Table 1.
δ−1/γ | n |
|
EP | n |
|
EP | n |
|
EP | ||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| |||||||||||||
Design | κ = 0.5 | κ = 1 | κ = 2 | ||||||||||
Scenario 1: η ≠ 0 γ ≠ 0 | |||||||||||||
| |||||||||||||
π0 = 0.1 | 1.2/0.4 | 3445 | .050 | .903 | 1385 | .050 | .902 | 1075 | .047 | .897 | |||
λ0 = 0.1 | 1.3/0.5 | 1818 | .047 | .902 | 734 | .051 | .901 | 599 | .052 | .902 | |||
ta = 1 | 1.4/0.6 | 1165 | .052 | .904 | 469 | .053 | .898 | 389 | .052 | .901 | |||
tf = 10 | 1.5/0.7 | 833 | .048 | .902 | 333 | .052 | .897 | 276 | .049 | .905 | |||
1.6/0.8 | 638 | .053 | .899 | 253 | .051 | .905 | 208 | .048 | .897 | ||||
1.7/0.9 | 512 | .053 | .900 | 202 | .051 | .906 | 164 | .050 | .900 | ||||
1.8/1.0 | 426 | .049 | .909 | 166 | .052 | .900 | 133 | .053 | .903 | ||||
| |||||||||||||
Scenario 2: η ≠ 0 γ = 0 | |||||||||||||
| |||||||||||||
π0 = 0.1 | 1.4/0 | 1783 | .049 | .900 | 801 | .048 | .900 | 1335 | .048 | .902 | |||
π1 = 0.1 | 1.5/0 | 1266 | .044 | .904 | 562 | .052 | .902 | 927 | .052 | .900 | |||
λ0 = 0.1 | 1.6/0 | 970 | .049 | .903 | 425 | .048 | .903 | 696 | .049 | .900 | |||
ta = 1 | 1.7/0 | 783 | .048 | .907 | 340 | .049 | .904 | 551 | .051 | .902 | |||
tf = 10 | 1.8/0 | 655 | .053 | .904 | 281 | .052 | .897 | 454 | .050 | .901 | |||
1.9/0 | 563 | .052 | .911 | 240 | .053 | .904 | 385 | .054 | .896 | ||||
2.0/0 | 495 | .051 | .904 | 209 | .050 | .908 | 333 | .052 | .905 | ||||
| |||||||||||||
Scenario 3: η = 0 γ ≠ 0 | |||||||||||||
| |||||||||||||
π0 = 0.1 | 1/1.0 | 5627 | .049 | .900 | 1489 | .050 | .899 | 427 | .052 | .905 | |||
λ0 = 0.1 | 1/1.1 | 4306 | .049 | .904 | 1148 | .050 | .904 | 338 | .047 | .902 | |||
λ1 = 0.1 | 1/1.2 | 3356 | .047 | .897 | 902 | .052 | .900 | 272 | .052 | .901 | |||
ta = 1 | 1/1.3 | 2657 | .052 | .903 | 720 | .049 | .897 | 222 | .050 | .899 | |||
tf = 10 | 1/1.4 | 2133 | .050 | .900 | 583 | .047 | .903 | 184 | .051 | .908 | |||
1/1.5 | 1734 | .053 | .895 | 478 | .050 | .902 | 154 | .049 | .902 | ||||
1/1.6 | 1425 | .046 | .908 | 396 | .050 | .898 | 131 | .051 | .911 |