Table A10.
Open in new tab

Same as Table A6 but for CQ Cir.

HJD-2 450 000.M1Mirror2-GaussianCorrelation
9115.506−34.8−35.4−36.40.0
9212.831−26.8−30.1−29.23.1
9240.847−44.5−40.1−43.8−5.6
9255.788−32.2−33.5−33.00.7
9271.693−35.5−34.7−36.2−0.2
HJD-2 450 000.M1Mirror2-GaussianCorrelation
9115.506−34.8−35.4−36.40.0
9212.831−26.8−30.1−29.23.1
9240.847−44.5−40.1−43.8−5.6
9255.788−32.2−33.5−33.00.7
9271.693−35.5−34.7−36.2−0.2

Note. The line was integrated from −300 to 300 km s−1 for the moment method. Wings with normalized fluxes between 1.15 and 1.4 were used for the mirror method. The double Gaussians had center velocities ±a = ±200 km s−1.

Table A10.
Open in new tab

Same as Table A6 but for CQ Cir.

HJD-2 450 000.M1Mirror2-GaussianCorrelation
9115.506−34.8−35.4−36.40.0
9212.831−26.8−30.1−29.23.1
9240.847−44.5−40.1−43.8−5.6
9255.788−32.2−33.5−33.00.7
9271.693−35.5−34.7−36.2−0.2
HJD-2 450 000.M1Mirror2-GaussianCorrelation
9115.506−34.8−35.4−36.40.0
9212.831−26.8−30.1−29.23.1
9240.847−44.5−40.1−43.8−5.6
9255.788−32.2−33.5−33.00.7
9271.693−35.5−34.7−36.2−0.2

Note. The line was integrated from −300 to 300 km s−1 for the moment method. Wings with normalized fluxes between 1.15 and 1.4 were used for the mirror method. The double Gaussians had center velocities ±a = ±200 km s−1.

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