RDP 9410: An Empirical Examination of the Fisher Effect in Australia Appendix A: Power Calculations
December 1994
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The power calculations found in Table A1 are obtained from Monte Carlo simulations using the same procedure that was described in Section 3.1.1, however, the data generating process is estimated from ARIMA models estimated in levels rather than first differences, that is, ARMA models. The power calculation for each test statistic in the table is the probability obtained from this Monte Carlo simulation of rejecting the null of a unit root given the alternative of no unit root using the size-corrected 5% critical value for the test statistic.
Sample period | Test statistics for πt | Test statistic for it | ||||
---|---|---|---|---|---|---|
DF | Zt | Zα | DF | Zt | Zα | |
1962 III–1993 IV | 0.093 | 0.094 | 0.090 | 0.053 | 0.032 | 0.029 |
1962 III–1979 III | 0.095 | 0.098 | 0.107 | 0.162 | 0.166 | 0.178 |
1979 IV–1993 IV | 0.057 | 0.059 | 0.044 | 0.112 | 0.119 | 0.142 |
Tables A2 and A3 contains the power calculations for test statistics from the Engle Granger two step method and the ECM equations reported in Table 3 using similar Monte Carlo simulations to those used in Table A1. The data generating process for the cointegration tests for a unit root in πt − it is an error correction model in which the error correction term is πt − it. Similarly, the data generating process used for the tests of a unit root in πt − it is an error correction model in which the error correction term is πt − it. The test statistics in Table A2 are the same as those reported in Table 2 and Table A1, that is, Dickey-Fuller t-tests and Phillips Zt and Zα tests.
Sample period | Test statistics for unit root in πt − it |
Test statistic for unit root in πt − it |
||||
---|---|---|---|---|---|---|
DF | Zt | Zα | DF | Zt | Zα | |
1962 III–1993 IV | 0.076 | 0.086 | 0.096 | 0.188 | 0.192 | 0.196 |
1962 III–1979 III | 0.449 | 0.503 | 0.606 | 0.461 | 0.507 | 0.573 |
1979 IV–1993 IV | 0.030 | 0.027 | 0.021 | 0.417 | 0.363 | 0.275 |
Sample period | Test statistics for unit root in πt − it |
Test statistic for unit root in πt − it |
||
---|---|---|---|---|
γ | δ | γ | δ | |
1962 III–1993 IV | 0.012 | 0.081 | 0.012 | 0.634 |
1962 III–1979 III | 0.034 | 0.358 | 0.072 | 0.750 |
1979 IV–1993 IV | 0.019 | 0.284 | 0.690 | 0.523 |
In most cases the power of tests in Table A1, A2 and A3 are very low. This stems from both the low power of the tests themselves and the low number of observations we have to work with.