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<strong>An</strong> <strong>Introduction</strong> <strong>to</strong><br />

<strong>Error</strong> <strong>Correction</strong> <strong>Models</strong><br />

Robin Best<br />

Oxford Spring School for Quantitative<br />

Methods in Social Research<br />

2008<br />

<strong>An</strong> <strong>Introduction</strong> <strong>to</strong> <strong>ECMs</strong><br />

The basic structure of an ECM<br />

ΔY t = α + βΔX t-1 - βEC t-1 + ε t<br />

Where EC is the error correction component of the model and measures the speed<br />

at which prior deviations from equilibrium are corrected.<br />

<strong>Error</strong> correction models can be used <strong>to</strong> estimate the following quantities of<br />

interest for all X variables.<br />

� Short term effects of X on Y<br />

� Long term effects of X on Y (long run multiplier)<br />

� The speed at which Y returns <strong>to</strong> equilibrium after a deviation has occurred.<br />

Applications of <strong>ECMs</strong> in the<br />

(Political Science) Literature<br />

• U.S. Presidential Approval/ U.K. Prime Ministerial Satisfaction<br />

• Policy Mood/Policy Sentiment<br />

• Support for Social Security<br />

• Consumer Confidence<br />

• Economic Expectations<br />

• Health Care Cost Containment/ Government Spending /Patronage Spending /<br />

Redistribution<br />

• Interest Rates/ Purchasing Power Parity<br />

• Growth in (U.S.) Presidential Staff<br />

• Arms Transfers<br />

• U.S. Judicial Influence<br />

<strong>An</strong> <strong>Introduction</strong> <strong>to</strong> <strong>ECMs</strong><br />

<strong>Error</strong> <strong>Correction</strong> <strong>Models</strong> (<strong>ECMs</strong>) are a category of multiple time series<br />

models that directly estimate the speed at which a dependent variable -<br />

Y - returns <strong>to</strong> equilibrium after a change in an independent variable - X.<br />

� <strong>ECMs</strong> are useful for estimating both short term and long term effects of<br />

one time series on another.<br />

• Thus, they often mesh well with our theories of political and social<br />

processes.<br />

• Theoretically-driven approach <strong>to</strong> estimating time series models.<br />

� <strong>ECMs</strong> are useful models when dealing with integrated data, but can<br />

also be used with stationary data.<br />

<strong>An</strong> <strong>Introduction</strong> <strong>to</strong> <strong>ECMs</strong><br />

� As we will see, the versatility of <strong>ECMs</strong> give them a number of desirable<br />

properties.<br />

• Estimates of short and long term effects<br />

• Easy interpretation of short and long term effects<br />

• Applications <strong>to</strong> both integrated and stationary time series data<br />

• Can be estimated with OLS<br />

• Model theoretical relationships<br />

� <strong>ECMs</strong> can be appropriate whenever (1) we have time series data and (2)<br />

are interested in both short and long term relationships between multiple<br />

time series.<br />

Overview of the Course<br />

I. Motivating <strong>ECMs</strong> with cointegrated data<br />

• Integration and cointegration<br />

• 2-step error correction estima<strong>to</strong>rs<br />

• Stata session #1<br />

II. Motivating <strong>ECMs</strong> with stationary data<br />

• The single equation ECM<br />

• Interpretation of long and short term effects<br />

• The Au<strong>to</strong>regressive Distributive Lag (ADL) model<br />

• Equivalence of the ECM and ADL<br />

• Stata session #2<br />

1


<strong>ECMs</strong> and Cointegration:<br />

Stationary vs. Integrated Time Series<br />

� Stationary time series data are mean reverting. That is, they have a<br />

finite mean and variance that do not depend on time.<br />

Y t = α + ρY t-1 + ε t<br />

Where | p | < 1 and ε t is also stationary with a mean of zero and variance σ 2<br />

� Note that when 0 < | p | < 1 the time series is stationary but contains<br />

au<strong>to</strong>correlation.<br />

<strong>ECMs</strong> and Cointegration:<br />

Integrated Time Series<br />

� Formally, an integrated series can be expressed as a function of all<br />

past disturbances at any point in time.<br />

t<br />

t∑<br />

ei<br />

i=<br />

1<br />

Or Y t = α + ρY t-1 + ε t<br />

Where p = 1<br />

Or Y t - Y t-1 = u t<br />

Where u t = ε t<br />

<strong>An</strong>d ε t is still a stationary process<br />

<strong>ECMs</strong> and Cointegration:<br />

Integrated Time Series<br />

(Theoretical) Sources of integration<br />

Y<br />

� The effect of past shocks is permanently incorporated in<strong>to</strong> the<br />

memory of the series.<br />

� The series is a function of other integrated processes.<br />

<strong>ECMs</strong> and Cointegration:<br />

Stationary vs. Integrated Time Series<br />

Often our time series data are not stationary, but appear <strong>to</strong> be integrated.<br />

Integrated time series data<br />

• Are not mean-reverting<br />

• appear <strong>to</strong> be on a ‘random walk’<br />

• Have current values that can be expressed as the sum of all previous changes<br />

• The effect of any shock is permanently incorporated in<strong>to</strong> the series<br />

• Thus, the best predic<strong>to</strong>r of the series at time t is the value at time t-1<br />

• Have a (theoretically) infinite variance and no mean.<br />

<strong>ECMs</strong> and Cointegration:<br />

Integrated Time Series<br />

Order of Integration<br />

� Integrated time series data that are stationary after being difference<br />

d times are Integrated of order d: I(d)<br />

� For our purposes, we focus on time series data that are I(1).<br />

• Data that are stationary after being first-differenced.<br />

� I(1) processes are fairly common in time series data<br />

A Drunk’s Random Walk<br />

0 20 40 60<br />

time<br />

2


<strong>ECMs</strong> and Cointegration:<br />

Integrated Time Series<br />

• <strong>An</strong>alyzing integrated time series in level form dramatically increases the<br />

likelihood of making a Type-II error.<br />

� Problem of spurious associations.<br />

� High R 2<br />

� Small standard errors and inflated t-ratios<br />

• A common solution <strong>to</strong> these problems is <strong>to</strong> analyze the data in differenced form.<br />

