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Transcript
The Probability of a Random Walk First Returning to
the Origin at Time t = 2n
Arturo Fernandez
University of California, Berkeley
Statistics 157: Topics In Stochastic Processes Seminar
February 1, 2011
What is the probability that a random walk, beginning at the origin, will
return to the origin at time t = 2n? The walk can move up (+1) or down (-1) at
any one step, with each movements having a probability of 1/2. The answer to
this question involves probability theory, combinatorial identities, and generating
functions.
1
Fernandez
1
2
Introduction: A Random Walk
(Note: The following discussion borrows from Chapter 12 of Grinstead and Snell’s Introduction
to Probability (Online Ed., 1997)1 and Prof. Pitman’s Online Lecture Notes2 )
Definition 1. Let{Xk }∞
k=1 = {X1 , X2 , X3 , ..., Xk , ...} be a sequence of independent and identically distributed (i.i.d) discrete random variables. For all n ≥ 1,
let Sn = X1 + X2 + X3 + · · · + XnP
. The sequence of partial sums {Sn }∞
n=1 , which
X
,
is
called
a
random
walk.
also can be denoted as the series ∞
n=1 n
In this discussion, we consider the case where the random variables Xi share
the following distribution function:
1
2 , if x = ±1
fX (x) =
(1)
0, otherwise
2
k-paths
Definition 2. When graphed on the Cartesian axis, we define a k-path to be
the path a random walk can take up to its k-th step (t = k), the plot of a unique
Sk .
Proposition 1. The probability of a 2m-path returning to the origin is
2m
m
(2)
22m
The argument for this proposition is based on the properties of the binomial
distribution. In this case, we have 2m trials and we want to know the probability
of m succeses, with probabilities p = 1/2 (of a +1 movement) and q = 1/2 (of a
-1 movement). Note that the number of +1 movements must equal the number of
-1 movements, or in this case our Xi s. We also conclude that the path can only
return to the origin at an even time. Therefore,
2m
2m
1
P(m successes in 2m trials) =
m
2
u2m = P0 (S2m = 0) =
3
First Return
Definition 3. A random walk has a first return to the origin at its 2m-th step
if:
1. m ≥ 1
2. S2k 6= 0 ∀k < m
We will express the probability of a random walk’s first return at time t = 2m
as f2m . Also, we define f0 = 0.
1
2
http://www.dartmouth.edu/˜chance/teaching aids/books articles/probability book/pdf.html
http://bibserver.berkeley.edu/150/lectures/lecture11/Lec11.pdf
Fernandez
3
Theorem 1. For n ≥ 1, {f2k } and {u2k } are related by the following equation:
u2n = f0 u2n + f2 u2n−2 + · · · + f2n u0
(3)
Proof. We begin by noting that the expression f2n 22n is equal to the number
of 2n-paths that only touch the origin at the endpoints, that is the on cartesian
coordiantes (0, 0) and (2n, 0). Similarly, u2n 22n is equal to the total number of 2npaths that end at the origin. The collection of these 2n-paths can be partitioned
into n sets, depending on their first return. For example, a path in this collection
that has its first return at t = 2k, consists of a path from (0, 0) to (2k, 0) that
only touches the origin at those endpoints and a path from (2k, 0) to (2n, 0) that
has no restrictions other than the probablistic constraints that we gave the Xi ’s.
Thus, the number of 2n-paths that have their first return at t = 2k is given by
f2k 22k u2n−2k 22n−2k = f2k u2n−2k 22n
If we sum, the right hand side of the above equality, over k, we find that
u2n 22n = f0 u2n 22n + f2 u2n−2 22n + · · · + f2n u0 22n
Dividing both sides by 22n gives (3).
Given this relation, we should now try to express f2n (unkown) in terms of
u2n (known). At this point, we use the properties of generating functions (power
series) to help us simplify the relation given by (3).
4
Generating Functions
We define the following generating functions, as derived from u2m and f2m ,
U (x) =
∞
X
u2m x
m
and F (x) =
m=0
∞
X
f2m xm
m=1
A convolution argument can be simplified as follows
! ∞
!
∞
X
X
F (x)U (x) =
f2m xm
u2k xk
=
=
m=1
∞
n
X X
n=1
∞
X
k=0
!
f2m u2n−2m
xn
m=1
u2n xn
n=1
= U (x) − 1
Which implies that,
1
U (x) − 1
=1−
(4)
U (x)
U (x)
Therefore, if we can find a closed-form solution for U (x), then we will have
one for F (x). We shift focus temporarily to establish some algebraic identities.
F (x) =
Fernandez
5
4
Algebra and Identities
By the Binomial Theorem
n
(1 + x) =
n X
n
k=0
k
xk
∀n ≥ 1
(5)
this can be generalized to
∞ X
a k
(1 + x) =
x
k
a
for |x| < 1
k=0
Also, note that
a
a(a − 1) · · · (a − k + 1)
:=
k!
k
∀a ∈ R
(6)
These identities will help us find the closed-form solution of U (x), we just need
to prove one more claim.
Claim.
1
2n
−2
= 22n (−1)n
n
n
(7)
Proof.
2n
n
1 2n(2n − 1) · · · (n + 1)(n)(n − 1) · · ·
n!
n(n − 1) · · · 1
1
= 2(2n − 1)2(2n − 3)2 · · · (5)2(3)2(1)
n!
1
= 2n · 1 · 3 · · · (2n − 1)
n!
1 1
1
1
1
= 22n ( )( + 1)( + 2) · · · ( + n − 1)
n!
2 2
2
2
1 2n
1
1
1
n
= 2 (−1) (− )(− − 1) · · · (− − n + 1)
n!
2
2
2
1
−2
= 22n (−1)n
n
=
by (6)
Fernandez
6
5
Formulas for U (x) and F (x)
We begin with the closed-form solution of U (x):
U (x) =
∞
X
u2n xn
n=0
∞ X
2n −2n n
=
2
x
n
n=0
1
∞
X
2n
n −2
2−2n xn
=
2 (−1)
n
n=0
∞ 1
X
−2
=
(−x)n
n
by (2)
by (7)
n=0
1
= (1 − x)− 2
by (5)
Recall that
F (x) =
∞
X
f2m xm
m=1
where f2m is the probability of the random walk’s (p = 12 , q = 12 ) first return at
time t = 2m.We continue with an application of the binomial theorem on the
results from above and (4).
F (x) = 1 − U (x)−1
1
= 1 − (1 − x) 2
∞ 1
X
2 (−x)n
=1−
n
n=1
∞ 1
X
2 (−1)n−1 (x)n
=
n
=
n=1
∞
X
f2m xm
m=1
Comparing the coefficients we deduce that:
f2n = (−1)n−1
2
n
2n
n
1
=
(2n −
1)22n
=
u2n
2n − 1