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Definition 16.4.1 We call a d -dimensional Feller process with characteristic triplet
(γ (x), Q(x), ν(x, d z)) a time-homogeneous admissible market model if it satisfies
the following properties.
d
(i) The vector function x
b(x)
∈ R
is smooth and bounded.
d
d
sym
×
∈ R
(ii) The matrix function x
Q(x)
is smooth and bounded and, for all
d , the matrix Q(x) is positive semidefinite.
(iii) The jump measure ν(x, d z) is constructed from d independent, univariate
Feller-Lévy measures with a 1-homogeneous copula function F that fulfills
the following estimate: there is a constant C> 0 such that for all u
∈ R
x
) d
(
R\{
0
}
0
and all n
∈ N
it holds
d
n F(u) C | n |+ 1
1 | u i | n i .
| n |!
min
{| u 1 | ,..., | u d |}
i
=
(iv) For the marginal densities ν i (x i , d z i )
=
k i (x, z) d z the mapping x i
ν i (x i ,B)
) .
(v) There exist univariate Lévy kernels k i (z) , i
is smooth for all B
B
(
R
=
1 ,...,d , with semi-heavy tails,
i.e. which satisfy
C e β | z | ,z<
1 ,
k i (z)
(16.19)
e β + z ,
z> 1 ,
for some constants C> 0, β > 0 and β + > 1. These Lévy kernels satisfy the
following estimates
0
ν i (x i ,B)
k i (z) d z
x i ∈ R
,B
B
(
R
), i
=
1 ,...,d.
B
(vi) Besides, we require the following estimates on the derivatives of k i (x, z)
x k i (x, z) C n + 1 n ! | z | Y i (x) δn 1 ,
z k i (x, z) C n + 1 n ! | z | Y i (x) n 1 ,
for any δ
( 0 , 1 ) , for all 0
=
z, x
∈ R
and Y< 2aswellas Y > 0, Y i (x)
=
Y i + Y i (x) , Y i ∈ R +
and Y i (x)
1 ,...,d .
(vii) Finally, we require F 0 to be a 1-homogeneous Lévy copula and k i (x i ,z i ) to
be Y i (x i ) -stable densities with tail integrals U i (x i ,z i ) , i
S
(
R
) , i
=
=
1 ,...,d such that
Ck i (x, z),
k i (x, z)
0 <
|
z
|
< 1 ,
x
∈ R
,i
=
1 ,...,d,
n F 0 (U 0 (x, z))
1 ···
n F(U(x,z))
C∂ 1 ···
0 <
|
z
|
< 1 ,
for some constant C> 0.
=
Remark 16.4.2 Note that the smoothness assumptions on Y i (x i ) , i
1 ,...,d ,are
necessary in order to obtain symbols as given in Definition 16.2.2 . We confine the
discussion to such symbols in order to use the results of [137] that rely on pseu-
dodifferential calculus for symbols of variable order, cf. [86, 104]. The derivation
of similar results for symbols with lower regularity is open to our knowledge.
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