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In this lecture, we will take about
invertibility of stochastic processes.

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It's going to be Introduction
to Invertibility.

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So objective is to learn invertibility
of a stochastic process.

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So let's look at these Two MA(1),
Moving Average of all through one models.

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Model 1 is Xt = Zt + 2Zt-1,

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Model 2 will have instead of
2 will have half of Zt-1.

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So what we want to do first,

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we'd like to point out the covariance
function of model one.

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What is the definition of
auto covariance function?

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Gamma (k) is basically covariance,
with an Xt plus k and Xt, right?

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So, basically the gamma (k) depends
on the difference between the steps,

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not Xt, not Xt + k.

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But k, the number of the lags in
between those two random variables.

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And we put the definition of Xt + k
into it for model 1 and xt and three

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which ez plus 2 zt minus 1 and then we try
to use the covariance, we expand this.

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Now the recipe takes the covariance
of zt plus k with the zt,

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zt plus k with zt minus 1.

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This term, with zt and
the same term with 2 zt minus 1.

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Now realize the full level,
if k is greater than 1,

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which would mean that t plus k minus
1 is greater than t, in other words,

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these guys are actually uncorrelated.

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There is no covary that
correlates the 0 between them.

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In other words, if k is greater than 1,
our gamma k is 0.

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This is
Theoretical Auto Covariance Function.

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Now if k is 0, exactly 0, that would
mean we are looking at gamma 0, right.

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And gamma 0 is basically the variance,
the variance of this expression.

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And we can see that this is
basically covariance Zt Zt,

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and covariance Zt Z2- 1 is going to
be 0 because they are uncorrelated.

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Zt- 1, Zt will be 0, but that Zt-
1 will have another variance here.

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The first Covariant will be most Gamma.

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I'm sorry Sigma squared and

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this one another Sigma squared and
then we'll get five Sigma squared.

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The Sigma is standard deviation
of the disturbance for

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k = 1, we write the definition of xt + 1,

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which is Zt+1 + 2Zt, we expand it,

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there's only correlated guys are 2Zt and
Zt, and that will give us 2 sigma square.

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If k is negative of course, gamma k,

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this is the covariance,
it's even function of K, so

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gamma K is same thing as gamma negative K
.So if i write auto covariance function.

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Auto covariance function looks like
this starting problem from lag two so

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great than lag one.

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Starting with Lag 2.

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We have n covariance, no auto covariance.

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K1, in other words, the conveyors
would like one and two sigmas squared.

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And then the covariance with
itself is five sigma squared.

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And then for negative one,
we just the symmetric.

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This is gamma negative K.

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And if I want to find out the correlation
fun, function, in other words, A,

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C, F,
all I have to do is basically divide.

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Gamma (k) to gamma (0), that's the
definition of auto correlation function.

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And the gamma (k) is basically,
I divided everything by 5 sigma squared.

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This becomes 0.

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This becomes 2 / 5, 1 and
this is auto correlation for -k.

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So this is our auto correlation function.

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So if I graph this we have autocorrelation
always at lag 0 which is self

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the XT has a correlation 1 with itself,
of course.

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And then we have some
autocorrelation in lag 1, then it.

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Right?
This is basically a famous picture for

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An ACF of an MA model.

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If you have MA1 model, then ACF has
to cut off starting from one on.

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Okay, now if I look at all
the correlation part of model 2, so

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I'm going to skip a few steps here.

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If we are concentrated on rho 1,

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the correlation with other
correlation with lag one.

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This is gamma 1 over gamma 0.

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This is all gamma 1, this is gamma 0.

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instead of 2s now we have halves.

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If we calculate this, it becomes 2 over 5.

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So if you write ACF of the model 2,
we get exactly the same ACF of model 1.

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So if we have now two different models
Model 1, Model 2, they only differ with

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this coefficient 2 and a half, but both of
them has an ACF which is exactly the same.

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Now, if you are trying to
model a time series, and

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if you believe that ACF
[INAUDIBLE] at some point,

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then you try to model it with MAQ models,
right, MA 1, MA 2.

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But, if ACF, a few more and

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make queue process would have the same
ACF that would be problematic to model.

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So we would like to somehow eliminate
one of these models in some way.

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So ACFs are same, there's exactly
the same ACF, Model 1 and Model 2.

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Okay.

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So let's pause that thought a little bit.

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So we're going to come back and
eliminate one of those models.

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But how you're going to eliminate.

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So let's talk about this invertibility,
inverting.

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So what are we going to do,
we going to take general MA1 process now

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that we have Xt which is equal
to Zt plus some beta and

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our models beta was either half or
two, okay.

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What we're going to do.

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We're going to find Zt from here, so
Zt is going to basically Xt- beta Z- 1.

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All right, but then instead of Zt- 1,

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we will use the same relation,
this precursor relation.

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Instead of Zt- 1, if we use this.

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Put t instead of t minus.

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Instead of t put t-1,
this is going to be Xt-1, beta Zt-2, and

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replace Zt-1 with that expression.

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And expand it.

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We get Xt minus beta Xt-1,
plus beta squared Zt-2.

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In other words,
Zt now is expressed as Xt and

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Xt-1, plus some In step 2.

