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Complex Analysis and Brownian Motion
Yuxuan Zhang
June 5, 2013
Abstract
This paper discusses some basic ideas of Brownian motion. Beginning
from measure theory, this paper makes a brief introduction to stochastic
process, stochastic calculus and Markov property, recurrence as well as
martingale related to Brownian motion. Later, it shows an application
of Brownian motion which applies Brownian motion to prove Liouville’s
theorem in complex analysis.
Contents
1 Introduction 2
2 Brownian Motion 3
2.1 Sigma Algebra . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3
2.2 Stochastic Process . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2.3 Brownian Motion . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2.4 Some related properties for Brownian motion . . . . . . . . . . . 6
2.4.1 Markov property . . . . . . . . . . . . . . . . . . . . . . . 6
2.4.2 Recurrence . . . . . . . . . . . . . . . . . . . . . . . . . . 6
2.4.3 Martingale . . . . . . . . . . . . . . . . . . . . . . . . . . 8
3 Stochastic Calculus 9
3.1 Introduction to Stochastic Calculus . . . . . . . . . . . . . . . . . 9
3.2 Ito Process and Ito’s Formula . . . . . . . . . . . . . . . . . . . . 10
4 The Application of Brownian Motion 12
4.1 Proof of Liouville’s theorem from Brownian motion . . . . . . . . 12
1
Complex Analysis and Brownian Motion 2
1 Introduction
The first observation to Brownian Motion was in 1827 by British botanist,
Robert Brown. When studying pollen grains under the microscope, he sur-
prisingly found that the pollen grains are not static but instead, move in some
irregular way. However, at that time, Brown cannot find out the mechanisms
which caused this strange motion. The puzzle existed for about 100 years un-
til Albert Einstein, who published a related paper in 1905, suggested that the
motion which Brown observed was caused by the impact from the moving wa-
ter molecules. Molecules constantly bombard the pollen grain and due to the
imbalance force from each direction, the pollen grain will move in a constantly
changing path. Brownian motion is a great example which we can directly
observe the consequence of the moving of unobservable particles and this obser-
vation provides a solid confirmation for the existence to the molecules and atoms.
Fig 1 A three dimensional Brownian Motion for times 0 ≤ t ≤ 2 [4].
Scientists have studied Brownian Motion for a long time, and mathematicians
also, from their perspective, provide their explanation and prediction result to
Brownian Motion. Brownian Motion now is not a mysterious observation to
confuse people any more, but instead, we apply what we get from the study to
Brownian Motion to help us determine more and more complex phenomenon
in this world. For example, the use of Brownian Motion to predict the Stock
market [5] and the application in the prediction of heat flow [1]. In this paper,
we will discuss the study of Brownian Motion structured in math related to
complex analysis and later, we will consider some examples related to Brownian
Motion.
Complex Analysis and Brownian Motion 3
2 Brownian Motion
In this section, we’ll cover up some definition and basic properties for Brownian
Motion.
2.1 Sigma Algebra
As the steal theoretical foundation of the modern probability, the measure the-
ory provides us a pure mathematical perspective of probability knowing from
the classical, frequency or subjective interpretations to probability from philos-
ophy. We’ll here only discuss some basic theorems building up the whole system.
Definition 2.1.1 (σ − algebra) A collection F of subsets of a set X is
called a σ − algebra if
• 1. ∅ ∈ F;
• 2. if A ∈ B, then A′ ∈ F;
• 3. if A , A , ... , A ,... ∈ B, then S∞ A ∈ F.
1 2 n i=1 i
The pair (X,F) is a field of sets, called a measurable space.
Next, we will give a formal definition of the probability space as well as the
probability measure.
Definition 2.1.2 (Probability Measure) A probability measure on a given
probability space is function υ satisfying the following conditions:
• 1. υ is a function map event space to unit interval [0, 1], or υ : Ω 7→ [0,1];
S P
• 2. υ( i∈I Ei) = i∈I υ(Ei)
Definition 2.1.3 (Probability Space) A probability space is a triple (Ω, F,
P) consisting of:
• the sample space Ω as an arbitrary non-empty set;
Ω
• the σ-algebra F ⊆ 2 ;
• the probability measure P : F 7→ [0,1] .
And the following is the formal definition of filtration, which will be used
later when defined stopping time and martingale.
Definition 2.1.4 (Filtration) A filtration on (Ω,F,P) is a collection mea-
surable sets F : t ≥ 0 which satisfies F ⊂ F ⊂ F if s < t.
t s t
Complex Analysis and Brownian Motion 4
2.2 Stochastic Process
Also called as random process, the stochastic process is often used to show the
evolutionofsomerandomvaluebasedontime. Notlikehowdeterministicprocess
works, which predicts the process can only develop in one way, stochastic pro-
cess allows some indetermination.
Definition 2.2.1 (Stochastic Process) Given a probability space (Ω,F,P)
and a measurable space (S,Σ), an S-valued stochastic process is a collection of
S-valued random variables on Ω, indexed by a totally ordered time set T. That
is, a stochastic process B is a collection
{Bt : t ∈ T}
where each B is an S-valued random variable on Ω. The space S is then called
i
the state space of the process.
In the study of stochastic process, there is a important concept called stopping
time. As a specific type of ”random time”, stopping time is a random variable
related to time with respect to the event space Ω. The following is the formal
definition of stopping time based on filtration.
Definition 2.2.2 (Stopping time) A random variable T : Ω 7→ [0,∞] de-
fined on a filtered probability space is called a stopping time with respect to the
filtration F if the set x ∈ Ω : T(x) ≤ t ∈ Ft for all t.
One of the example of stopping time is the first occasion of the expected event.
From stopping time, we can decide whether T ≤ t simply by knowing the states
of the stochastic process until time t [6].
2.3 Brownian Motion
Now, based on our theories above, we’ll be able to give the formal definition of
Brownian motion based on measure theory.
Definition 2.3.1 (d − dimensional Brownian Motion) A d-dimensional
Brownian motion is a stochastic process Bt : Ω 7→ R from the probability space
(Ω,F,P) to Rd such that the following properties hold:
• 1. (Independent Increments) For any finite sequence of times t0 < t1 <
... < tn, the distributions Bt −Bt for i = 1,...,n are independent,
i+1 i
• 2. For all ω ∈ Ω, the parametrization function t 7→ Bt(ω) is continuous,
• 3. (Stationary) For any pair s,t ≥ 0, let B −B ∈A,
s+t s
Z 1 −|x|2/2t
P(Bs+t −Bs) = A (2πt)d/2e dx.
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