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Proof
See [3, Chap. 1.2.4].
Note that in (
10.2
) the integral with respect to the Lévy measure exists since the
integrand is bounded outside of any neighborhood of 0 and
e
iξz
(z
2
)
1
−
+
iξz
1
}
=
O
as
|
z
|→
0
.
{|
z
|≤
1
But there are many other ways to obtain an integrable integrand. We could, for
example, replace 1
by any bounded measurable function
f
: R → R
satisfying
{|
z
|≤
1
}
=
+
O
|
|
|
|→
=
O
|
|
|
|→∞
f(z)
. Different choices
of
f
do not affect
σ
2
and
ν
.But
γ
depends on the choice of the truncation function.
1
(
z
)
as
z
0 and
f(z)
(
1
/
z
)
as
z
If the Lévy measure satisfies
1
|
z
|
ν(
d
z) <
∞
, we can use the zero function as
f
|
z
|≤
and get
1
e
iξz
ν(
d
z),
1
2
σ
2
ξ
2
=−
+
+
−
ψ(ξ)
iγ
0
ξ
(10.3)
R
. We denote this representation by the triplet
(σ
2
,ν,γ
0
)
0
. Furthermore,
with
γ
0
∈ R
if
ν(
d
z) <
∞
,i.e.
X
is a compound Poisson process, we can rewrite (
10.3
)as
R
+
λ
1
2
σ
2
ξ
2
−
e
iξz
)ν
0
(
d
z),
ψ(ξ)
=−
iγ
0
ξ
+
(
1
(10.4)
R
=
with
λ
ν/λ
. We say that
X
is of
finite activity
with
jump intensity
λ
and jump size distribution
ν
0
. If the Lévy measure satisfies
ν(
d
z)
and
ν
0
=
R
>
1
|
z
|
ν(
d
z) <
∞
, then, letting
f
be a constant function 1, we obtain
|
z
|
1
iξz
ν(
d
z),
1
2
σ
2
ξ
2
e
iξz
ψ(ξ)
=−
iγ
c
ξ
+
+
−
+
(10.5)
R
with triplet
(σ
2
,ν,γ
c
)
c
where
γ
c
is called the center of
X
since
E[
X
t
]=
γ
c
t
.We
use the representation (
10.5
) instead of (
10.2
) throughout this work but omit the sub-
script
c
for simplicity. No arbitrage considerations require Lévy processes employed
in mathematical finance to be martingales. The following result gives sufficient con-
ditions of the characteristic triplet to ensure this.
Lemma 10.1.5
Let X be a Lévy process with characteristic triplet (σ
2
,ν,γ)
.
As-
sume
,
and
>
1
e
z
ν(
d
z) <
.
Then
,
e
X
>
1
|
|
∞
∞
z
ν(
d
z) <
is a martingale with
|
z
|
|
z
|
respect to the filtration
F
of X if and only if
σ
2
2
+
(e
z
γ
+
−
1
−
z)ν(
d
z)
=
0
.
R
Proof
We obtain for 0
≤
t<s
using the independent and stationary increments
property
e
X
s
e
X
t
+
X
s
−
X
t
e
X
t
e
X
s
−
X
t
E[
|
F
t
]=E[
|
F
t
]=
E[
]
e
X
t
e
X
s
−
t
e
X
t
e
(t
−
s)ψ(
−
i)
.
=
E[
]=
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