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STOCHASTIC

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400 MERTON<br />

To derive (91), an "artificial" state variable, x(t), is constructed with<br />

x(t) = 0 while the individual is alive and x(t) — 1 in the event of death.<br />

Therefore, the stochastic process which generates x is defined by<br />

dx = dq and y ^ 1 with probability one (92)<br />

and T is now defined by x as<br />

T = min{f | t > 0 and x(t) = 1}. (93)<br />

The derived utility function, J, can be considered a function of the state<br />

variables W, x, and t subject to the boundary condition<br />

J(W, x, t) = B(W, t) when x = 1. (94)<br />

In this form, example three is shown to be of the same type as examples<br />

one and two in that the occurrence of the Poisson event causes a state<br />

variable to be incremented, and (91) is of the same form as (78) and (83).<br />

A comparison of (91) for the particular case when B = 0 (no bequests)<br />

with (82) suggested the following theorem. 31<br />

THEOREM VI. If r is as defined in (93) and U is such that the integral<br />

E0[f„ U(C, t) dt] is absolutely convergent, then the maximization of<br />

E„[f0 U(C, t) dt] is equivalent to the maximization of

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