� Look only at short term effects<br />

<strong>ECMs</strong> and Cointegration<br />

� Two time series are cointegrated if<br />

� Both are integrated of the same order.<br />

� There is a linear combination of the two time series that is I(0) - i.e. -<br />

stationary.<br />

� Two (or more) series are cointegrated if each has a long run component,<br />

but these components cancel out between the series.<br />

� Share s<strong>to</strong>chastic trends<br />

� Conintegrated data are never expected <strong>to</strong> drift <strong>to</strong>o far away from each<br />

other, maintaining an equilibrium relationship.<br />

A Dog’s Random Walk<br />

0 20 40 60<br />

time<br />

<strong>ECMs</strong> and Cointegration:<br />

Integrated Time Series<br />

• <strong>An</strong>alyzing time series data in differenced form solves the spurious<br />

regression problem, but may “throw the baby out with the bathwater.”<br />

• A model that includes only (lagged) differenced variables assumes the<br />

effects of the X variables on Y never last longer than one time period.<br />

• What if our time series share a long run relationship?<br />

• If the time series share an equilibrium relationship with an errorcorrection<br />

mechanism, then the s<strong>to</strong>chastic trends of the time series will<br />

be correlated with one another.<br />

• Cointegration<br />

<strong>ECMs</strong> and Cointegration<br />

� Lets go back <strong>to</strong> the drunk’s random walk and call the drunk X. The<br />

random walk can be expressed as<br />

X t - X t-1 = u t<br />

� Where u t represents the stationary, white-noise shocks.<br />

� <strong>An</strong>other rather trivial example of a random walk is the walk (or jaunt) of a<br />

dog, which can be expressed as<br />

Y t - Y t-1 = w t<br />

� Where w t represents the stationary, while-noise process of the dog’s<br />

steps.<br />

<strong>ECMs</strong> and Cointegration<br />

But what if the dog belongs <strong>to</strong> the drunk?<br />

� Then the two random walks are likely <strong>to</strong> have an equilibrium relationship and <strong>to</strong><br />

be cointegrated (Murray 1994).<br />

� Deviations from this equilibrium relationship will be corrected over time.<br />

� Thus, part of the s<strong>to</strong>chastic processes of both walks will be shared and will<br />

correct deviations the equilibrium<br />

X t - X t-1 = u t + c(Y t-1 - X t-1 )<br />

Y t - Y t-1 = w t + d(X t-1 - Y t-1 )<br />

Where the terms in parentheses are the error correcting mechanisms<br />

3


The Drunk and Her Dog<br />

0 20 40 60<br />

time<br />

drunk dog<br />

<strong>ECMs</strong> and Cointegration<br />

Y t = βX t + Z t<br />

Here, Z represents the portion of Y (in levels) that is not attributable <strong>to</strong> X.<br />

� In short, Z will capture the error correction relationship by capturing the<br />

degree <strong>to</strong> which Y and X are out of equilibrium.<br />

Z will capture any shock <strong>to</strong> either Y or X. If Y and X are cointegrated, then<br />

the relationship between the two will adjust accordingly.<br />

<strong>ECMs</strong> and Cointegration<br />

� We might theorize that shocks <strong>to</strong> X have two effects on ΔY.<br />

� Some portion of shocks <strong>to</strong> X might immediately affect Y in the next time<br />

period, so that ΔY t responds <strong>to</strong> ΔX t-1 .<br />

� A shock <strong>to</strong> X t will also disturb the equilibrium between Y and X, sending Y<br />

on a long term movement <strong>to</strong> a value that reproduces the equilibrium state<br />

given the new value of X.<br />

� Thus ΔY t is a function of both ΔX t-1 and the degree <strong>to</strong> which the two<br />

variables were out of equilibrium in the previous time period.<br />

<strong>ECMs</strong> and Cointegration<br />

Two I(1) time series (X t and Y t ) are cointegrated if there is some linear<br />

combination that is stationary.<br />

Z t = Y t - βX t<br />

Where Z is the portion of (levels of) Y that are not shared with X: the equilibrium<br />

errors.<br />

We can also rewrite this equation in regression form<br />

Y t = βX t + Z t<br />

Where the cointegrating vec<strong>to</strong>r - Z t - can be obtained by regressing Y t on X t .<br />

<strong>ECMs</strong> and Cointegration<br />

ΔY t will be a function of the degree <strong>to</strong> which the two time series were out of<br />

equilibrium in the previous period: Z t-1<br />

Z t-1 = Y t-1 - X t-1<br />

� When Z = 0 the system is in its equilibrium state<br />

� Y t will respond negatively <strong>to</strong> Z t-1 .<br />

� If Z is negative, then Y is <strong>to</strong>o high and will be adjusted downward in the next<br />

period.<br />

� If Z is positive, then Y is <strong>to</strong>o low and will be adjusted upward in the next time<br />

period.<br />

Engle and Granger Two-Step ECM<br />

� If two time series are integrated of the same order AND some linear<br />

combination of them is stationary, then the two series are cointegrated.<br />

� Cointegrated series share a s<strong>to</strong>chastic component and a long term<br />

equilibrium relationship.<br />

� Deviations from this equilibrium relationship as a result of shocks will be<br />

corrected over time.<br />

� We can think of ∆Y t as responding <strong>to</strong> shocks <strong>to</strong> X over the short and long<br />

term.<br />

4


Engle and Granger Two-Step ECM<br />

� Engle and Granger (1987) suggested an appropriate model for Y, based<br />

two or more time series that are cointegrated.<br />

� First, we can obtain an estimate of Z by regressing Y on X.<br />

� Second, we can regress ΔY t on Z t-1 plus any relevant short term<br />

effects.<br />

Engle and Granger Two-Step ECM<br />

� In Step 1, where we estimate the cointegrating regression we can -<br />

and should - include all variables we expect <strong>to</strong><br />

1) be cointegrated<br />

2) have sustained shocks on the equilibrium.<br />

� The variables that have sustained shocks on the equilibrium are<br />

usually regarded as exogenous shocks and often take the form of<br />

dummy variables.<br />

Engle and Granger Two-Step ECM<br />

The basic structure of the ECM<br />

ΔY t = α + βΔX t-1 - βEC t-1 + ε t<br />

In the Engle and Granger Two-Step Method the EC component is derived from<br />

cointegrated time series as Z.<br />

∆Y t = β 0 ∆X t-1 - β 1 Z t-1<br />

β 0 captures the short term effects of X in the prior period on Y in the current period.<br />

