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and u as the felicity functions have the same optimal paths as solutions,<br />
so for the sake of the study of the possible solutions of a given family of<br />
C 4 ¡functions, there is no any loss of generality if we assume that ju X j 4<br />
=1<br />
for any member of the family. Nevertheless, in our framework we have<br />
chosen to make the assumption explicitly, because the assumption A6 is not<br />
necessarily invariant after this normalization, that is, if we have an arbitrary<br />
familyU 0 as following<br />
U 0 = © u 0 :D ! < j (u;D) satisfying A1-A7 andu 0 2C 4ª ;<br />
for someB 0 2 < ++ in A6, then the normalized family<br />
¾<br />
U =<br />
½u:D ! < j u= u0<br />
ju 0 X j ,u 0 2U 0<br />
4<br />
may not satisfy A6 for any B 2 < ++ (uniformly), although it will satisfy<br />
A1-A5 and A7.<br />
Note that for any u 2 U and ± 2<br />
³^±;1´<br />
, we have that intL 6= ;, since<br />
S = © x 2 < n + j(x;x) 2D ª ½ L , and intS 6= ; by A3. Therefore, since the<br />
proof of the main theorem of this paper is based on the existence of optimal paths<br />
that can be supported by full Weitzman prices, it will su¢ce to takek 0 2intS<br />
(note thatS½X 1 ; by ³^±;1´ (A4)), and then, by iii) in Theorem 1, n weowill have that,<br />
for allu2U and± 2 ; there exists an optimal path k u;±<br />
t fromk 0 that<br />
can be supported by full Weitzman prices. Furthermore, due to di¤erentiability<br />
and concavity i of u, and interiority of the path, we will have for all u 2 U and<br />
± 2<br />
³^±;1 :<br />
where<br />
D 1 u(k u;± ;k u;± )=± ¡1 q u;± ; D 2 u(k u;± ;k u;± )=¡q u;± (16)<br />
D 1 u(k u;±<br />
t¡1;k u;±<br />
t )=± ¡1 q u;±<br />
t¡1 D 2 u(k u;±<br />
t¡1;k u;±<br />
t )=¡q u;±<br />
t ; (17)<br />
D 1 u(k u;± ;k u;± )=(@=@x)u(x;k u;± )c x=k u;±; D 1 u(kt¡1;k u;± u;±<br />
t )=(@=@x)u(x;k t )c x=k<br />
u;± ;<br />
t¡1<br />
and similarly for D 2 u(k u;±<br />
suppose thatk 0 2intS:<br />
t¡1;k u;±<br />
t ) and D 2 u(k u;± ;k u;± ). Thus, henceforth we will<br />
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