Canonical form for time series
We start with a doubly-infinite time series At each point in time
, in addition to
, we are given an information set
It is natural to assume that with time we know more and more:
for all
. We want to apply the idea used in two simpler situations before:
1) Mean-plus-deviation-from-mean representation: , where
,
,
2) Conditional-mean-plus-remainder representation: having some information set , we can write
, where
,
,
Notation: for any random variable , the conditional mean
will be denoted
.
Following the above idea, we can write . Hence, denoting
,
, we get the canonical form
(1)
Properties
a) Conditional mean of the remainder: , because
. This implies for the unconditional mean
by the LIE.
b) Conditional variances of and
are the same:
c) The two terms in (1) are conditionally uncorrelated:
( is known at time
).
They are also unconditionally uncorrelated: by the LIE
d) Full (long-term) variance of , in addition to
, includes variance of the conditional mean
:
e) The remainders are uncorrelated. When considering for
, by symmetry of covariance we can assume that
. Then, remembering that
is known at time
, by the LIE we have
Question: do the remainders represent white noise?
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