248 12 Absolutely Continuous Local Martingale Measures
stopping timeμ=∞onGcand equal to inf{t|Lt≤^12 Lσ}on the setG.The
outcome
(^1) G=
(
1
Lμ
−
1
Lσ
)
Lσ (^1) G
is the result of a 1-admissible strategy and clearly produces arbitrage. We may
therefore suppose thatP[G∩F]>0 and hence we also have
∫
GUσ>0. Again
this suffices to show thatUσ>0ontheset{Lσ> 0 }and again implies that
T≤ν. The proof of the lemma is complete now.
Proof of the Main Theorem 12.4.2.We now calculate the decomposition of
the continuous semi-martingaleSunderPF.IfS =M+Ais the Doob-
Meyer decomposition ofSunderPthen, underPF we writeS=M ̃+A ̃
whereA ̃t=At+
∫d〈M,U〉s
Us , see [L 77]. This integral exists for the measurePF
since onF the processUis bounded away from 0. A more explicit formula
forA ̃can be found if we use the structure of〈M, U〉. We thereto use the
Kunita-Watanabe decomposition of theL^2 -martingaleUwith respect to the
martingaleM. This is done in the following way (see [J 79]). The space of
allL^2 -martingales of the formα·Mis a stable space and in fact we have
‖(α·M)∞‖ 2 =E[
∫
α′d〈M, M〉α]. The orthogonal projection ofU∞on this
space is given by (β·M)∞for some predictable processβ, where of course
E
[∫
β′d〈M, M〉β
]
<∞.
In this notation we may write:
d〈M, U〉=d〈M, M〉β.
It follows that also
∫
β′d〈M, M〉β<∞a.s. for the measurePF and the
measuredA ̃can be written as
dA ̃=d〈M, M〉
(
ht+
βt
Ut
)
=d〈M, M〉kt.
Here we have putk=h+Uβto simplify notation.
To prove the(NFLVR)property forSunderPF we use the criterion of
Theorem 12.1.3 above.
Step1: the set of 1-admissible integrands forPF is bounded inL^0 (F).
From the properties ofβandhwe deduce that, for the measure,PF,the
integral ∫
∞
0
k′td〈M, M〉kt<∞ PF-a.s..
ThePF-local martingaleL ̃is now defined as
̃Lt=exp
(
−
∫t
0
k′udM ̃u−
1
2
∫t
0
ku′d〈M, M〉uku