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And then we can continue.

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Instead of zt2.

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We can put again, xt minus 2 minus beta.

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Xz t minus 3, and so forth.

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We can continue with this,
in theory, until infinity.

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Then we'll, sorry.

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So we can continue this until infinity.

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What do we obtain?

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We obtain Zt is equal to Xt- Bxt- 1
+ B squared xt- 2- B cubed xt- 3.

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And it goes on and on and on.

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Right?
So what does this mean?

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Now the rest if you find xt here, xt = zt

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+ linear combination, but this is series,
it's not a linear combination anymore.

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Infinite series, and xt is on every
exterior value in the past, right.

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So you can think of this AR processes
are the regressive process.

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But the order, well it doesn't matter, the
order is infinity, this is AR infinity.

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Process.

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So what did we do?

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Well, we kind of inverted MA(1) process
into other with order infinity.

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Here's the one thing you have to
keep in mind, this is a series here,

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there's an infinite series here.

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And whenever we see an infinite series,

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we have to Keep in mind that it might be
convergent or divergent,you have to make

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sure that is actually
convergent in some sense.

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Okay, now I'm going repeat the same
thing using Backward shift operator,

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let's utilize Backward shift operator.

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For Ma1 process, Xt can be written as
Beta(B)Zt, and where is my Beta(B)?

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Beta(B) is basically 1 + Beta B.

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That's our polynomial operator acting on
Zt, and that will give us Ma1 process.

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Now, I would like to somehow
write Zt in terms of Xt.

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So what am I going to do?

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I'm going to find inverse operator So

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if the Beta B is our polynomial operator,
somehow if I can find inverse operator,

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and put in the inverse operator
into the left-hand side,

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then Zt is expressed some
inverse operator, acting on Xt.

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In other words,
Zt will be expressed in terms of Xts.

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Okay.

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So what is a Beta B inverse?

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Well, Beta B is 1 plus Beta B.

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And we can write this as
1 over 1 plus Beta B.

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This is not fraction.

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This is basically inverse
operator of 1 plus Beta B.

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And what we're going to
do is the following.

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We're going to act like this Beta B Is
a complex number for a minute.

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Assume that it's not actually an operator.

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It's a complex number.

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Think of z, and then expand this.

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This is the usual geometric expansion.

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This is geometric series.

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1 minus r plus r squared minus, I'm sorry.

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1 R, R is negative beta B.

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So it's going to be 1 plus R
plus R square plus R cubed but

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then since I have 1 minus negative
beta B here sign will alternate.

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So this is our inverse operator and

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if we act this operator this
Z inverse operator on our X,

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T then we will obtain well one Well,
this is not really one.

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This is Xt, so this is a typo here.

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This operator is acting on Xt,
1 acting on Xt.

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The Xt, and then this is going to
give us Xt minus 1 and so forth.

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In either way we invert that
Ma1 process into ar infinity.

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And we express Zt as infinite sum of Xts
with some weight in front of them, right?

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So how do we make sure that this
series is actually convergent series?

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Well it turns out That that series
is convergent in some sense,

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this is random variables,

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adding them up, so we have to talk
about convergence of random variables.

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This is not usual sequence, series.

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It is random variables involved here.

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There's this notion called mean-square
convergence Which is an option that

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medial will be there about
this mean square root is.

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But we actually proved this resolved.

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But for now let's use this as a black box.

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This series is convergent.

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It means squared tens.

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If and only if absolute value of beta,

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absolute value of beta is less than Okay
let's get a definition of invertibility.

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In general,
it make t as a stochastic process.

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It doesn't have to be [INAUDIBLE].

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Xt is a stochastic process and
think of Z is a notation right?

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It's random disperse of
white noise [INAUDIBLE].

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They say Xt is invertible.

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If Zt can be expressed as infinite series.

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Pie K, Xt minus k.

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K goes from zero to infinity.

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This is like AR infinity process,

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where This pk is the sum of the absolute
value of pk's is convergent.

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Now there was a series just of
pk's are absolutely convergent.

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This is the definition of
invertibility of a stochastic process.

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Now in our model one,
let's go back to our model one, model two.

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Remember those are the two models we have.

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It's tame ACF who wants
to eliminate one of them.

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If you look at model one our pi
k going to be since beta is 2,

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it's going to be sum of 2 the k.

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And this series really diverges here.

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But if you look at Model 2,
the [INAUDIBLE] case is 1 over 2.

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If you look at some of the 1 over
2 to the k, we talked about this,

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this is a geometric series, and
it is a convergence series.

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So what are we going to do?

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We're going to eliminate Model 1 and
go with Model 2.

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Somehow we will assume
that we would like to

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have our model to have
something worth splitting.

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Okay, so model choice.

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For invertibility to hold,

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we choose Model 2 since the absolute
value 1 over 2 is less than 1.

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In this way,

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our ACF uniquely determines the MA
process that we've been looking for.

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So what have you learn?

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You have learned that definition of
invertibility of a stochastic process.

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And then we learned the invertibility
condition Guarantees that

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unique MA process corresponding to
the observed Author Correlation Function,

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in other words, ACF.