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Fig. 5.1
American put option
Denoting by
T t,T the set of all stopping times for S t with values in the interval
(t, T ) , the value of an American option is given by
τ T t,T E e r(τ t) g(S τ )
s .
V(t,s)
:=
sup
|
S t =
(5.1)
As for the European vanilla style contracts, there is a close connection between
the probabilistic representation ( 5.1 ) of the price and a deterministic, PDE based
representation of the price. We have
Theorem 5.1.1 Let v(t,x) be a sufficiently smooth solution of the following system
of inequalities
BS v
t v
A
+
rv
0
in J
× R
,
g(e x )
v(t,x)
in J
× R
,
(5.2)
BS v
(∂ t v
A
+
rv)(g
v)
=
0
in J
× R
,
g(e x )
v( 0 ,x)
=
in
R
.
Then , V(T t,e x ) = v(t,x) .
A proof can be found in [15], we also refer to [98] for further details. For each
J there exists the so-called optimal exercise price s (t)
t
( 0 ,K) such that for all
s (t) the value of the American put option is the value of immediate exercise,
i.e. V(t,s) = g(s) , while for s>s (t) the value exceeds the immediate exercise
value, see Fig. 5.1 .
s
s>s (t)
The region
C := {
(t, s)
|
}
is called the continuation
c of
region and the complement
is the exercise region . Since the optimal exercise
price is not known a priori, it is called a free boundary for the associated pricing PDE
and the problem of determining the option price is then a free boundary problem .
Note that the inequalities ( 5.2 ) do not involve the free boundary s (t) .
C
C
Remark 5.1.2 In the Black-Scholes model, the derivative of V at x = s (t) is con-
tinuous which is known as the smooth pasting condition. This does not hold for pure
jump models.
 
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