The spin axes orbital alignment of both stars within the eclipsing binary system V1143 Cyg using the Rossiter-McLaughlin effect

被引:77
作者
Albrecht, S.
Reffert, S.
Snellen, I.
Quirrenbach, A.
Mitchell, D. S.
机构
[1] Leiden Univ, Leiden Observ, NL-2300 RA Leiden, Netherlands
[2] ZAH Landwssternwarte, D-69117 Heidelberg, Germany
[3] Calif Polytech State Univ San Luis Obispo, San Luis Obispo, CA 93407 USA
关键词
stars : individual : V1143 Cyg; binaries : eclipsing; techniques : spectroscopic; methods : data analysis binaries : spectroscopic;
D O I
10.1051/0004-6361:20077953
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Context. The Rossiter-McLaughlin (RM) effect, a rotational effect in eclipsing systems, provides unique insight into the relative orientation of stellar spin axes and orbital axes of eclipsing binary systems. Aims. Our aim is to develop a robust method to analyze the RM effect in an eclipsing system with two nearly equally bright components. This gives access to the orientation of the stellar rotation axes and may shed light on questions of binary formation and evolution. For example, a misalignment between the spin axes and the angular momentum of the system could bring the observed and theoretical apsidal motion into better agreement for some systems, including V1143 Cyg. Methods. High-resolution spectra have been obtained both out of eclipse and during the primary and secondary eclipses in the V1143 Cyg system, using the 0.6m Coude Auxiliary Telescope ( CAT) and the high-resolution Hamilton Echelle Spectrograph at the Lick Observatory. The Rossiter-McLaughlin effect is analyzed in two ways: ( 1) by measuring the shift of the line center of gravity during different phases of the eclipses and ( 2) by analysis of the line shape change of the rotational broadening function during eclipses. Results. We measured the projection of the stellar rotation axes using the rotation effect for both main-sequence stars in an eclipsing binary system. The projected axes of both stars are aligned with the orbital spin within the observational uncertainties, with the angle of the primary rotation axis beta(p) = 0.3 +/- 1.5 degrees, and the angle of the secondary rotation axis beta(s) = -1.2 +/- 1.6 degrees, thereby showing that the remaining difference between the theoretical and observed apsidal motion for this system is not due to a misalignment of the stellar rotation axes. Both methods utilized in this paper work very well, even at times when the broadening profiles of the two stars overlap.
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页码:565 / U118
页数:11
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