β 1 captures the rate at which the system Y adjusts <strong>to</strong> the equilibrium state after a<br />

shock. In other words, it captures the speed of error correction.<br />

Step 1:<br />

Engle and Granger Two-Step ECM<br />

Y t = α + βX t + Z t<br />

The cointegrating vec<strong>to</strong>r - Z - is measured by taking the residuals from the<br />

regression of Y t on X t<br />

Z t = Y t - βX t - α<br />

Step 2:<br />

Regress changes on Y on lagged changes in X as well as the equilibrium errors<br />

represented by Z.<br />

∆Y t = β 0 ∆X t-1 - β 1 Z t-1<br />

Note that all variables in this model are stationary.<br />

Engle and Granger Two-Step ECM<br />

The cointegrating regression is performed as Y t = α + βX t + Z t<br />

Which we can also conceptualize as<br />

Z t = Y t - (α +βX t )<br />

If we add a series of j exogenous shocks - represented as w j<br />

Then<br />

Y t = α + βX t + βW 1t + βW 2t +βW 3t + Z t<br />

Z t = Y t - (α +βX t + βW 1t + βW 2t +βW 3t )<br />

Engle and Granger Two-Step ECM<br />

Note that the Engle and Granger 2-Step method is really a 4-step method.<br />

1) Determine that all time series are integrated of the same order.<br />

2) Demonstrate that the time series are cointegrated<br />

3) Obtain an estimate of the cointegrating vec<strong>to</strong>r - Z - by regressing<br />

Y t on X t and taking the residuals.<br />

4) Enter the lagged residuals - Z - in<strong>to</strong> a regression of ∆Y t on ∆X t-1 .<br />

5


Engle and Granger Two-Step ECM<br />

� Viewed from this perspective, it is easy <strong>to</strong> see why error correction<br />

models have become so closely associated with cointegration (we will<br />

come back <strong>to</strong> this later).<br />

� Integrated time series present a problem for time series analysis - at<br />

least in terms of long term relationships.<br />

� When integrated time series variables are also cointegrated, error<br />

correction models provide a nice solution <strong>to</strong> this problem.<br />

Cointegration and <strong>Error</strong><br />

<strong>Correction</strong> in Political Science<br />

� Prime Ministerial Statisfaction (U.K.) and Conservative Party<br />

Support<br />

� Arms transfers by the U.S. and Soviet Union<br />

� Economic expectations and U.S. Presidential Approval<br />

� U.S. Domestic Policy Sentiment and Economic Expectations<br />

� Support for U.S. Social Security and the S<strong>to</strong>ck Market<br />

X and Y: Cointegrated?<br />

0 5 10 15 20 25<br />

1960m1 1961m1 1962m1 1963m1 1964m1 1965m1<br />

months<br />

Y X<br />

Cointegration and <strong>Error</strong> <strong>Correction</strong><br />

� One of the first instances of error correction was Davidson et. al.’s<br />

(1978) study of consumer expenditure and income in the U.K..<br />

� The Engle and Granger approach <strong>to</strong> error correction models follows<br />

nicely from the field of economics, where integration and cointegration<br />

among time series is theoretically common.<br />

� <strong>Error</strong> correction models were imported from economics.<br />

� Would we expect data from the social sciences <strong>to</strong> follow similar<br />

patterns of integration and cointegration?<br />

The Engle and Granger Two-Step<br />

ECM: Putting it in<strong>to</strong> Practice<br />

� Lets imagine we have two time series - perhaps the drunk and her dog -<br />

but lets call the drunk ‘X’ and the dog ‘Y’.<br />

� From a theoretical perspective, we believe changes in X will have both<br />

short and long term effects on Y, since we expect X and Y <strong>to</strong> have an<br />

equilibrium relationship.<br />

� We expect changes in X <strong>to</strong> produce long run responses in Y, as Y<br />

adjusts back <strong>to</strong> the equilibrium state.<br />

Engle and Granger Two-Step ECM<br />

First, we need <strong>to</strong> determine that both X and Y are integrated of the same order.<br />

• Which means we first need <strong>to</strong> demonstrate that both X and Y are, in fact,<br />

integrated processes.<br />

• We should also think about the likely stationary or nonstationary nature of our<br />

time series from a theoretical perspective.<br />

Tests for unit-root process tend <strong>to</strong> be controversial, primarily due <strong>to</strong> their low power.<br />

For our purposes, we will focus on Dickey-Fuller (DF) and Augmented Dickey-Fuller<br />

tests <strong>to</strong> examine the (non)stationarity of our time series.<br />

6


Dickey-Fuller Tests<br />

Basic Dickey-Fuller test<br />

With a constant (drift)<br />

With a time trend<br />

Δ t = xt−1<br />

x γ + ε<br />

x α γ + ε<br />

Δ t = t + xt−1<br />

x α γ + β + ε<br />

Δ t = t + xt−1<br />

Augmented Dickey-Fuller<br />

We can remove any remaining serial correlation in ε t by introducing an<br />

appropriate number of lagged differences of X in the equation.<br />

k<br />

Δ t = xt−1<br />

+ ∑<br />

i=<br />

1<br />

x γ β Δx<br />

+ ε<br />

k<br />

Δ t = t + γxt<br />

−1<br />

+ ∑<br />

i=<br />

1<br />

x α β Δx<br />

+ ε<br />

Where i = 1, 2, …k<br />

Null hypotheses are the same as the DF tests<br />

Is X Integrated?<br />

dfuller X, lags(4) regress<br />

i<br />

1t−i<br />

1t<br />

−i<br />

Augmented Dickey-Fuller test for unit root Number of obs = 59<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) 0.690 -3.567 -2.923 -2.596<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.9896<br />

------------------------------------------------------------------------------<br />

D.X | Coef. Std. Err. t P>|t| [95% Conf.Interval]<br />

-------------+----------------------------------------------------------------<br />

