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Asset Pricing John H. Cochrane June 12, 2000

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SECTION 3.5 STATE DIAGRAM AND PRICE FUNCTION<br />

b 0 x =E(xx 0 ) −1 E(yx 0 )x. This ideal is often illustrated by a residual vector ε that is perpendicular<br />

to a plane definedbytherighthandvariablesx. Thus, when the inner product is<br />

defined by a second moment, the operation “project y onto x” isaregression. (If x does not<br />

include a constant, you don’t add one.)<br />

The geometric interpretation of Figure 7 also is valid if we generalize the setup to an<br />

infinite-dimensional state space, i.e. if we think of continuously-valued random variables.<br />

Instead of vectors, which are functions from R S to R, random variables are (measurable)<br />

functions from Ω to R. Nonetheless, we can still think of them as vectors. The equivalent<br />

of R s is now a Hilbert space L 2 , which denotes spaces generated by linear combinations<br />

of square integrable functions from Ω to the real line, or the space of random variables with<br />

finite second moments. We can still define an “inner product” between two such elements<br />

by x · y = E(xy), andp(x) =E(mx) can still be interpreted as “m is perpendicular to<br />

(hyper)planes of constant price.” Proving theorems in this context is a bit harder. You can’t<br />

just say things like “we can take a line perpendicular to any plane,” such things have to be<br />

proved. Sometimes, finite-dimensional thinking can lead you to errors, so it’s important to<br />

prove things the right way, keeping the finite dimensional pictures in mind for interpretation.<br />

Hansen and Richard (1987) is a very good reference for the Hilbert space machinery.<br />

63

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