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376 MERTON<br />

where pit is the instantaneous correlation coefficient between the Wiener<br />

processes dzt and dij."<br />

Armed with Ito's Lemma, we are now able to formally differentiate<br />

most smooth functions of Brownian motions (and hence integrate<br />

stochastic differential equations of the Ito type). 7<br />

Before proceeding to the discussion of asset price behavior, another<br />

concept useful for working with Ito Processes is the differential generator<br />

(or weak infinitesimal operator) of the stochastic process P(t). Define<br />

the function G(P, t) by<br />

G(P> t) s jim Et [W + ft. + AI-WO^ (2)<br />

when the limit exists and where "E" is the conditional expectation<br />

operator, conditional on knowing P(t). If the Pt(t) are generated by Ito<br />

Processes, then the differential generator of P, SCP , is defined by<br />

d *<br />

Y'spt ' at ' 2 ^ ^ " ept dPj '<br />

^^i/iA+4-+^ii^-<br />

where f = (fx ,...,/„), g = (g,,..., £„), and au = gigip(J. Further, it can<br />

be shown that<br />

6{P, t) = &PIG(P,«)]. (4)<br />

G can be interpreted as the "average" or expected time rate of change of<br />

•This multiplication rule has given_rise to the formalism of writing the Wiener<br />

process differentials as dzt = ^ Vdt where the ^ are standard normal variates<br />

{e.g., see [3]).<br />

7 Warning: derivatives (and integrals) of functions of Brownian motions are similar<br />

to, but different from, the rules for deterministic differentials and integrals. For example,<br />

if<br />

then dP = Pdz. Hence<br />

p(t) = p(0) eSl*-i> = P(0) ««i«-ioi-i

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