Open Access
Table 3.
Time-delay measurements for seven wavelength bins containing a combination of MgII and FeII emission, after subtracting the power-law component.
| HE 0435-4312 | |||||||
|---|---|---|---|---|---|---|---|
| Methods | Curve 1 | Curve 2 | Curve 3 | Curve 4 | Curve 5 | Curve 6 | Curve 7 |
| Javelin (peak) | 492.0 |
500.0 |
505.0 |
495.0 |
490.0 |
490.0 |
492.0 |
| Javelin (mean) | 706.7 |
705.7 |
600.9 |
649.7 |
747.6 |
863.1 |
755.9 |
| ICCF (rmax) | 620.0 (0.66) | 496.0 (0.65) | 585.0 (0.56) | 486.0 (0.45) | 620.0 (0.37) | 620.0 (0.48) | 620.0 (0.62) |
| ICCF (centroid) |
 |
 |
 |
 |
 |
 |
 |
| ICCF (peak) |
 |
 |
 |
 |
 |
 |
 |
| χ2 (min) | 656.29 | 519.26 | 513.26 | 511.26 | 515.26 | 519.28 | 656.33 |
| χ2 (bootstrap) |
 |
 |
 |
 |
 |
 |
 |
| zDCF |
 |
 |
 |
 |
 |
 |
 |
| von Neumann (min) | 501.0 | 476.0 | 560.0 | 560.0 | 560.0 | 560.0 | 501.0 |
| von Neumann (bootstrap) |
 |
 |
 |
 |
 |
 |
 |
| Bartels (min) | 538.0 | 560.0 | 574.0 | 487.0 | 610.0 | 560.0 | 560.0 |
| Bartels (bootstrap) |
 |
 |
 |
 |
 |
 |
 |
| HE 0413-4031 | |||||||
| Javelin (peak) | 940.5 |
953.9 |
970.4 |
932.7 |
939.7 |
945.6 |
953.7 |
| Javelin (mean) | 946.6 |
909.2 |
895.1 |
866.4 |
795.4 |
661 |
924.3 |
| ICCF (rmax) | 770.0 (0.61) | 768.0 (0.64) | 792.0 (0.72) | 831.0 (0.79) | 792.0 (0.85) | 635.0 (0.85) | 774.0 (0.72) |
| ICCF (centroid) |
 |
 |
 |
 |
 |
 |
 |
| ICCF (peak) |
 |
 |
 |
7 |
 |
 |
 |
| χ2 (min) | 718.36 | 763.38 | 730.37 | 718.36 | 718.36 | 633.32 | 764.38 |
| χ2 (bootstrap) |
 |
 |
 |
 |
 |
 |
 |
| zDCF |
 |
 |
 |
 |
 |
 |
 |
| von Neumann (min) | 734.0 | 734.0 | 721.0 | 721.0 | 721.0 | 634.0 | 734.0 |
| von Neumann (bootstrap) |
 |
 |
 |
 |
 |
 |
 |
| Bartels (min) | 812.0 | 734.0 | 826.0 | 812.0 | 719.0 | 615.0 | 734.0 |
| Bartels (bootstrap) |
 |
 |
 |
 |
 |
 |
 |
Notes. Curves 1 and 7 mostly contain FeII, and curves 4 and 5 are strongly dominated by MgII. For ICCF, we also show the maximum correlation coefficient in the parenthesis.
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