Cointegration, Stationarity and Error Correction Models



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Cointegration, Stationarity and Error Correction Models.
From the notes you need to know:
The definition of weak or covariance stationarity on page 2 of the notes plus an intuitive understanding of the term.
Testing for unit roots, the Dickey Fuller test and the Augmented Dickey Fuller test
The concept of cointegration (pages 2 & 3).

Testing for cointegration (Page 5-6)


The Engle Granger representation theorem
Error Correction Models – including superconsistency of the long run equilibrium parameters (page 4-5)
The Engle Granger two step method
The Role of cointegration in economics

To supplement these we have:




Trend Stationarity
The following is an AR(1) (autoregressive with lag depth or order 1) with a deterministic linear trend term

Yt = θYt-1 + δ + γt + εt (1)


Where |θ| < 1
The moving average (MA) representation of this on past error terms is

Yt = θtY0 + μ0 + μ1t + εt + θεt-1 + θ2εt-2 + θ3εt-3 + ….. (2)


E(Yt) = θtY0 + μ0 + μ1t → μ0 + μ1t as t → ∞ (3)

This has a finite, unchanging variance, but no constant mean (because of μ1t). Thus the process is not stationary.



However, the deviation from the mean
Yt = Yt – E[Yt] = Yt - μ0 - μ1t (4)
is stationary and hence Yt is called a trend stationary process. Thus the shocks to the process are transitory and the process is ‘mean reverting’, with the mean μ0 + μ1t being the ‘attractor’.

UNIT ROOT PROCESSES

The following is an AR(1) model with a unit root θ=1


Yt = θYt-1 + δ + εt = Yt-1 + δ + εt (5)
It is clearly non-staionary with no specified mean. But the process ∆Yt is stationary and we term Yt a difference stationary process (in this case I(1))
Yt = Yt-1 + δ + εt (6)
Yt = Yt-2 + δ + εt + δ + εt-1 (substituting for Yt-1) (7)
Yt = Yt-3 + δ + εt + δ + εt-1 + δ + ε-2 (substituting for Yt-2)

Yt-3 + δ + δ + δ + εt + εt-1 + ε-2 (7)


And so on until:
Yt = Y0 + δt + Σεi (8)
Hence E[Yt] = Y0 + δt (9)
The effect of the initial value Y0 stays in the process. We can also see from (8) that shocks have permanent effects and the figure below shows the impact of a large shock. The process has no attractor.


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