190 CHAPTER 5. BROWNIAN MOTION
by property 1 of the definition of standard Brownian motion.
A routine (but omitted) computation of the fourth moment of the normal
distribution shows that
E
[
Wnk^2
]
= 2t^2 / 4 n.
Finally, by property 2 of the definition of standard Brownian motion
E[WnkWnj] = 0,k 6 =j.
Now, expanding the square of the sum, and applying all of these computa-
tions
E
{ 2 n
∑
k=1
Wnk
} 2
=
∑^2 n
k=1
E
[
Wnk^2
]
= 2n+1t^2 / 4 n= 2t^2 / 2 n.
Now apply Chebyshev’s Inequality to see:
P
[∣
∣
∣
∣
∣
∑^2 n
k=1
Wnk
∣
∣
∣
∣
∣
>
]
≤
2 t^2
^2
(
1
2
)n
.
Now since
∑
(1/2)nis a convergent series, the Borel-Cantelli lemma implies
that the event ∣
∣
∣
∣
∣
∑^2 n
k=1
Wnk
∣
∣
∣
∣
∣
>
can occur for only finitely manyn. That is, for any >0, there is anN,
such that forn > N ∣
∣
∣
∣
∣
∑^2 n
k=1
Wnk
∣
∣
∣
∣
∣
< .
Therefore we must have that limn→∞
∑ 2 n
k=1Wnk= 0, and we have established
what we wished to show.
Remark.Here’s a less rigorous and somewhat different explanation of why
the squared variation of Brownian motion may be guessed to bet, see [5].
Consider
∑n
k=1
(
W
(
kt
n
)
−W
(
(k−1)t
n