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2014 | OriginalPaper | Buchkapitel

Introduction to Stochastic Calculus and to the Resolution of PDEs Using Monte Carlo Simulations

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Abstract

I give a pedagogical introduction to Brownian motion, stochastic calculus introduced by Itô in the fifties, following the elementary (at least not too technical) approach by Föllmer [Seminar on Probability, XV (Univ. Strasbourg, Strasbourg, 1979/1980) (French), pp. 143–150. Springer, Berlin, 1981]. Based on this, I develop the connection with linear and semi-linear parabolic PDEs. Then, I provide and analyze some Monte Carlo methods to approximate the solution to these PDEs. This course is aimed at master students, Ph.D. students and researchers interesting in the connection of stochastic processes with PDEs and their numerical counterpart. The reader is supposed to be familiar with basic concepts of probability (say first chapters of the book Probability essentials by Jacod and Protter [Probability Essentials, 2nd edn. Springer, Berlin, 2003]), but no a priori knowledge on martingales and stochastic processes is required.

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Fußnoten
1
A Gaussian random variable X (see [46]) with mean μ and variance σ 2 > 0 (often denoted by \(\mathcal{N}(\mu,\sigma ^{2})\)) is the r.v. with density
$$\displaystyle{ g_{\mu,\sigma ^{2}}(x) = \frac{1} {\sigma \sqrt{2\pi }}\mathrm{exp}[-\frac{(x-\mu )^{2}} {2\sigma ^{2}} ],\quad x \in \mathbb{R}. }$$
If σ 2 = 0, X = μ with probability 1. Moreover, for any \(u \in \mathbb{R}\), \(\mathbb{E}(e^{\mathit{uX}}) = e^{u\mu +\frac{1} {2} u^{2}\sigma ^{2}}\).
 
2
Two random variables X 1 and X 2 are independent if and only if \(\mathbb{E}(f(X_{1})g(X_{2})) = \mathbb{E}(f(X_{1}))\mathbb{E}(g(X_{2}))\) for any bounded functions f and g. This extends similarly to a vector.
 
3
\((X_{1},\ldots,X_{n})\) is a Gaussian vector if and only if for any \((\lambda _{i})_{1\leq i\leq n} \in \mathbb{R}^{n}\), \(\sum _{i=1}^{n}\lambda _{i}X_{i}\) has a Gaussian distribution. Independent Gaussian random variables form a Gaussian vector. A process (X t ) t is Gaussian if \((X_{t_{1}},\ldots,X_{t_{n}})\) is a Gaussian vector for any times \((t_{1},\ldots,t_{n})\) and any n. A Gaussian process is characterized by its mean \(m(t) = \mathbb{E}(X_{t})\) and its covariance function \(K(s,t) = \mathbb{C}\mathrm{ov}(X_{s},X_{t})\).
 
4
We recall that “an event A occurs a.s.” (almost surely) if \(\mathbb{P}(\omega:\omega \in A) = 1\) or equivalently if {w: wA} is a set of zero probability measure.
 
5
Here, we use the following standard result: let (X n ) n ≥ 1 be a sequence of random variables, each having the Gaussian distribution with mean μ n and variance σ n 2. If the distribution of X n converges, then (μ n , σ n 2) converge to (μ, σ 2), and the limit distribution is Gaussian with mean μ and variance σ 2. We recall that if X n converges a.s., then it also converges in distribution.
 
6
This growth condition can be relaxed into \(\vert f(x)\vert \leq C\exp \left (\frac{\vert x\vert ^{2}} {2\alpha } \right )\) for any x, for some positive constants C and α: in that case, the smoothness of the function u is satisfied for t < α only.
 
7
Here again, the boundedness could be relaxed to some exponential growth.
 
8
Meaning that for a deterministic positive constant C, \(\mathbb{P}(U \leq C) = 1\).
 
9
Actually, (19) proves that M is a martingale and the result to be proved is related to the optional sampling theorem.
 
10
Indeed, the result gives uniqueness and not the existence.
 
12
Indeed, we can show that \(\mathbb{E}(\sigma _{M}^{2}) = \mathbb{V}\mathrm{ar}(X)\).
 
13
In fact, it generally depends on the regularity of u.
 
14
This labeling comes from the infinitesimal decomposition of \(\mathbb{E}(f(X_{t}))\) as time is small, \(\partial _{t}\mathbb{E}(f(X_{t}))\vert _{t=0} = L_{b,\sigma ^{2}}^{\mathtt{ABM}}f(x)\), see Proposition 12.
 
15
Integrability is the right assumption.
 
16
That is the sum of \(\sum _{t_{i}\leq t}\vert A_{t_{i+1}} - A_{t_{i}}\vert \) exists and is finite, for instance A is continuously differentiable.
 
17
Leading to the notion of strong solution; the case of non-smooth coefficients is much more delicate and related to weak solutions, see [67].
 
18
Up to a set of zero probability measure.
 
19
To simplify the exposure.
 
20
Uniquely defined if y is close to the boundary.
 
21
Meaning that \(m(O) = \mathbb{E}(R\vert O)\).
 
22
There may be some colinearities within (ϕ j ) 1≤j≤K.
 
23
Also called variance term.
 
24
Squared bias term.
 
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Metadaten
Titel
Introduction to Stochastic Calculus and to the Resolution of PDEs Using Monte Carlo Simulations
verfasst von
Emmanuel Gobet
Copyright-Jahr
2014
DOI
https://doi.org/10.1007/978-3-319-02839-2_3

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