Theory and Modern Applications
Table 4 The results of the FFFFF-FI-ADF (FFFFF-FI-ADF)
FFFFF-FI-ADF | Brazil | Chile | France | Germany | Italy |
|---|---|---|---|---|---|
AG | d = 0.402 | d = 0.633 | d = 0.256 | d = 0.405 | d = 0.539 |
−6.688 (0.000) | −5.343 (0.000) | −5.617 (0.000) | −3.313 (0.007) | −2.257 (0.054) | |
New method. | d = 0.401 | d = 0.006 | d = 0.170 | d = 0.013 | d = 0.378 |
−6.695 (0.000) | −3.709 (0.000) | −4.520 (0.000) | −3.382 (0.007) | −2.453 (0.034) | |
GPH | d = 0.393 | d = 0.621 | d = 0.321 | d = 0.522 | d>1.000 |
−6.713 (0.000) | −5.350 (0.000) | −5.671 (0.000) | −3.252 (0.003) |  | |
RE | d = 0.185 | d = 0.325 | d = 0.296 | d = 0.583 | d = 0.766 |
−7.225 (0.000) | −5.404 (0.000) | −5.652 (0.000) | −3.213 (0.003) | −1.986 (0.045) | |
Frac. Fre. | 0.4 | 0.1 | 1.1 | 1.1 | 1.0 |
FFFFF-FI-ADF | Russia | Spain | Turkey | UK | US |
|---|---|---|---|---|---|
AG | d = 0.183 | d = 0.654 | d = 0.904 | d = 0.147 | d>1.000 |
−1.299 (0.679) | −1.903 (0.065) | −3.122 (0.001) | −4.614 (0.003) |  | |
New method. | d>0.7 | d = 0.556 | d = 0.151 | d = 0.139 | d = 0.133 |
|  | −1.955 (0.083) | −2.893 (0.065) | −5.339 (0.000) | −3.208 (0.057) | |
GPH | d = 0.289 | d = 0.684 | d = 0.922 | d>1.000 | d>1.000 |
−0.972 (0.687) | −1.888 (0.064) | −3.129 (0.002) |  |  | |
RE | d = 0.876 | d = 0.753 | d = 0.817 | d = 0.317 | d = 0.608 |
0.232 (0.690) | −1.856 (0.054) | −3.087 (0.003) | −5.549 (0.000) | −3.076 (0.006) | |
Frac. Fre. | 0.8 | 1.1 | 1.3 | 0.1 | 1.0 |