X |<br />

L1. | .0696672 .1008978 0.69 0.493 -.1327082 .2720426<br />

LD. | -.5724812 .1738494 -3.29 0.002 -.9211789 .2237835<br />

L2D. | -.4935811 .1776346 -2.78 0.008 -.8498709 -.1372912<br />

L3D. | -.2891465 .1677748 -1.72 0.091 -.6256601 .0473671<br />

L4D. | -.0898266 .1468121 -0.61 0.543 -.3842943 .2046412<br />

_cons | -.2525666 .839646 -0.30 0.765 -1.936683 1.43155<br />

------------------------------------------------------------------------------<br />

i<br />

t<br />

t<br />

t<br />

t<br />

t<br />

t<br />

Dickey-Fuller Tests<br />

Basic Dickey-Fuller test<br />

With a constant (drift)<br />

With a time trend<br />

Δ t = xt<br />

−1<br />

x γ + ε<br />

Δ t = t + γxt−1<br />

x α + ε<br />

x α γ + β + ε<br />

Δ t = t + xt−1<br />

If X is a random walk process, then γ = 0<br />

The null hypothesis is that X is a random walk<br />

MacKinnon values for statistical significance<br />

Note that in small samples the standard error of γ will be large, making it likely that<br />

we fail <strong>to</strong> reject the null when we really should<br />

dfuller X, regress<br />

Is X Integrated?<br />

Dickey-Fuller test for unit root Number of obs = 63<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) -1.852 -3.562 -2.920 -2.595<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.3548<br />

------------------------------------------------------------------------------<br />

D.X | Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+----------------------------------------------------------------<br />

X |<br />

L1. | -.1492285 .0805656 -1.85 0.069 -.3103293 .0118724<br />

_cons | 1.365817 .7149307 1.91 0.061 -.0637749 2.79541<br />

------------------------------------------------------------------------------------------------------------------------------------------------<br />

Is X Integrated?<br />

If X is I(1), then the first difference of X should be stationary.<br />

dfuller dif_X<br />

Dickey-Fuller test for unit root Number of obs = 62<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) -10.779 -3.563 -2.920 -2.595<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.0000<br />

t<br />

t<br />

t<br />

t<br />

7


Is Y Integrated?<br />

dfuller Y, regress<br />

Dickey-Fuller test for unit root Number of obs = 63<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) -1.323 -3.562 -2.920 -2.595<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.6184<br />

------------------------------------------------------------------------------<br />

D.Y | Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+----------------------------------------------------------------<br />

Y |<br />

L1. | -.0854922 .064599 -1.32 0.191 -.2146659 .0436814<br />

_cons | 1.061271 .7208156 1.47 0.146 -.3800884 2.502631<br />

------------------------------------------------------------------------------<br />

Cointegration<br />

� Both X and Y appear <strong>to</strong> be integrated of the same order: I(1).<br />

� If they are cointegrated, then they share s<strong>to</strong>chastic trends.<br />

� In the following regression, ε t should be stationary and β should be<br />

statistically significant and in the expected direction.<br />

Lets see if this is the case<br />

predict r, resid<br />

dfuller r<br />

Y t = α t + βX t +ε t<br />

Cointegrating Regression<br />

Dickey-Fuller test for unit root Number of obs = 63<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) -5.487 -3.562 -2.920 -2.595<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.0000<br />

Is Y Integrated?<br />

dfuller dif_Y, regress<br />

Dickey-Fuller test for unit root Number of obs = 62<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) -9.071 -3.563 -2.920 -2.595<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.0000<br />

------------------------------------------------------------------------------<br />

D.dif_Y | Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------dif_Y<br />

|<br />

L1. | -1.159903 .1278662 -9.07 0.000 -1.415674 -.9041329<br />

_cons | .2219184 .3259962 0.68 0.499 -.4301711 .8740078<br />

------------------------------------------------------------------------------<br />

regress Y X<br />

Cointegrating Regression<br />

Source | SS df MS Number of obs = 64<br />

-------------+------------------------------ F( 1, 62) = 92.49<br />

Model | 1009.22604 1 1009.22604 Prob > F = 0.0000<br />

Residual | 676.523964 62 10.9116768 R-squared = 0.5987<br />

-------------+------------------------------ Adj R-squared = 0.5922<br />

Total | 1685.75 63 26.7579365 Root MSE = 3.3033<br />

------------------------------------------------------------------------------<br />

Y | Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+----------------------------------------------------------------<br />

X | 1.206126 .1254135 9.62 0.000 .9554281 1.456824<br />

_cons | .0108108 1.135884 0.01 0.992 -2.259789 2.28141<br />

------------------------------------------------------------------------------<br />

-15 -10 -5 0 5 10<br />

Residuals<br />

1960m1 1961m1 1962m1 1963m1 1964m1 1965m1<br />

months<br />

8


Engle and Granger Two-Step ECM<br />

� Our residuals from the cointegrating regression capture deviations from<br />

the equilibrium of X and Y.<br />

� Therefore, we can estimate both the short and long term effects of X on<br />

Y by including the lagged residuals from the cointegrating regression as<br />

our measure of the error correction mechanism.<br />

ΔY t = α + β 1 *ΔX t-1 + β 2 *R t-1 +ε t<br />

Granger Causality and <strong>ECMs</strong><br />

Granger Causality:<br />

� A variable - X – Granger causes another variable – Y – if Y can be<br />

better predicted by the lagged values of both X and Y than by the lagged<br />

values of Y alone (see Freeman 1983).<br />

� Standard Granger causality tests can result in incorrect inferences about<br />

causality when there is an error correction process.<br />

� The Engle-Granger approach <strong>to</strong> <strong>ECMs</strong> begins by assuming all variables<br />

in the cointegrating regression are jointly endogeneous.<br />

� Thus, in the previous example we should also estimate a cointegrating<br />

regression of X on Y.<br />

Granger Causality<br />

regress dif_Y l.dif_Y l.dif_X lag_Y lag_X<br />

Source | SS df MS Number of obs = 62<br />

-------------+------------------------------ F( 4, 57) = 2.97<br />

Model | 69.5277246 4 17.3819311 Prob > F = 0.0270<br />

Residual | 334.149695 57 5.86227535 R-squared = 0.1722<br />

-------------+------------------------------ Adj R-squared = 0.1141<br />

Total | 403.677419 61 6.61766261 Root MSE = 2.4212<br />

-----------------------------------------------------------------------------dif_Y<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------dif_Y<br />

|<br />

L1. | .0483244 .1399056 0.35 0.731 -.2318318 .3284806<br />

dif_X |<br />

L1. | -.2205689 .1802099 -1.22 0.226 -.581433 .1402952<br />

lag_Y | -.3557259 .1161894 -3.06 0.003 -.5883911 -.1230606<br />

lag_X | .5675793 .1899981 2.99 0.004 .1871146 .948044<br />

_cons | -.928984 .9426534 -0.99 0.329 -2.816615 .9586468<br />

------------------------------------------------------------------------------<br />

