THE FIRST DETERMINATION OF THE VISCOSITY PARAMETER IN THE CIRCUMSTELLAR DISK OF A Be STAR

被引:77
作者
Carciofi, Alex C. [1 ]
Bjorkman, Jon E. [1 ,2 ]
Otero, Sebastian A. [3 ]
Okazaki, Atsuo T. [4 ]
Stefl, Stanislav [5 ]
Rivinius, Thomas [5 ]
Baade, Dietrich [6 ]
Haubois, Xavier [1 ]
机构
[1] Univ Sao Paulo, Inst Astron Geofis & Ciencias Atmosfer, BR-05508900 Sao Paulo, Brazil
[2] Univ Toledo, Dept Phys & Astron, Ritter Observ, Toledo, OH 43606 USA
[3] Amer Assoc Variable Star Observers, Cambridge, MA 02138 USA
[4] Hokkai Gakuen Univ, Fac Engn, Toyohira Ku, Sapporo, Hokkaido 0628605, Japan
[5] European Org Astron Res So Hemisphere, Santiago 19, Chile
[6] European Org Astron Res So Hemisphere, D-85748 Garching, Germany
基金
巴西圣保罗研究基金会;
关键词
circumstellar matter; stars: activity; stars:; emission-line; Be; stars: individual (28 CMa); NONRADIAL PULSATION; CYCLIC VARIABILITY; KEPLERIAN DISKS; OMEGA CMA; MASS-LOSS; STELLAR; EMISSION; ROTATION; LINE; RATES;
D O I
10.1088/2041-8205/744/1/L15
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Be stars possess gaseous circumstellar decretion disks, which are well described using standard alpha-disk theory. The Be star 28 CMa recently underwent a long outburst followed by a long period of quiescence, during which the disk dissipated. Here we present the first time-dependent models of the dissipation of a viscous decretion disk. By modeling the rate of decline of the V-band excess, we determine that the viscosity parameter alpha = 1.0 +/- 0.2, corresponding to a mass injection rate (M) over dot = (3.5 +/- 1.3) x 10(-8) M-circle dot yr(-1). Such a large value of a suggests that the origin of the turbulent viscosity is an instability in the disk whose growth is limited by shock dissipation. The mass injection rate is more than an order of magnitude larger than the wind mass-loss rate inferred from UV observations, implying that the mass injection mechanism most likely is not the stellar wind, but some other mechanism.
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页数:5
相关论文
共 32 条
[1]  
ANDO H, 1986, ASTRON ASTROPHYS, V163, P97
[2]  
Argelander F.W. A., 1843, URANOMETRIA NOVA
[3]  
BAADE D, 2011, IAU SYMP P SERIES, V272, P1, DOI DOI 10.1017/S1743921311009914
[4]  
Bjorkman JE, 2005, ASTR SOC P, V337, P75
[5]   Cyclic variability of the circumstellar disk of the Be star ζ Tauri II. Testing the 2D global disk oscillation model [J].
Carciofi, A. C. ;
Okazaki, A. T. ;
le Bouquin, J. -B. ;
Stefl, S. ;
Rivinius, Th. ;
Baade, D. ;
Bjorkman, J. E. ;
Hummel, C. A. .
ASTRONOMY & ASTROPHYSICS, 2009, 504 (03) :915-927
[6]   Non-LTE Monte Carlo radiative transfer. I. The thermal properties of Keplerian disks around classical Be stars [J].
Carciofi, AC ;
Bjorkman, JE .
ASTROPHYSICAL JOURNAL, 2006, 639 (02) :1081-1094
[7]   The circumstellar discs of Be stars [J].
Carciofi, Alex C. .
ACTIVE OB STARS: STRUCTURE, EVOLUTION, MASS-LOSS, AND CRITICAL LIMITS, 2011, (272) :325-336
[8]   A statistical study of threshold rotation rates for the formation of disks around Be stars [J].
Cranmer, SR .
ASTROPHYSICAL JOURNAL, 2005, 634 (01) :585-601
[9]   A PULSATIONAL MECHANISM FOR PRODUCING KEPLERIAN DISKS AROUND Be STARS [J].
Cranmer, Steven R. .
ASTROPHYSICAL JOURNAL, 2009, 701 (01) :396-413
[10]   Line-driven ablation and wind tilting by external irradiation [J].
Gayley, KG ;
Owocki, SP ;
Cranmer, SR .
ASTROPHYSICAL JOURNAL, 1999, 513 (01) :442-459