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d
. The spaces of order
m
(x)
R
≤
where
u
is the zero extension of
u
to all of
0,
d
, are defined by duality. We have
∀
x
∈ R
( H
−
m
(x)
(G))
∗
,
where duality is understood with respect to the “pivot” space
L
2
(G)
,i.e.
L
2
(G)
∗
=
L
2
(G)
.
H
m
(x)
(G)
:=
Remark 16.2.3
In the Black-Scholes case,
H
1
(
R
d
)
is obtained as the domain of the
corresponding bilinear form while
H
0
(G)
is the domain in the localized case, see
Chap. 4. In the Lévy case, we obtain anisotropic Sobolev spaces as in (
16.9
) and the
spaces
H
s
(G)
in the localized case for
Q
=
0, see Chap. 14.For
Q>
0 the domains
are equal to those in the Black-Scholes case, cf. [134, Theorem 4.8].
Several examples of Feller processes are provided in this section. The methods
presented in this work are not applicable to all of them. But admissible market mod-
els are derived ensuring the well-posedness of the corresponding pricing equations
and the applicability of finite element methods. Subordination can be used to con-
struct Feller processes. However, the structure of the symbol is more involved than
in the Lévy setting. We also present a construction of Feller processes using Lévy
copulas.
16.3 Subordination
Many Lévy models in the context of option pricing are constructed via subordination
of a Brownian motion by a corresponding stochastic clock, e.g. an NIG process [8]
or a VG process [119]. We describe a similar construction for Feller processes and
point out similarities and differences to the Lévy case. Bernstein functions play a
crucial role in the representation of subordinators.
C
∞
(
0
,
Definition 16.3.1
A function
f(x)
∈
∞
)
is called a Bernstein function if
1
)
k
∂
k
f(x)
∂x
k
f
≥
0
,(
−
≤
0
,
∀
k
∈ N
.
e
−
cx
,
c
Example 16.3.2
The functions
f
1
(x)
=
c
,
f
2
(x)
=
cx
and
f
3
(x)
=
1
−
≥
0
are Bernstein functions.
Bernstein functions admit the following representation.
Theorem 16.3.3
For any Bernstein function f(x) there exists a measure μ on
(
0
,
∞
)
,
with
∞
s
∞
s
μ(
d
s) <
1
+
0
+
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