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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 )
a J (ϕ, φ)
(x))φ(x)ν( d z) d x.
(10.22)
:=
(ϕ(x
+
z)
ϕ(x)
R
R
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