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Example 11.2.2
(Black-Scholes model) We consider a one-dimensional diffusion
process
X
with the infinitesimal generator
1
2
σ
2
∂
x
f(x).
For the sensitivity of the price with respect to the volatility
σ
, the set of admissible
parameters
1
2
σ
2
∂
xx
f(x)
−
BS
f )(x)
=
(
A
S
η
is
S
η
= R
+
with
η
=
σ
.Wehave
(
A
V
∗
),
(δσ )f )(x)
=
δσσ
0
∂
xx
f(x)
−
δσσ
0
∂
x
f(x)
∈
L
(
V
,
with
δσ
∈ R =
C
. The Dirichlet form
a(δσ
;·
,
·
)
appearing in the weak formulation
(
11.8
)of
u(δσ )
is given by
;
=
δσσ
0
(∂
x
ϕ,∂
x
φ)
+
δσσ
0
(∂
x
ϕ,φ).
a(δσ
ϕ,φ)
In this setting,
V
=
V
=
H
0
(G)
.
Example 11.2.3
(Tempered stable model) We consider a one-dimensional pure
jump process
X
with the tempered stable density
k
as in (10.10) and infinitesimal
generator
J
f )(x)
zf
(x))k(z)
d
z.
(
A
=
(f (x
+
z)
−
f(x)
−
R
For the sensitivity of the price with respect to the jump intensity parameter
α
of the
Lévy process
X
,wehave
S
η
=
=
(
0
,
2
)
with
η
α
and
δα
(
A
zf
(x))k(z)
d
z
(
V
,
V
∗
),
(δα)f )(x)
=
(f (x
+
z)
−
f(x)
−
∈
L
R
where the kernel
k
is given by
k(z)
:= −
ln
|
z
|
k(z).
It is easy to check that
,
|
k(z)
d
z<
>
1
k(z)
d
z<
1
z
2
∞
∞
. In this setting,
|
z
|≤
z
|
V
=
H
α/
2
+
ε
(G)
⊂
H
α/
2
(G)
=
V
,
ε>
0.
For the discretization of (
11.7
), (
11.8
), we can use either finite differences or
finite elements. Here, we consider the finite element method and obtain the matrix
form of (
11.8
)
u
m
+
1
N
Find
∈ R
such that for
m
=
0
,...,M
−
1
,
u
m
+
1
u
m
t
A
(θ
u
m
+
1
θ)
u
m
),
(
M
+
θt
A
)
=
(
M
−
(
1
−
θ)t
A
)
−
+
(
1
−
u
0
=
0
,
A
is matrix of the Dirichlet form
A
ij
where
a(δη
;·
,
·
)
in the basis of
V
N
,
=
N
, and
u
m
+
1
,
m
a(δη
;
b
j
,b
i
)
for 1
≤
i, j
≤
=
0
,...,M
−
1, is the coefficient vector
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