| HJD-2 450 000. . | M1 . | Mirror . | 2-Gaussian . | Correlation . |
|---|---|---|---|---|
| 8446.917 | 12.7 | 15.5 | 15.6 | 0.0 |
| 8462.819 | 16.7 | 19.2 | 19.1 | 4.8 |
| 8520.683 | 22.0 | 25.4 | 24.6 | 9.6 |
| 8546.628 | 13.6 | 16.5 | 16.7 | 0.2 |
| 8886.720 | 18.6 | 22.3 | 21.0 | 4.4 |
| 8898.659 | 25.2 | 30.8 | 30.4 | 12.8 |
| 8946.593 | 16.3 | 20.4 | 20.9 | 2.1 |
| 8948.628 | 13.7 | 18.4 | 18.3 | −0.7 |
| 9112.990 | 24.3 | 30.5 | 30.2 | 11.9 |
| 9165.816 | 14.0 | 16.6 | 17.4 | 1.1 |
| 9166.823 | 14.7 | 17.1 | 18.0 | 1.8 |
| 9195.801 | 20.8 | 23.9 | 23.7 | 9.1 |
| 9217.791 | 25.5 | 30.7 | 29.9 | 13.5 |
| 9238.713 | 24.7 | 28.6 | 27.6 | 12.3 |
| 9248.649 | 18.5 | 21.0 | 20.7 | 5.6 |
| 9252.681 | 18.9 | 21.6 | 21.1 | 5.1 |
| 9301.606 | 23.1 | 25.5 | 26.1 | 10.8 |
| 9312.574 | 26.8 | 31.0 | 31.1 | 14.5 |
| 9494.993 | 19.0 | 20.8 | 21.6 | 6.7 |
| HJD-2 450 000. . | M1 . | Mirror . | 2-Gaussian . | Correlation . |
|---|---|---|---|---|
| 8446.917 | 12.7 | 15.5 | 15.6 | 0.0 |
| 8462.819 | 16.7 | 19.2 | 19.1 | 4.8 |
| 8520.683 | 22.0 | 25.4 | 24.6 | 9.6 |
| 8546.628 | 13.6 | 16.5 | 16.7 | 0.2 |
| 8886.720 | 18.6 | 22.3 | 21.0 | 4.4 |
| 8898.659 | 25.2 | 30.8 | 30.4 | 12.8 |
| 8946.593 | 16.3 | 20.4 | 20.9 | 2.1 |
| 8948.628 | 13.7 | 18.4 | 18.3 | −0.7 |
| 9112.990 | 24.3 | 30.5 | 30.2 | 11.9 |
| 9165.816 | 14.0 | 16.6 | 17.4 | 1.1 |
| 9166.823 | 14.7 | 17.1 | 18.0 | 1.8 |
| 9195.801 | 20.8 | 23.9 | 23.7 | 9.1 |
| 9217.791 | 25.5 | 30.7 | 29.9 | 13.5 |
| 9238.713 | 24.7 | 28.6 | 27.6 | 12.3 |
| 9248.649 | 18.5 | 21.0 | 20.7 | 5.6 |
| 9252.681 | 18.9 | 21.6 | 21.1 | 5.1 |
| 9301.606 | 23.1 | 25.5 | 26.1 | 10.8 |
| 9312.574 | 26.8 | 31.0 | 31.1 | 14.5 |
| 9494.993 | 19.0 | 20.8 | 21.6 | 6.7 |
Note. The line was integrated from -−500 to 500 km s−1 for the moment method. Wings with normalized fluxes between 1.4 and 2.2 were used for the mirror method. The double Gaussians had center velocities ±a = ±220 km s−1.
| HJD-2 450 000. . | M1 . | Mirror . | 2-Gaussian . | Correlation . |
|---|---|---|---|---|
| 8446.917 | 12.7 | 15.5 | 15.6 | 0.0 |
| 8462.819 | 16.7 | 19.2 | 19.1 | 4.8 |
| 8520.683 | 22.0 | 25.4 | 24.6 | 9.6 |
| 8546.628 | 13.6 | 16.5 | 16.7 | 0.2 |
| 8886.720 | 18.6 | 22.3 | 21.0 | 4.4 |
| 8898.659 | 25.2 | 30.8 | 30.4 | 12.8 |
| 8946.593 | 16.3 | 20.4 | 20.9 | 2.1 |
| 8948.628 | 13.7 | 18.4 | 18.3 | −0.7 |
| 9112.990 | 24.3 | 30.5 | 30.2 | 11.9 |
| 9165.816 | 14.0 | 16.6 | 17.4 | 1.1 |
| 9166.823 | 14.7 | 17.1 | 18.0 | 1.8 |
| 9195.801 | 20.8 | 23.9 | 23.7 | 9.1 |
| 9217.791 | 25.5 | 30.7 | 29.9 | 13.5 |
| 9238.713 | 24.7 | 28.6 | 27.6 | 12.3 |
| 9248.649 | 18.5 | 21.0 | 20.7 | 5.6 |
| 9252.681 | 18.9 | 21.6 | 21.1 | 5.1 |
| 9301.606 | 23.1 | 25.5 | 26.1 | 10.8 |
| 9312.574 | 26.8 | 31.0 | 31.1 | 14.5 |
| 9494.993 | 19.0 | 20.8 | 21.6 | 6.7 |
| HJD-2 450 000. . | M1 . | Mirror . | 2-Gaussian . | Correlation . |
|---|---|---|---|---|
| 8446.917 | 12.7 | 15.5 | 15.6 | 0.0 |
| 8462.819 | 16.7 | 19.2 | 19.1 | 4.8 |
| 8520.683 | 22.0 | 25.4 | 24.6 | 9.6 |
| 8546.628 | 13.6 | 16.5 | 16.7 | 0.2 |
| 8886.720 | 18.6 | 22.3 | 21.0 | 4.4 |
| 8898.659 | 25.2 | 30.8 | 30.4 | 12.8 |
| 8946.593 | 16.3 | 20.4 | 20.9 | 2.1 |
| 8948.628 | 13.7 | 18.4 | 18.3 | −0.7 |
| 9112.990 | 24.3 | 30.5 | 30.2 | 11.9 |
| 9165.816 | 14.0 | 16.6 | 17.4 | 1.1 |
| 9166.823 | 14.7 | 17.1 | 18.0 | 1.8 |
| 9195.801 | 20.8 | 23.9 | 23.7 | 9.1 |
| 9217.791 | 25.5 | 30.7 | 29.9 | 13.5 |
| 9238.713 | 24.7 | 28.6 | 27.6 | 12.3 |
| 9248.649 | 18.5 | 21.0 | 20.7 | 5.6 |
| 9252.681 | 18.9 | 21.6 | 21.1 | 5.1 |
| 9301.606 | 23.1 | 25.5 | 26.1 | 10.8 |
| 9312.574 | 26.8 | 31.0 | 31.1 | 14.5 |
| 9494.993 | 19.0 | 20.8 | 21.6 | 6.7 |
Note. The line was integrated from -−500 to 500 km s−1 for the moment method. Wings with normalized fluxes between 1.4 and 2.2 were used for the mirror method. The double Gaussians had center velocities ±a = ±220 km s−1.
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