Absolute parameters of young stars: HX Velorum

Author(s):  
M G Blackford ◽  
A Erdem ◽  
D Sürgit ◽  
B Özkardeş ◽  
E Budding ◽  
...  
2011 ◽  
Vol 418 (4) ◽  
pp. 2812-2812
Author(s):  
by E. Budding ◽  
G. İnlek ◽  
O. Demircan

Author(s):  
R J Butland ◽  
A Erdem ◽  
B Özkardeş ◽  
M G Blackford ◽  
D Sürgit ◽  
...  

2015 ◽  
Vol 448 (4) ◽  
pp. 3784-3796 ◽  
Author(s):  
E. Budding ◽  
R. Butland ◽  
M. Blackford

2009 ◽  
Vol 393 (2) ◽  
pp. 501-510 ◽  
Author(s):  
E. Budding ◽  
G. İnlek ◽  
O. Demircan

Author(s):  
E Budding ◽  
T Love ◽  
M G Blackford ◽  
T Banks ◽  
M J Rhodes

Abstract New spectrometric data on V Pup are combined with satellite photometry (HIPPARCOS and recent TESS) to allow a revision of the absolute parameters with increased precision. We find: M1 = 14.0±0.5, M2 = 7.3±0.3 (M⊙); R1 = 5.48±0.18, R2 = 4.59±0.15 (R⊙); T1 26000±1000, T2 24000 ±1000 (K), age 5 ±1 (Myr), photometric distance 320 ±10 (pc). The TESS photometry reveals low-amplitude (∼0.002 mag) variations of the β Cep kind, consistent with the deduced evolutionary condition and age of the optical primary. This fact provides independent support to our understanding of the system as in a process of Case A type interactive evolution that can be compared with μ1 Sco. The ∼10 M⊙ amount of matter shed by the over-luminous present secondary must have been mostly ejected from the system rather than transferred, thus taking angular momentum out of the orbit and keeping the pair in relative close proximity. New times of minima for V Pup have been studied and the results compared with previous analyses. The implied variation of period is consistent with the Case A evolutionary model, though we offer only a tentative sketch of the original arrangement of this massive system. We are not able to confirm the previously reported cyclical variations having a 5.47 yr period with the new data, though a direct comparison between the HIPPARCOS and TESS photometry points to the presence of third light from a star that is cooler than those of the close binary, as mentioned in previous literature.


2017 ◽  
Vol 470 (2) ◽  
pp. 2007-2017 ◽  
Author(s):  
W. S. G. Walker ◽  
M. Blackford ◽  
R. Butland ◽  
E. Budding

2010 ◽  
Vol 403 (3) ◽  
pp. 1448-1456 ◽  
Author(s):  
E. Budding ◽  
A. Erdem ◽  
G. İnlek ◽  
O. Demircan

1999 ◽  
Vol 118 (5) ◽  
pp. 2409-2423 ◽  
Author(s):  
Christopher J. Dolan and Robert D. Mathieu
Keyword(s):  

1997 ◽  
Vol 182 ◽  
pp. 391-405 ◽  
Author(s):  
Lee Hartmann

Outflows from low-mass young stellar objects are thought to draw upon the energy released by accretion onto T Tauri stars. I briefly summarize the evidence for this accretion and outline present estimates of mass accretion rates. Young stars show a very large range of accretion rates, and this has important implications for both mass ejection and for the structure of stellar magnetospheres which may truncate T Tauri disks.


2020 ◽  
Vol 501 (1) ◽  
pp. L12-L17
Author(s):  
Christina Schoettler ◽  
Richard J Parker

ABSTRACT Planetary systems appear to form contemporaneously around young stars within young star-forming regions. Within these environments, the chances of survival, as well as the long-term evolution of these systems, are influenced by factors such as dynamical interactions with other stars and photoevaporation from massive stars. These interactions can also cause young stars to be ejected from their birth regions and become runaways. We present examples of such runaway stars in the vicinity of the Orion Nebula Cluster (ONC) found in Gaia DR2 data that have retained their discs during the ejection process. Once set on their path, these runaways usually do not encounter any other dense regions that could endanger the survival of their discs or young planetary systems. However, we show that it is possible for star–disc systems, presumably ejected from one dense star-forming region, to encounter a second dense region, in our case the ONC. While the interactions of the ejected star–disc systems in the second region are unlikely to be the same as in their birth region, a second encounter will increase the risk to the disc or planetary system from malign external effects.


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