X 0 + σ t0dB s e −θ(t−s) .(A.1)Proof. The proof can also be found on [Wikipedia]. Let X t be the solution of the correspond<strong>in</strong>gstochastic differential equation, i.e.dX t = −θX t dt + σdB t .(A.2)Consider the function f(X t ,t):=e θt X t . Accord<strong>in</strong>g to Ito’s formula, f(X t ,t) satisfies theSDE:d(f(X t ,t)) = ∂f ∂fdt +∂t ∂x dX t + 1 ∂ 2 f2 ∂x 2 σ2 dt(A.3)= θe θt X t dt − θe θt X t dt + e θt σdB t = e θt σdB t . (A.4)The process f(X t ,t) is therefore given by the stochastic <strong>in</strong>tegrale θt X t = f(X t ,t)=X 0 + σ t0dB s e θs .(A.5)

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