Engle and Granger Two-Step ECM<br />

regress dif_Y dlag_X lag_r<br />

Source | SS df MS Number of obs = 62<br />

-------------+------------------------------ F( 2, 59) = 5.09<br />

Model | 59.4494524 2 29.7247262 Prob > F = 0.0091<br />

Residual | 344.227967 59 5.83437232 R-squared = 0.1473<br />

-------------+------------------------------ Adj R-squared = 0.1184<br />

Total | 403.677419 61 6.61766261 Root MSE = 2.4154<br />

-----------------------------------------------------------------------------dif_Y<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------dlag_X<br />

| -.1161038 .1609359 -0.72 0.473 -.4381358 .2059282<br />

lag_r | -.3160139 .0999927 -3.16 0.002 -.5160988 -.1159291<br />

_cons | .210471 .3074794 0.68 0.496 -.4047939 .8257358<br />

------------------------------------------------------------------------------<br />

The error correction mechanism is negative and significant, suggesting that<br />

deviations from equilibrium are corrected at about 32% per month.<br />

However, X does not appear <strong>to</strong> have significant short term effects on Y.<br />

Granger Causality<br />

• Granger causality can be ascertained in the ECM framework by<br />

regressing each time series in differenced form on all time series in<br />

both differenced and level form.<br />

• If an EC representation is appropriate, then in at least one of the<br />

regressions:<br />

� The lagged level of the predicted variable should be negative and<br />

significant.<br />

� The lagged level of the other variable should be in the expected<br />

direction and significant.<br />

Granger Causality<br />

regress dif_X l.dif_X l.dif_Y lag_X lag_Y<br />

Source | SS df MS Number of obs = 62<br />

-------------+------------------------------ F( 4, 57) = 5.87<br />

Model | 74.2042429 4 18.5510607 Prob > F = 0.0005<br />

Residual | 180.182854 57 3.1611027 R-squared = 0.2917<br />

-------------+------------------------------ Adj R-squared = 0.2420<br />

Total | 254.387097 61 4.17028027 Root MSE = 1.7779<br />

-----------------------------------------------------------------------------dif_X<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------dif_X<br />

|<br />

L1. | -.0640245 .132332 -0.48 0.630 -.3290147 .2009657<br />

dif_Y |<br />

L1. | .0014809 .1027357 0.01 0.989 -.2042438 .2072056<br />

lag_X | -.4676537 .1395197 -3.35 0.001 -.7470371 -.1882703<br />

lag_Y | .2847586 .0853204 3.34 0.001 .1139075 .4556097<br />

_cons | 1.194109 .6922106 1.73 0.090 -.1920183 2.580237<br />

------------------------------------------------------------------------------<br />

9


<strong>ECMs</strong>, Causality, and Theory<br />

� In the social sciences, our theories (usually) tell us which time series<br />

should be on the left side of the equation and which should be on the<br />

right.<br />

� The Engle and Granger approach assumes endogeneity between the<br />

cointegrating time series.<br />

Integration Issues<br />

<strong>Error</strong> correction approaches that rely on cointegration of two or more I(1)<br />

time series become problematic when we are dealing with data that are<br />

not truly (co)integrated.<br />

� I(1) processes may be incorrectly included in<strong>to</strong> the cointegrating<br />

regression - producing spurious associations - if two other I(1)<br />

cointegrated time series are already included (Durr 1992)<br />

� This problem increases with sample size.<br />

� The low power of unit root tests can lead us <strong>to</strong> conclude our data are<br />

integrated when they are not.<br />

More Integration Issues<br />

Under these conditions, we are likely <strong>to</strong> draw faulty inferences from the<br />

two-step procedure.<br />

We might conclude:<br />

� Our data are integrated when they are not.<br />

� Our data are cointegrated when they are not.<br />

� Our data are not cointegrated, therefore, an ECM is not appropriate<br />

Engle and Granger Two-Step<br />

Technique: Issues and Limitations<br />

� Does not clearly distinguish dependent variables from independent<br />

variables.<br />

� In the social sciences the Engle and Granger two-step ECM might not be<br />

consistent with our theories.<br />

� Is appropriate when dealing with cointegrated time series.<br />

� Can we clearly distinguish between integrated and stationary processes?<br />

More Integration Issues<br />

In the social sciences, we are more likely <strong>to</strong> have data that are<br />

� Near integrated (p = 0, but there is memory. p may not = 0 in finite<br />

samples.)<br />

� Fractionally integrated (0 < p < 1, where when 0 < p < .5 the data are<br />

mean-reverting and have finite variance, and when .5 ≤ p < 1 the data are<br />

mean-reverting but have infinite variance)<br />

� A combined process of both stationary and integrated data<br />

� Aggregated data<br />

Integration Issues and <strong>ECMs</strong><br />

� Under these conditions, we are often better off estimating a single<br />

equation ECM.<br />

� Single equation <strong>ECMs</strong> solve some of these problems and avoid others.<br />

� However, single equation <strong>ECMs</strong> require weak exogeneity.<br />

10


Single Equation<br />

<strong>Error</strong> <strong>Correction</strong> <strong>Models</strong><br />

� Following theory, Single Equation <strong>ECMs</strong> clearly distinguish between<br />

dependent and independent variables.<br />

� Single Equation <strong>ECMs</strong> are appropriate for both cointegrated and longmemoried,<br />

but stationary, data.<br />

� Cointegration may imply error correction, but does error correction imply<br />

cointegration?<br />

� Single Equation <strong>ECMs</strong> estimate a long term effect for each independent<br />

variable, allowing us <strong>to</strong> judge the contribution of each.<br />

� Allow for easier interpretation of the effects of the independent variables.<br />

