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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)
0 ξ
(10.3)
R
. We denote this representation by the triplet 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 0 ( d z),
ψ(ξ) =− 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)
=−
c ξ
+
+
+
(10.5)
R
with triplet 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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