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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 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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