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Quick review on ODEs Brownian motion Densities of the solution Stochastic Differential Equations SIMBA, Barcelona. David Ba nos April 7th, 2014. SIMBA, Barcelona. David Ba nos Stochastic Differential Equations Quick review on


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Quick review on ODE’s Brownian motion Densities of the solution

Stochastic Differential Equations

SIMBA, Barcelona. David Ba˜ nos April 7th, 2014.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Quick review on ODE’s Brownian motion Densities of the solution

Table of contents

1 Quick review on ODE’s 2 Brownian motion 3 Densities of the solution

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Quick review on ODE’s Brownian motion Densities of the solution

Ordinary Differential Equation

Let f : [t0, T] × Rd → Rd and x : [0, T] → Rd dx(t) = f (t, x(t))dt, t0 t T, x(t0) = x0 ∈ Rd. (1) If a solution to the Cauchy problem (1) exists we can write x(t) = x0 + t

t0

f (s, x(s))ds, t0 t T. (2)

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Ordinary Differential Equation

Let f : [t0, T] × Rd → Rd and x : [0, T] → Rd dx(t) = f (t, x(t))dt, t0 t T, x(t0) = x0 ∈ Rd. (1) If a solution to the Cauchy problem (1) exists we can write x(t) = x0 + t

t0

f (s, x(s))ds, t0 t T. (2) Example If f (s, x(s)) = x(s) then (1) has a closed form solution given by x(t) = x0et.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Existence and Uniqueness of Solutions

Picard-Lindel¨

  • f theorem (suff. cond. for local existence and

uniqueness) Peano’s theorem (suff. cond. for existence) Carath´ eodory’s theorem (weaker version of Peano’s theorem) Okamura’s theorem (nec. an suff. conditions for uniqueness) ...

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Brownian motion

In 1827, while examining grains of pollen of the plant Clarkia pulchella suspended in water under a microscope, Brown

  • bserved small particles ejected from the pollen grains,

executing a continuous jittery motion. He then observed the same motion in particles of inorganic matter, enabling him to rule

  • ut the hypothesis that the effect was life-related. Although Brown

did not provide a theory to explain the motion, and Jan Ingenhousz already had reported a similar effect using charcoal particles, in German and French publications of 1784 and 1785, the phenomenon is now known as Brownian motion.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Brownian motion and SDE’s

Let (Ω, F, P) be a probability space. A stochastic process B : [0, T] × Ω → Rd defined on (Ω, F, P) is said to be a standard Brownian motion (moviment Browni` a) or a Wiener process if

1 B0 = 0, P − a.s. 2 Given two times s, t ∈ [0, T], s < t, the law of Bt+s − Bs is

the same as Bt.

3 The increments Bt − Bs and Bv − Bu are independent for all

u < v, s < t.

4 Bt ∼ N(0, t) for all t ∈ [0, T]. SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Brownian motion and SDE’s

Let (Ω, F, P) be a probability space. A stochastic process B : [0, T] × Ω → Rd defined on (Ω, F, P) is said to be a standard Brownian motion (moviment Browni` a) or a Wiener process if

1 B0 = 0, P − a.s. 2 Given two times s, t ∈ [0, T], s < t, the law of Bt+s − Bs is

the same as Bt.

3 The increments Bt − Bs and Bv − Bu are independent for all

u < v, s < t.

4 Bt ∼ N(0, t) for all t ∈ [0, T].

In addition, we can choose a version such that Bt is almost surely

  • continuous. The existence of a stochastic process defined as above

is not immediate (Kolmogorov’s existence theorem).

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Brownian motion

To have intuition working with {Bt(ω), t ∈ [0, T], ω ∈ Ω} we present four sample paths of a standard Brownian motion.

Figure: Four realizations of a standard Brownian motion on the

interval [0, 1].

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Stochastic Differential Equation

A (ordinary) stochastic differential equation with additive noise is an equation of the form: dXt= b(t, Xt)dt + σdBt, t ∈ [0, T], X0 = x ∈ Rd (3) where σ is a parameter often called volatility.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Stochastic Differential Equation

A (ordinary) stochastic differential equation with additive noise is an equation of the form: dXt= b(t, Xt)dt + σdBt, t ∈ [0, T], X0 = x ∈ Rd (3) where σ is a parameter often called volatility. Then if a solution to (4) exists we write Xt = x + t b(s, Xs)ds + σBt.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Stochastic Differential Equation

A (ordinary) stochastic differential equation with additive noise is an equation of the form: dXt= b(t, Xt)dt + σdBt, t ∈ [0, T], X0 = x ∈ Rd (3) where σ is a parameter often called volatility. Then if a solution to (4) exists we write Xt = x + t b(s, Xs)ds + σBt. Observe that for each ω ∈ Ω Xt(ω) = x + t b(s, Xs(ω))ds + σBt(ω).

