The extended molecular envelope of the asymptotic giant branch star π1 Gruis as seen by ALMA I. Large-scale kinematic structure and CO excitation properties

被引:24
作者
Doan, L. [1 ]
Ramstedt, S. [1 ]
Vlemmings, W. H. T. [2 ]
Hofner, S. [1 ]
De Beck, E. [2 ]
Kerschbaum, F. [3 ]
Lindqvist, M. [2 ]
Maercker, M. [2 ]
Mohamed, S. [4 ,5 ,6 ]
Paladini, C. [7 ]
Wittkowski, M. [8 ]
机构
[1] Uppsala Univ, Dept Phys & Astron, Box 516, S-75120 Uppsala, Sweden
[2] Chalmers Univ Technol, Dept Earth & Space Sci, S-43992 Onsala, Sweden
[3] Univ Vienna, Dept Astrophys, Turkenschanzstr 17, A-1180 Vienna, Austria
[4] South African Astron Observ, POB 9, ZA-7935 Observatory, South Africa
[5] Univ Cape Town, Dept Astron, ZA-7701 Rondebosch, South Africa
[6] Natl Inst Theoret Phys, Private Bag X1, ZA-7602 Matieland, South Africa
[7] Univ Libre Bruxelles, Inst Astron & Astrophys, Campus Plaine CP 226,Blvd Triomphe, B-1050 Brussels, Belgium
[8] European Southern Observ, Karl Schwarzschild Str 2, D-85748 Garching, Germany
基金
欧洲研究理事会; 新加坡国家研究基金会;
关键词
stars: AGB and post-AGB; stars: mass-loss; stars: individual: pi(1) Gru; stars: general; radio lines: stars; binaries: general; PROTOPLANETARY NEBULA CRL-618; PLANETARY-NEBULAE; AGB STARS; MASS-LOSS; S-STARS; MAGNETIC-FIELDS; BIPOLAR OUTFLOW; DRIVEN WINDS; V-HYDRAE; DISK;
D O I
10.1051/0004-6361/201730703
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Context. The S-type asymptotic giant branch (AGB) star pi(1) Gru has a known companion at a separation of 2 ''.7 (approximate to 400 AU). Previous observations of the circumstellar envelope (CSE) show strong deviations from spherical symmetry. The envelope structure, including an equatorial torus and a fast bipolar outflow, is rarely seen in the AGB phase and is particularly unexpected in such a wide binary system. Therefore a second, closer companion has been suggested, but the evidence is not conclusive. Aims. The aim is to make a 3D model of the CSE and to constrain the density and temperature distribution using new spatially resolved observations of the CO rotational lines. Methods. We have observed the J = 3-2 line emission from (CO)-C-12 and (CO)-C-13 using the compact arrays of the Atacama Large Millimeter/submillimeter Array (ALMA). The new ALMA data, together with previously published (CO)-C-12 J = 2-1 data from the Submillimeter Array (SMA), and the (CO)-C-12 J = 5-4 and J = 9-8 lines observed with Herschel/Heterodyne Instrument for the Far-Infrared (HIFI), is modeled with the 3D non-LTE radiative transfer code SHAPEMOL. Results. The data analysis clearly confirms the torus-bipolar structure. The 3D model of the CSE that satisfactorily reproduces the data consists of three kinematic components: a radially expanding torus with velocity slowly increasing from 8 to 13 km s(-1) along the equator plane; a radially expanding component at the center with a constant velocity of 14 km s(-1); and a fast, bipolar outflow with velocity proportionally increasing from 14 km s(-1) at the base up to 100 km s(-1) at the tip, following a linear radial dependence. The results are used to estimate an average mass-loss rate during the creation of the torus of 7.7 x 10(-7) M-circle dot yr(-1). The total mass and linear momentum of the fast outflow are estimated at 7.3 x 10(-4) M-circle dot and 9.6 x 10(37) g cm s(-1), respectively. The momentum of the outflow is in excess (by a factor of about 20) of what could be generated by radiation pressure alone, in agreement with recent findings for more evolved sources. The best-fit model also suggests a (CO)-C-12/(CO)-C-13 abundance ratio of 50. Possible shaping scenarios for the gas envelope are discussed.
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页数:14
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