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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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