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Stochastic Differential Equation

A (ordinary) stochastic differential equation is an equation of the form: dXt= b(t, Xt)dt + σ(t, Xt)dBt, t ∈ [0, T], X0= x ∈ Rd (4) where b : [0, T] × Rd → Rd is a measurable function and σ : [0, T] × Rd → Rd×m is a suitable function.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Quick review on ODE’s Brownian motion Densities of the solution

Stochastic Differential Equation

A (ordinary) stochastic differential equation is an equation of the form: dXt= b(t, Xt)dt + σ(t, Xt)dBt, t ∈ [0, T], X0= x ∈ Rd (4) where b : [0, T] × Rd → Rd is a measurable function and σ : [0, T] × Rd → Rd×m is a suitable function. Then if a solution to (4) exists we write Xt = x + t b(s, Xs)ds + t σ(s, Xs)dBs.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Stochastic Differential Equation

Figure: Two samples of Brownian motion with drift at different

starting points.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Stochastic Differential Equation

Figure: Three samples fo a geometric Brownian motion with

µ = 0.05 and σ = 0.02.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Path properties of the Brownian motion

The function the function t → Bt(ω) has the following properties: Takes both strictly positive and strictly negative numbers on (0, ε) for every ε > 0. It is continuous everywhere but differentiable nowhere. It has infinite variation. Finite quadratic variation. The set of zeros is a nowhere dense perfect set of Lebesgue measure 0 and Hausdorff dimension 1/2. H¨

  • lder-continuous paths of index α < 1/2.

Hausdorff dimension 1.5.

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Stochastic integral

Let Bt(ω), t ∈ [0, T], ω ∈ Ω be a standard Brownian motion. Consider a process Xt satisfying some conditions. Then T XtdBt := lim

n→∞

  • [ti,ti+1]∈πn

Xti(Bti+1 − Bti) (Itˆ

  • integral)

T XtdBt := lim

n→∞

  • [ti,ti+1]∈πn

X ti +ti+1

2

(Bti+1−Bti) (Stratonovich integral) The convergence above is in probability (in fact, in L2(Ω)).

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Back to ODE theory

Consider the Cauchy problem

  • dx(t) = b(t, x(t))dt, t ∈ [0, T],

x(t0) = x0 ∈ R. Theorem (Picard-Lindel¨

  • f)

If b is continuous in t and Lipschitz continuous in x then there exists a unique (local) strong solution to the Cauchy problem above.

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Back to SDE theory

Consider the SDE

  • dXt = b(t, Xt)dt + dBt, t ∈ [0, T],

X0 = x ∈ R. Theorem (Stochastic version of Existence and Uniqueness) If b satisfies one of the following conditions then there exists a unique (global) strong solution to SDE above. b is Lipschitz continuous in x uniformly in t. b is bounded and measurable. b is of linear growth, i.e. |b(t, x)| C(1 + |x|). b satisfies T

  • R |b(t, x)|qdx

p/q dt < ∞. ...

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Densities of solutions to SDE’s

Xt is a process which for each fixed t, Xt is a random variable and hence it has a law but not necessarily a density.

Figure: Devil’s staircase function. (taken from Wikipedia)

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Densities of solutions to SDE’s

Hence, it is not even clear whether the solution to an SDE has a density! A sufficient condition for Xt to admit a density is the following: E

  • exp

1 2 T b(Xt)2dt

  • < ∞ (Novikov’s condition)

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Densities of solutions to SDE’s

A lot of research on this direction has been done. Given an SDE with some conditions on b and σ. Does Xt admit a density? How regular is it?

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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References

Karatzas, Ioannis, Shreve, Steven E. Brownian motion and Stochastic Calculus. Springer 1998. David Nualart, The Malliavin Calculus and Related Topics. Springer 2006. Bernt Øksendal. Stochastic Differential Equations. Springer.

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations

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Thank you!

SIMBA, Barcelona. David Ba˜ nos Stochastic Differential Equations