Single Equation <strong>ECMs</strong><br />

� Single Equation <strong>Error</strong> <strong>Correction</strong> <strong>Models</strong> are useful<br />

� When our theories dictate the causal relationships of interest<br />

� When we have long-memoried/stationary data<br />

A basic single equation ECM:<br />

∆Y t = α + β 0 *∆X t - β 1 (Y t-1 - β 2 X t-1 ) + ε t<br />

The Single Equation ECM<br />

∆Y t = α + β 0*∆X t - β 1(Y t-1 - β 2X t-1) + βε t<br />

The portion of the equation in parentheses is the error correction mechanism.<br />

(Y t-1 - β 2 X t-1 ) = 0 when Y and X are in their equilibrium state<br />

β 0 estimates the short term effect of an increase in X on Y<br />

β 1 estimates the speed of return <strong>to</strong> equilibrium after a deviation.<br />

If the ECM approach is appropriate, then -1 < β 1 < 0<br />

β 2 estimates the long term effect that a one unit increase in X has on Y. This long<br />

term effect will be distributed over future time periods according <strong>to</strong> the rate of<br />

error correction - β 1<br />

Single Equation <strong>ECMs</strong><br />

� Our theories might specify long and short term effects of independent<br />

variables on a dependent variable even when our data are stationary.<br />

� The concepts of error correction, equilibrium , and long term effects are<br />

not unique <strong>to</strong> cointegrated data.<br />

� Furthermore, an ECM may provide a more useful modeling technique for<br />

stationary data than alternative approaches.<br />

� Our theories may be better represented by a single equation ECM.<br />

The Single Equation ECM<br />

Basic form of the ECM<br />

Engle and Granger two-step ECM<br />

The Single Equation ECM<br />

ΔY t = α + βΔX t-1 - βEC t-1 + ε t<br />

∆Y t = β 0 ∆X t-1 - β 1 Z t-1<br />

Where Z t = Y t - βX t - α<br />

∆Y t = α + β 0 *∆X t - β 1 (Y t-1 - β 2 X t-1 ) + ε t<br />

The Single Equation ECM<br />

∆Y t = α + β 0*∆X t - β 1(Y t-1 - β 2X t-1) + ε t<br />

The values for which Y and X are in their long term equilibrium relationship are<br />

Y = k0 + k1X α<br />

Where k0<br />

=<br />

β<br />

<strong>An</strong>d β 2<br />

k1<br />

=<br />

β<br />

1<br />

1<br />

Where k 1 is the <strong>to</strong>tal long term effect of X on Y (a.k.a the long run multiplier) - -<br />

distributed over future time periods.<br />

Single equation <strong>ECMs</strong> are particularly useful for allowing us <strong>to</strong> also estimate k 1 ’s<br />

standard error, and therefore statistical significance.<br />

11


The Single Equation ECM<br />

Since the long term effect is a ratio of two coefficients, we could calculate its<br />

standard error using the variance and covariance matrix<br />

Alternatively, we can use the Bewley transformation <strong>to</strong> estimate the standard error.<br />

This requires estimating the following regression.<br />

Y t = α+ δ 0 ∆Y t + δ 1 X t - δ 2 ∆X t + μ t<br />

Where δ 1 is the long term effect and is estimated with a standard error<br />

Notice the problem: we have ∆Y t on the right side of the equation<br />

We can proxy ∆Y t as:<br />

∆Y t = α + βY t-1 + βX t + β∆X t + ε t<br />

<strong>An</strong>d use our predicted values of ∆Y t in the Bewley transformation regression<br />

Single Equation <strong>ECMs</strong> in the<br />

(Political Science) Literature<br />

� Judicial Influence<br />

� Health Care Cost Containment<br />

� Interest Rates<br />

� Patronage Spending<br />

� Growth in Presidential Staff<br />

� Government Spending<br />

� Consumer Confidence<br />

� Redistribution<br />

<strong>ECMs</strong> and ADL <strong>Models</strong><br />

� We know Au<strong>to</strong>regressive Distributive Lag models are appropriate for<br />

stationary data (stationary data is, in fact, a requirement of these<br />

models).<br />

� Forms of single equation <strong>ECMs</strong> and ADL models are equivalent.<br />

� We can derive a single equation ECM from a general ADL model:<br />

Y t = α + β 0Y t-1 + β 1X t + β 2X t-1 + ε t<br />

The Single Equation ECM<br />

We can easily extend the single equation ECM <strong>to</strong> include more<br />

independent variables<br />

∆Y t = α + β∆X 1t + β∆X 2t + β∆X 3t - β(Y t-1 - βX 1t-1 - βX 2t-1 - βX 3t-1 ) + ε t<br />

Note that each independent variable is now forced <strong>to</strong> make an<br />

independent contribution <strong>to</strong> the long term relationship, solving one of<br />

the problems in the two-step estima<strong>to</strong>r.<br />

Single Equation <strong>ECMs</strong><br />

� Single Equation <strong>ECMs</strong><br />

� Provide the same information about the rate of error correction as the<br />

Engle and Granger two-step method.<br />

� Provide more information about the long term effect of each independent<br />

variable - including its standard error - than the Engle and Granger twostep<br />

method.<br />

� Illustrate that <strong>ECMs</strong> are appropriate for both cointegrated and stationary<br />

data.<br />

� How do we know Single Equation <strong>ECMs</strong> are appropriate with<br />

stationary data?<br />

<strong>ECMs</strong> and the ADL<br />

Y t = α + β 0 Y t-1 + β 1 X t + β 2 X t-1 + ε t<br />

∆Y t = α + (β 0 - 1)Y t-1 + β 1 X t + β 2 X t-1 + ε t<br />

∆Y t = α + (β 0 - 1)Y t-1 + β 1 ΔX t + (β 1 + β 2 )X t-1 + ε t<br />

Where φ 0 = β 0 - 1 and φ 1 = β 1 + β 2<br />

∆Y t = α + φ 0 Y t-1 + β 1 ΔX t + φ 1 X t-1 + ε t<br />

We can rewrite this equation in error correction form as<br />

∆Y t = α + β 1 ΔX t - φ 0 (Y t-1 - φ 1 X t-1 ) + ε t<br />

12


<strong>ECMs</strong> and the ADL<br />

We can see that the ADL model provides information similar <strong>to</strong> the ECM.<br />

