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The
removal of drift
is important for stability of the numerical algorithm. For nota-
tional simplicity, we also removed the interest rate
r
.
Remark 10.3.4
If the Lévy measure satisfies
1
|
z
|
ν(
d
z) <
∞
, we remove the
|
z
|≤
drift
γ
0
which is given, due to the martingale condition, by
σ
2
2
−
(e
z
γ
0
=−
−
1
)ν(
d
z),
R
and obtain the generator
1
2
σ
2
∂
xx
f(x)
J
f )(x)
(
A
=
+
(f (x
+
z)
−
f (x))ν(
d
z).
R
10.4 Variational Formulation
For the variational formulation, we need Sobolev spaces of fractional order, i.e.
H
s
(
)
,
s>
0. For any integer
m
, we defined the
H
m
-norm using the derivative
∂
m
(see Sect. 3.1). Equivalently, we can also define the norm using the Fourier transfor-
mation. In particular, for
∂
m
u
∈
L
2
(
R
)
we have, by using Plancherel's theorem,
R
2
π
2
π
∂
m
u(ξ)
2
d
ξ
∂
m
u(x)
2
d
x
2
m
2
d
ξ,
|
|
=
=
|
ξ
|
|
u(ξ )
|
R
R
R
(
2
π)
−
1
e
−
iξz
u(z)
d
z
denotes the Fourier transform of
u
. Therefore,
we can define an equivalent
H
s
-norm for
s>
0via
where
u(ξ)
=
2
+|
ξ
|
)
2
s
2
d
ξ,
u
H
s
(
R
)
:=
(
1
|
u(ξ )
|
R
and set
H
s
(
L
2
(
R
)
:= {
u
∈
R
)
:
u
H
s
(
R
)
<
∞}
.Wealsoset
1 if
σ>
0
,
α/
2 f
σ
ρ
=
0
,
with
α
giveninAssumption
10.2.3
. The variational formulation of the PIDE (
10.19
)
reads
=
L
2
(J
H
ρ
(
H
1
(J
L
2
(
;
R
∩
;
R
Find
u
∈
))
))
such that
a
J
(u, v)
H
ρ
(
(∂
t
u, v)
+
=
0
,
∀
v
∈
R
),
a.e. in
J,
(10.21)
u(
0
)
=
u
0
,
g(e
x
)
and the bilinear form
a
J
(
H
ρ
(
H
ρ
(
where
u
0
(x)
:=
·
,
·
)
:
R
)
×
R
)
→ R
is given
by
1
2
σ
2
(ϕ
,φ
)
a
J
(ϕ, φ)
zϕ
(x))φ(x)ν(
d
z)
d
x.
(10.22)
:=
−
(ϕ(x
+
z)
−
ϕ(x)
−
R
R
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