92 Dynamical Systems
and a utility function u such that the optimal transition function h of
(, u,δ) exhibits a three-period cycle. This construction is based on the
example of Nishimura, Sorger and Yano (Chapter 9).
Here is a special case of Sorger (1992) (the proof of which is due to
T. Mitra). Choose units of measurement so that S = [0, 1], and assume
u(0, 0) = 0, strengthen [A.4] and assume that u : →
R
+
is strictly
concave: u(θ(x, y) +(1 − θ)(x
, y
)) >θu(x, y) +(1 − θ)u(x
, y
), for
0 <θ <1 (where (x, y) ∈,(x
, y
) ∈). Suppose that in this model
(, u,δ) the optimal transition function h is of the form
h(x) = 4x(1 − x)0≤ x ≤ 1. (9.57.1)
Then the discount factor δ must satisfy
δ<
1
2
, (R)
To see how the restriction (R) on δ emerges, note that if the optimal
transition function h is given by (9.57.1) then the sequence
x
∗
=
x
∗
t
∞
0
={(1/2), 1, 0, 0,...} (9.57.2)
is an optimal program from (1/2).
Now, suppose, to the contrary, that δ ≥ (1/2). Define θ = 1/(1 +2δ),
and note that 0 <θ ≤ (1/2). One establishes a contradiction by showing
that a program that starts at (1/2) then goes to θ in the next period and
thereafter follows an optimal program from θ, provides higher discounted
sum of utilities than the program (9.57.2) from 1/2; that is, u[(1/2),θ] +
δV (θ ) > V (1/2).
Since u(0, 0) = 0wehaveV (0) = 0. Now [(1/2),θ] = [θ(1/2) +
θδ(1) + θδ(0), θ (1) +θδ(0) +θδ(0)]. Since ((1/2), 1) ∈and (1, 0) ∈
and (0, 0) ∈, and θ + θδ + θδ = 1, we have [(1/2),θ] ∈by con-
vexity of . Further, strict concavity of u and u(0, 0) = 0 imply that
u((1/2),θ) >θu((1/2), 1) + θδu(1, 0). (9.57.3)
Now, since 1 = h(1/2) and 0 = h(1), we have by the optimality equation
u((1/2), 1) = V (1/2) − δV (1) (9.57.4)
u(1, 0) = V (1) − δV (0) = V (1). (9.57.5)