3.1 The Complete Case 35
under the constraint
EQ[XT]=
∑N
n=1
qnξn ≤ x. (3.3)
To verify that (3.2) and (3.3) are indeed equivalent to the original problem
(3.1) above (in the present finite, complete case), note that by Theorem 2.4.2
a random variable (XT(ωn))Nn=1=(ξn)Nn=1can be dominated by a random
variable of the formx+(H·S)T=x+
∑T
t=1Ht∆StiffEQ[XT]=
∑N
n=1qnξn≤
x. This basic relation has a particularly evident interpretation in the present
setting, asqnis simply the price of the asset (^1) {ωn}.
We have writtenξnforXT(ωn) to stress that (3.2) is simply a concave
maximisation problem inRN with one linear constraint which is a rather
elementary problem. To solve it, we form the Lagrangian
L(ξ 1 ,...,ξN,y)=
∑N
n=1
pnU(ξn)−y
(N
∑
n=1
qnξn−x
)
(3.4)
=
∑N
n=1
pn
(
U(ξn)−yqpnnξn
)
+yx. (3.5)
We have used the lettery≥0 instead of the usualλ≥0 for the Lagrange
multiplier; the reason is the dual relation betweenxandywhich will become
apparent in a moment.
Write
Φ(ξ 1 ,...,ξN) = inf
y> 0
L(ξ 1 ,...,ξN,y),ξn∈dom(U), (3.6)
and
Ψ(y)= sup
ξ 1 ,...,ξN
L(ξ 1 ,...,ξN,y),y≥ 0. (3.7)
Note that we have
sup
ξ 1 ,...,ξN
Φ(ξ 1 ,...,ξN)= sup
ξ 1 ,...,ξN
∑N
n=1qnξn≤x
∑N
n=1
pnU(ξn)=u(x). (3.8)
Indeed, if (ξ 1 ,...,ξN) is in the admissible region
{∑
N
n=1qnξn≤x
}
,then
Φ(ξ 1 ,...,ξN)=L(ξ 1 ,...,ξN,0) =
∑N
n=1pnU(ξn). On the other hand, if
(ξ 1 ,...,ξN)satisfies
∑N
n=1qnξn >x, then by lettingy→∞in (3.6) we
note thatΦ(ξ 1 ,...,ξN)=−∞.
Regarding the functionΨ(y) we make the following pleasant observation,
which is the basic reason for the efficiency of the duality approach: using the