BM Cas – a long-period eclipsing young supergiant binary system in common envelope stage

2007 ◽  
Vol 26 (4-5) ◽  
pp. 339-350 ◽  
Author(s):  
I. Pustylnik ◽  
P. Kalv ◽  
V. Harvig ◽  
T. Aas
2005 ◽  
Vol 296 (1-4) ◽  
pp. 457-460 ◽  
Author(s):  
P. Kalv ◽  
V. Harvig ◽  
I. B. Pustylnik

2015 ◽  
Vol 576 ◽  
pp. L15 ◽  
Author(s):  
H. Olofsson ◽  
W. H. T. Vlemmings ◽  
M. Maercker ◽  
E. M. L. Humphreys ◽  
M. Lindqvist ◽  
...  

1989 ◽  
Vol 106 ◽  
pp. 234-234
Author(s):  
Joel A. Eaton

Binaries with very wide spearations are thought to evolve to small separations through a catastrophic form of mass exchange/loss known as common-envelope evolution. The theory of this process is fairly well developed, but proper tests remain elusive. Simply put, the theory argues that the rapidly shrinking Roche lobe of the mass losing giant will strip away the giant's main-sequence companion. Loss of mass from the system during the process carries away orbital angular momentum, thereby strengthening the effect.


1989 ◽  
Vol 8 ◽  
pp. 155-159
Author(s):  
R. E. Taam

AbstractThe current understanding of the common envelope binary phase of evolution is presented. The results obtained from the detailed computations of the hydrodynamical evolution of this phase demonstrate that the deposition of energy by the double core via frictional processes is sufficiently rapid to drive a mass outflow, primarily in the equatorial plane of the binary system. Specifically, recent calculations suggest that large amounts of mass and angular momentum can be lost from the binary system in a such a phase. Since the time scale for mass loss at the final phase of evolution is much shorter than the orbital decay time scale of the companion, the tranformation of binary systems from long orbital periods (> month) to short orbital periods (< day) is likely. The energy efficiency factor for the process is estimated to lie in the range between 0.3 and 0.6.


Science ◽  
2020 ◽  
Vol 367 (6476) ◽  
pp. 415-418 ◽  
Author(s):  
Anders Jerkstrand ◽  
Keiichi Maeda ◽  
Koji S. Kawabata

Superluminous supernovae radiate up to 100 times more energy than normal supernovae. The origin of this energy and the nature of the stellar progenitors of these transients are poorly understood. We identify neutral iron lines in the spectrum of one such supernova, SN 2006gy, and show that they require a large mass of iron (≳0.3 solar masses) expanding at 1500 kilometers per second. By modeling a standard type Ia supernova hitting a shell of circumstellar material, we produce a light curve and late-time iron-dominated spectrum that match the observations of SN 2006gy. In such a scenario, common envelope evolution of a progenitor binary system can synchronize envelope ejection and supernova explosion and may explain these bright transients.


1982 ◽  
Vol 70 ◽  
pp. 275-282 ◽  
Author(s):  
Bronislaw Rudak

AbstractThe evolutionary relations between symbiotic stars and cataclysmic variables are presented. The symbiotic stars are assumed to be long period detached binaries containing a carbon-oxygen degenerate primary and a red giant losing its mass through a spherically symmetric wind. Such systems can be obtained in Case C evolution, provided a common envelope during a rapid mass transfer phase was not formed. The same way recurrent novae containing a red giant as a secondary component may be produced. The factors influencing the differences between symbiotic stars and nova-type stars are discussed.


1980 ◽  
Vol 236 ◽  
pp. L25 ◽  
Author(s):  
R. N. Manchester ◽  
L. M. Newton ◽  
D. J. Cooke ◽  
A. G. Lyne
Keyword(s):  

Nature ◽  
1993 ◽  
Vol 361 (6407) ◽  
pp. 47-49 ◽  
Author(s):  
A. G. Lyne ◽  
J. D. Biggs ◽  
P. A. Harrison ◽  
M. Bailes

2005 ◽  
Vol 61 (5) ◽  
pp. 492-497 ◽  
Author(s):  
Kouichi Kifune ◽  
Yoshiki Kubota ◽  
Toshiyuki Matsunaga ◽  
Noboru Yamada

The crystal structure of the δ-phase in the Sb–Te binary system has been determined by synchrotron powder diffraction. It is clearly shown that many intermetallic compounds, which have different stacking periods depending on compound composition, exist in this phase. These structures are based on the cubic ABC stacking structure, and two kinds of fundamental structural units form an intergrowth along the stacking direction at the atomic level. The chemical formulae of these compounds are expressed as Sb2n Te3, where n is an integer and the number of stacking layers is 2n + 3. There is a relationship of inverse proportionality between the stacking period and the Te concentration.


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