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UNIVERSITÄT POTSDAM - Prof. Dr. Paul JJ Welfens

UNIVERSITÄT POTSDAM - Prof. Dr. Paul JJ Welfens

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duction factors and the indicator variables for technical progress, as well as for the role<br />

of information and communication were considered, first of all the first step of Engle<br />

and Granger’s two-step procedure was applied, in which existing long-term relations<br />

were identified and estimated without specifying the short-term dynamics. However,<br />

the distribution of the estimators of the cointegrating vector provided by such a static<br />

regression is generally non-normal, and so inference cannot be drawn about the significance<br />

of the individual parameters by using the standard ‘t’ tests. For this reason the<br />

three-step procedure, proposed by Engle and Yoo (cf. ENGLE / YOO, 1991) was subsequently<br />

used to remedy this shortcoming. Their third step, added to the Engle-<br />

Granger two-step procedure, provided a correction to the parameter estimates of the<br />

first stage static regression which made them asymptotically equivalent to FIML and<br />

provided a set of standard errors which allows the valid calculation of standard ‘t’ tests.<br />

The superior long-term production function was then used to at least roughly assess the<br />

effects of the technical progress approximated by the indicator variables and of the<br />

need for information and communication, approximated by the number of telephone<br />

calls, as well as the impact of the usual production factors on economic growth from<br />

1961 until 1990.<br />

Tab 8: Estimation Results for the Augmented Production Function<br />

Variable First step of Engle/Granger Third step of Engle/Yoo<br />

unrestricted α + β =1<br />

unrestricted α + β =1<br />

Constant -3.1574 -2.7882 -3.4344 -3.1174<br />

(-4.8813) a) (-5.5155) (-12.8774) (-8.4231)<br />

k t<br />

0.4073 0.3634 0.4372 0.3448<br />

(4.9118) (5.3738) (11.2103) (5.9142)<br />

l t<br />

0.7460 0.6366 0.7893 0.6552<br />

(5.4446) -- (15.9455) --<br />

pat t−2<br />

0.1611 0.1833 0.1738 0.2315<br />

(1.6913) (1.9955) (6.2744) (3.4501)<br />

lex t<br />

0.0494 0.0631 0.0498 0.0833<br />

(1.5696) (2.2805) (4.4865) (3.5447)<br />

tc t<br />

0.1580 0.1803 0.1390 0.1795<br />

(2.7992) (3.5497) (5.7917) (4.2943)<br />

D80 -0.0168 -0.0165 -0.0169 -0.0161<br />

(-2.1905) (-2.1551) (-7.6818) (-2.9815)<br />

D81 -0.0202 -0.0223 -0.0202 -0.0239<br />

(-2.6738) (-3.0828) (-8.7826) (-4.3455)<br />

R 2 0.9977 0.9974 0.9976 0.9973<br />

37

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