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Using [143, Theorem 25.18], it suffices to show that there exist a constant C(T,σ) >
0 such that
e q | X T | 1
x
C(T,σ)e γ 1 R + γ 2 | x | .
E
} |
X t =
{|
X T |
>R
σ 2 / 2, with the transition probability p T t ,
We have for μ
=
r
e q | X T | 1
} | X t = x
e q | z + x | 1
E
=
p T t (z) d z
{|
X T |
>R
{|
z
+
x
|
>R
}
R
e q | x |
1
2 πσ 2 (T
e (z μ(T t)) 2 /( 2 σ 2 (T t)) d z
e q | z | 1 {| z + x | >R }
t)
R
C 1 (T , σ ) e q | x |
e (q + μ/σ 2 ) | z | 1 {| z + x | >R } e z 2 /( 2 σ 2 (T t)) d z
R
C 1 (T , σ ) e q | x |
e q μ/σ 2 )(R −| x | ) e η | z | e z 2 /( 2 σ 2 (T t)) d z
R
C 1 (T , σ ) e γ 1 R + γ 2 | x |
e η | z | e z 2 /( 2 σ 2 (T t)) d z,
R
q . Since
R
e η | z | e z 2 /( 2 σ 2 (T t)) d z<
μ/σ 2 , and γ 2 =
with γ 1 =
η
q
γ 1 +
for
μ/σ 2 .
any η> 0, we obtain the required result by choosing η>q
+
Remark 4.3.2 We see from Theorem 4.3.1 that v R
v exponentially for a fixed x
→∞
as R
. The artificial zero Dirichlet barrier type conditions at x
R are not
describing correctly the asymptotic behavior of the price v(t,x) for large
|
x
|
. Since
the barrier option price v R is a good approximation to v for
|
x
|
R , R should be
selected substantially larger than the values of x of interest.
The barrier option price v R can again be computed as the solution of a PDE
provided some smoothness assumptions.
C 1 , 2 (J
C 0 (J
Theorem 4.3.3 Let v R (t, x)
× R
)
× R
) beasolutionof
BS v R
t v R + A
rv R =
0
(4.12)
on ( 0 ,T)
×
G where the terminal and boundary conditions are given by
g(e x ),
G c .
v R (T , x)
=
x
G,
v R (t, x)
=
0
on ( 0 ,T)
×
Then , v R (t, x) can also be represented as in ( 4.11 ).
Now we can restate the problem ( 4.8 ) on the bounded domain:
L 2 (J
H 0 (G))
H 1 (J
L 2 (G)) such that
Find u R
;
;
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