Y t = α + β 0 Y t-1 + β 1 X t + β 2 X t-1 + ε t<br />

β 0 estimates the proportion of the deviation from equilibrium at t-1 that is maintained<br />

at time t. β 0 - 1 tells us the speed of return.<br />

β 1 estimates the short term effect of X on Y<br />

β 1 + β 2 estimates the long term effect of a unit change in X on Y (the coefficient on<br />

X t-1 in the ECM)<br />

<strong>ECMs</strong> and ADL <strong>Models</strong><br />

What does this mean?<br />

� <strong>ECMs</strong> are isophormic <strong>to</strong> ADL models<br />

� We can use them with stationary data<br />

� Certain forms of ADL models are - in a general sense - error correction<br />

models. They can be used <strong>to</strong> estimate:<br />

� The speed of return <strong>to</strong> equilibrium after a deviation has occurred.<br />

� Long term equilibrium relationships between variables.<br />

� Long and short term effects of independent variables on the dependent<br />

variable.<br />

Single Equation ECM<br />

� Lets imagine our theory about the relationship between X and Y states:<br />

� X causes Y.<br />

� X should have both a short term and a long term effect on Y.<br />

� We don’t have reason <strong>to</strong> suspect cointegration from a theoretical<br />

standpoint.<br />

� But we believe X and Y share a long term equilibrium relationship<br />

<strong>ECMs</strong> and the ADL<br />

Y t = α + β 0 Y t-1 + β 1 X t + β 2 X t-1 + ε t<br />

<strong>An</strong>d the <strong>to</strong>tal long term effect/long run multiplier - k 1 - is therefore:<br />

β 2 + β1<br />

k1<br />

=<br />

1 − β<br />

Y and X will be in their long term equilibrium state when Y = k 0 + k 1 X<br />

where<br />

0<br />

α<br />

k0<br />

=<br />

1− β<br />

The EC and ADL <strong>Models</strong>: Notation<br />

Lets use the following notation for the single equation ECM and the ADL<br />

ECM<br />

ADL<br />

∆Y t = α + β 0∆X t - β 1(Y t-1 - β 2X t-1) + ε t<br />

Y t = α + β 0Y t-1 + β 1X t + β 2X t-1 + ε t<br />

Single Equation ECM<br />

We determine that our Y variable is stationary (with 95% confidence), ruling out an<br />

ECM based on cointegration<br />

dfuller y, regress<br />

Dickey-Fuller test for unit root Number of obs = 55<br />

---------- Interpolated Dickey-Fuller ---------<br />

Test 1% Critical 5% Critical 10% Critical<br />

Statistic Value Value Value<br />

------------------------------------------------------------------------------<br />

Z(t) -3.353 -3.573 -2.926 -2.598<br />

------------------------------------------------------------------------------<br />

MacKinnon approximate p-value for Z(t) = 0.0127<br />

0<br />

13


Single Equation ECM<br />

We then estimate the single equation ECM<br />

As<br />

∆Y t = α + β 0∆X t - β 1(Y t-1 - β 2X t-1) + ε t<br />

∆Y t = α + β 0∆X t + β 1Y t-1 + β 2X t-1 + ε t<br />

If our error correction approach is correct, then β 1 should be -1 < β 1 < 0 and<br />

significant.<br />

Single Equation ECM<br />

The results indicate the following equation<br />

∆Y t = 13.12 + 1.32*∆X t -.42*Y t-1 + .52*X t-1 + ε t<br />

Which we can write in error correction form as<br />

∆Y t = 13.12 + 1.32*∆X t -.42(Y t-1 - 1.22*X t-1 ) + ε t<br />

Where 1.22 is our calculation of the long run multiplier<br />

Single Equation ECM<br />

∆Y t = α + 1.32*∆X t -.42(Y t-1 - 1.22*X t-1 ) + ε t<br />

Changes in X have both an immediate and long term effect on Y<br />

When the portion of the equation in parentheses = 0, X and Y are in their<br />

equilibrium state.<br />

Increases in X will cause deviations from this equilibrium, causing Y <strong>to</strong> be <strong>to</strong>o low.<br />

Y will then increase <strong>to</strong> correct this disequilibrium, with 42% of the (remaining)<br />

deviation corrected in each subsequent time period.<br />

Single Equation ECM<br />

regress dif_y dif_x lag_y lag_x<br />

Source | SS df MS Number of obs = 55<br />

-------------+------------------------------ F( 3, 51) = 21.40<br />

Model | 238.216589 3 79.4055296 Prob > F = 0.0000<br />

Residual | 189.278033 51 3.71133398 R-squared = 0.5572<br />

-------------+------------------------------ Adj R-squared = 0.5312<br />

Total | 427.494622 54 7.91656707 Root MSE = 1.9265<br />

-----------------------------------------------------------------------------dif_y<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------dif_x<br />

| 1.324821 .200003 6.62 0.000 .9232986 1.726344<br />

lag_y | -.4248235 .1146587 -3.71 0.001 -.6550105 -.1946365<br />

lag_x | .5182186 .1971867 2.63 0.011 .1223498 .9140873<br />

_cons | 13.12112 4.201755 3.12 0.003 4.685745 21.55649<br />

------------------------------------------------------------------------------<br />

Single Equation ECM<br />

∆Y t = 13.12 + 1.32*∆X t -.42(Y t-1 - 1.22*X t-1) + ε t<br />

Y and X are in their long term equilibrium state when<br />

Y = 30.89 + 1.22X<br />

So that when X = 1<br />

Y = 32.11<br />

Single Equation ECM<br />

∆Y t = α + 1.32*∆X t -.42(Y t-1 - 1.22*X t-1 ) + ε t<br />

A one unit increase in X immediately produces a 1.32 unit increase in Y.<br />

Increases in X also disrupt the the long term equilibrium relationship between these<br />

two variables, causing Y <strong>to</strong> be <strong>to</strong>o low.<br />

Y will respond by increasing a <strong>to</strong>tal of 1.22 points, spread over future time periods at<br />

