The outer orbit of the high-mass stellar triple system Herschel 36 determined with the VLTI

被引:2
作者
Sanchez-Bermudez, J. [1 ,2 ]
Hummel, C. A. [3 ]
Diaz-Lopez, J. [1 ]
Alberdi, A. [4 ]
Schoedel, R. [4 ]
Arias, J., I [5 ]
Barba, R. H. [5 ]
Bastida-Escamilla, E. [6 ]
Brandner, W. [2 ]
Apellaniz, J. Maiz [4 ,7 ]
Pott, J-U [2 ]
机构
[1] Univ Nacl Autonoma Mexico, Inst Astron, Apdo Postal 70264, Ciudad De Mexico 04510, Mexico
[2] Max Planck Inst Astron, Konigstuhl 17, D-69117 Heidelberg, Germany
[3] European Southern Observ, Karl Schwarzschild Str 2, D-85748 Garching, Germany
[4] Inst Astrofis Andalucia IAA CSIC, Glorieta Astron S-N, E-18008 Granada, Spain
[5] Univ La Serena, Dept Fis & Astron, Av Cisternas 1200 Norte, La Serena, Chile
[6] Tecnol Monterrey, Escuela Ingn & Ciencias, Ave Eugenio Garza Sada 2501, Monterrey 64849, NL, Mexico
[7] CSIC INTA, Ctr Astrobiol, Campus ESAC Camino Bajo Castillo S-N, E-28692 Villanueva De La Canada, Spain
关键词
techniques: interferometric; (stars:) binaries: general; stars: massive; DATA REDUCTION; ACCRETION; AMBER/VLTI; COLLAPSE; CLUSTER; STARS;
D O I
10.1093/mnras/stac1238
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Multiplicity is a ubiquitous characteristic of massive stars. Multiple systems offer us a unique observational constraint on the formation of high-mass systems. Herschel 36 A is a massive triple system composed of a close binary (Ab1-Ab2) and an outer component (Aa). We measured the orbital motion of the outer component of Herschel 36 A using infrared interferometry with the AMBER and PIONIER instruments of ESO's Very Large Telescope Interferometer. Our immediate aims are to constrain the masses of all components of this system and to determine if the outer orbit is co-planar with the inner one. Reported spectroscopic data for all two components of this system and our interferometric data allow us to derive full orbital solutions for the outer orbit Aa-Ab and the inner orbit Ab1-Ab2. For the first time, we derive the absolute masses of m(Aa) = 22.3 +/- 1.7, m(Ab1) = 20.5 +/- 1.5, and m(Ab2) = 12.5 +/- 0.9 M-circle dot. Despite not being able to resolve the close binary components, we infer the inclination of their orbit by imposing the same parallax as the outer orbit. Inclinations derived from the inner and outer orbits imply a modest difference of about 22 degrees between the orbital planes. We discuss this result and the formation of Herschel 36 A in the context of Core Accretion and Competitive Accretion models, which make different predictions regarding the statistic of the relative orbital inclinations.
引用
收藏
页码:1162 / 1168
页数:7
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