Theory and Modern Applications
ε ↓∖ N → | 32 | 64 | 128 | 256 | 512 | 1,024 |
---|---|---|---|---|---|---|
2−5 | 5.155E − 04 | 1.465E − 04 | 3.789E − 05 | 9.552E − 06 | 2.403E − 06 | 8.200E − 07 |
2−6 | 7.592E − 04 | 2.664E − 04 | 7.515E − 05 | 1.945E − 05 | 4.911E − 06 | 1.202E − 06 |
2−7 | 8.368E − 04 | 3.857E − 04 | 1.353E − 04 | 3.818E − 05 | 9.876E − 06 | 2.470E − 06 |
2−8 | 8.409E − 04 | 4.251E − 04 | 1.944E − 04 | 6.821E − 05 | 1.924E − 05 | 4.963E − 06 |
2−9 | 8.409E − 04 | 4.272E − 04 | 2.143E − 04 | 9.756E − 05 | 3.425E − 05 | 9.658E − 06 |
2−10 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.075E − 04 | 4.892E − 05 | 1.717E − 05 |
2−11 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.387E − 05 | 2.450E − 05 |
2−12 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.694E − 05 |
2−13 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−14 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−15 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−16 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−17 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−18 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−19 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
2−20 | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
\(E^{N}\) | 8.409E − 04 | 4.272E − 04 | 2.153E − 04 | 1.081E − 04 | 5.414E − 05 | 2.707E − 05 |
\(R^{N}\) | 9.769E − 01 | 9.885E − 01 | 9.947E − 01 | 9.969E − 01 | 9.998E − 01 | 8.436E − 01 |