a rate of 42% per time period.<br />

� Y will increase .52 points at t<br />

� Then another .3 points at t+1<br />

� Then another .2 points at t+2<br />

� Then another .1 points at t+3<br />

� Then another .05 points at t+4<br />

� Then another .03 points at t+5<br />

� Until the change in X at t-1 has virtually no effect on Y<br />

14


0 .5 1 1.5<br />

Change in Y<br />

0 2 4 6<br />

Time Period<br />

Single Equation ECM<br />

We can determine the standard error and confidence level of the <strong>to</strong>tal long term<br />

effect of X on Y through the Bewley transformation regression.<br />

First, we can obtain an estimate of ΔY by estimating ∆Y t = α + βY t-1 + βX t + β∆X t + ε t<br />

regress dif_y lag_y x dif_x<br />

Source | SS df MS Number of obs = 55<br />

-------------+------------------------------ F( 3, 51) = 21.40<br />

Model | 238.216589 3 79.4055296 Prob > F = 0.0000<br />

Residual | 189.278033 51 3.71133398 R-squared = 0.5572<br />

-------------+------------------------------ Adj R-squared = 0.5312<br />

Total | 427.494622 54 7.91656707 Root MSE = 1.9265<br />

-----------------------------------------------------------------------------dif_y<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------lag_y<br />

| -.4248235 .1146587 -3.71 0.001 -.6550105 -.1946365<br />

x | .5182186 .1971867 2.63 0.011 .1223498 .9140873<br />

dif_x | .8066027 .2278972 3.54 0.001 .34908 1.264125<br />

_cons | 13.12112 4.201755 3.12 0.003 4.685745 21.55649<br />

------------------------------------------------------------------------------<br />

Single Equation ECM<br />

� We can see our estimate of the long term effect of X on Y has a<br />

standard error of .12 and is statistically significant.<br />

� Can we gain similar estimates of the short and long term effects of X<br />

on Y from the ADL model?<br />

1 1.5 2 2.5<br />

Y<br />

0 2 4 6<br />

Time Period<br />

Single Equation ECM<br />

<strong>An</strong>d take the predicted values of ∆Y t <strong>to</strong> estimate Y t = α+ δ 0 ∆Y t + δ 1 X t - δ 2 ∆X t + μ t<br />

predict deltaYhat<br />

regress y deltaYhat x dif_x<br />

Source | SS df MS Number of obs = 55<br />

-------------+------------------------------ F( 3, 51) = 47.74<br />

Model | 531.551099 3 177.1837 Prob > F = 0.0000<br />

Residual | 189.278039 51 3.7113341 R-squared = 0.7374<br />

-------------+------------------------------ Adj R-squared = 0.7220<br />

Total | 720.829138 54 13.3486877 Root MSE = 1.9265<br />

-----------------------------------------------------------------------------y<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------deltaYhat<br />

| -1.353919 .2698973 -5.02 0.000 -1.89576 -.8120773<br />

x | 1.219844 .1245296 9.80 0.000 .9698408 1.469848<br />

dif_x | 1.898677 .3963791 4.79 0.000 1.102913 2.694442<br />

_cons | 30.88605 2.68463 11.50 0.000 25.49643 36.27567<br />

------------------------------------------------------------------------------<br />

Equivalence of the EC and ADL models<br />

First, lets estimate Y t = α + β 0 Y t-1 + β 1 X t + β 2 X t-1 + ε t<br />

regress y lag_y x lag_x<br />

Source | SS df MS Number of obs = 55<br />

-------------+------------------------------ F( 3, 51) = 47.74<br />

Model | 531.551105 3 177.183702 Prob > F = 0.0000<br />

Residual | 189.278033 51 3.71133398 R-squared = 0.7374<br />

-------------+------------------------------ Adj R-squared = 0.7220<br />

Total | 720.829138 54 13.3486877 Root MSE = 1.9265<br />

-----------------------------------------------------------------------------y<br />

| Coef. Std. Err. t P>|t| [95% Conf. Interval]<br />

-------------+---------------------------------------------------------------lag_y<br />

| .5751765 .1146587 5.02 0.000 .3449895 .8053635<br />

x | 1.324821 .200003 6.62 0.000 .9232986 1.726344<br />

lag_x | -.8066027 .2278972 -3.54 0.001 -1.264125 -.34908<br />

_cons | 13.12112 4.201755 3.12 0.003 4.685745 21.55649<br />

------------------------------------------------------------------------------<br />

15


Equivalence of the EC and ADL models<br />

The results imply the equation Y t = 13.12 + .58*Y t-1 + 1.32*X t -.81*X t-1 + ε t<br />

Our estimate of the contemporaneous effects of X on Y 1.32 units: the same as in<br />

the ECM.<br />

The long term effect of X on Y at t+1 can be calculated as:<br />

1.32 - .81 = .52 which is equivalent <strong>to</strong> the .52 estimate in the ECM<br />

Deviations from equilibrium are maintained at a rate of 58% per time period, which<br />

implies that deviations from equilibrium are corrected at a rate of 42% per time<br />

period (.58 - 1).<br />

<strong>Error</strong> <strong>Correction</strong> <strong>Models</strong><br />

� A Flexible Modeling approach<br />

� Stationary and Integrated Data<br />

� Long and Short Term Effects<br />

� Engle and Granger two-step ECM versus Single Equation ECM<br />

� Importance of Theory<br />

� Integrated or Stationary Data? Single Equation <strong>ECMs</strong> avoid this debate.<br />

� Single equation <strong>ECMs</strong> don’t require cointegration and ease interpretation of<br />

causal relationships.<br />

� Single equation <strong>ECMs</strong> and ADL models<br />

� Equivalence: ADL models can provide the same information about short<br />

and long term effects.<br />

� Standard error for the long term effects of independent variables is<br />

relatively easy <strong>to</strong> obtain in the single equation ECM<br />

Equivalence of the EC and ADL <strong>Models</strong><br />

Y t = 13.12 + .58*Y t-1 + 1.32*X t -.81*X t-1 + ε t<br />

The <strong>to</strong>tal long term effect/long run multiplier can be calculated as<br />

(1.32 - .81)/(.58 - 1) = 1.22 which is equivalent <strong>to</strong> the ECM estimate.<br />

Note, however, that we do not have a standard error for the long run<br />

multiplier.<br />

Y and X will be in their long term equilibrium state when<br />

Y = 30.89 + 1.22X<br />

16

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