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Then, using the
θ
-scheme for the time discretization, we obtain the matrix problem
Find
u
m
+
1
N
∈ R
such that for
m
=
0
,...,M
−
1
θt
A
J
)
u
m
+
1
θ)t
A
J
)
u
m
,
+
=
−
−
(10.28)
(
M
(
M
(
1
u
0
N
=
u
0
,
with
A
J
N
×
N
∈ R
defined for
i
=
1
,...,N
,
h
2
2
k
0
k
1
,
1
k
1
A
i,i
=
−
−
h
2
2
k
j
k
j
−
1
,j
1
A
i,i
+
j
=
k
j
+
1
−
−
=
1
,...,N
−
i,
h
2
2
k
j
k
j
−
1
,j
1
A
i,i
−
j
=
k
j
+
1
−
−
=
1
,...,i
−
1
.
The variables
k
j
,
k
j
can be expressed in closed form using
k
(
−
3
)
and
k
(
−
4
)
:
h
h
k
0
k
(
−
2
)
(y
=
−
x)
d
y
d
x
0
0
k
(
−
2
)
(y
−
x)
d
y
d
x
h
x
h
k
(
−
2
)
(y
−
x)
d
y
+
=
0
0
x
h
k
(
−
3
)
(
0
−
)
k
(
−
3
)
(
0
+
)
d
x
k
(
−
3
)
(
k
(
−
3
)
(h
=
−
−
x)
+
−
x)
−
0
h
k
(
−
3
)
(
0
−
)
k
(
−
3
)
(
0
+
)
+
k
(
−
4
)
(
k
(
−
4
)
(
0
−
)
k
(
−
4
)
(
0
+
)
=
−
−
h)
−
−
+
k
(
−
4
)
(h),
k
j
2
k
(
−
4
)
(j h)
k
(
−
4
)
((j
k
(
−
4
)
((j
1
.
Note that, using finite elements, we computed the matrix entries exactly (assuming
that the antiderivatives
k
(
−
3
)
and
k
(
−
4
)
of the density function
k(z)
are explicitly
available) on the subspace
V
N
⊂
V
, and therefore still obtain the optimal conver-
gence rate
=−
+
−
1
)h)
+
+
1
)h),
j
=
1
,...,N
−
(h
2
)
whereas for finite differences we approximated the integral and
only obtain convergence rate
O
O
(h)
.
Remark 10.6.2
As already noted in Remark
10.6.1
, if the Lévy measure
ν
satis-
fies the assumptions
or
1
|
z
|
ν(
d
z) <
∞
1
ν(
d
z) <
∞
, we have the bilinear
|
z
|≤
|
z
|≤
forms
a
J
(ϕ, φ)
ϕ
(y)φ(x)k
−
1
(y
=
−
x)
d
y
d
x,
G
G
λ
a
J
(ϕ, φ)
=
ϕ(y)φ(x)k(y
−
x)
d
y
d
x
−
ϕ(x)φ(x)
d
x,
G
G
G
and similar discretization schemes can be derived.
Example 10.6.3
To have an exact solution available, we consider the variance
gamma model [118] with parameter
σ
0
.
3. The den-
sity of the variance gamma distribution for the log-returns has not only “fatter” tails
=
0
.
3,
ϑ
=
0
.
25 and
θ
=−
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