2010
DOI: 10.1088/0004-637x/724/1/546
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Interacting Binaries With Eccentric Orbits. Iii. Orbital Evolution Due to Direct Impact and Self-Accretion

Abstract: The rapid circularization and synchronization of the stellar components in an eccentric binary system at the onset of Roche lobe overflow is a fundamental assumption common to all binary stellar evolution and population synthesis codes, even though the validity of this assumption is questionable both theoretically and observationally. Here we calculate the evolution of the orbital elements of an eccentric binary through the direct three-body integration of a massive particle ejected through the inner Lagrangia… Show more

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Cited by 54 publications
(97 citation statements)
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“…et al , Motl et al 2007), while others suggest that much of the angular momentum can be fed back even in the absence of tidal coupling between the stars (Sepinsky et al 2010). However the best observational calibration of the space density of AM CVn stars gives a space density around a factor of 10 lower than previously assumed, and around 250 times lower than that of the detached systems, suggesting perhaps that in fact many detached DWDs do not survive mass transfer (Roelofs et al 2007).…”
Section: Spin-orbit Coupling and Am Cvn Numbersmentioning
confidence: 97%
“…et al , Motl et al 2007), while others suggest that much of the angular momentum can be fed back even in the absence of tidal coupling between the stars (Sepinsky et al 2010). However the best observational calibration of the space density of AM CVn stars gives a space density around a factor of 10 lower than previously assumed, and around 250 times lower than that of the detached systems, suggesting perhaps that in fact many detached DWDs do not survive mass transfer (Roelofs et al 2007).…”
Section: Spin-orbit Coupling and Am Cvn Numbersmentioning
confidence: 97%
“…Despite the relevance of nonzero eccentricity in mass transfer processes, binary population synthesis codes such as Star-Track (Belczynski et al 2008), BSE (Hurley et al 2002) and the updated binary c (Izzard et al 2004(Izzard et al , 2006(Izzard et al , 2009Claeys et al 2014), and SeBa (Portegies Zwart & Verbunt 1996;Toonen et al 2012), enforce circular orbits at the onset of mass transfer. Nevertheless, the problem of mass loss/mass transfer has been studied for over half a century (e.g., Huang 1956;Hadjidemetriou 1963;Kruszewski 1964;Piotrowski 1964;Matese & Whitmire 1983, 1984, and has received more recent attention in numerical studies (e.g., Regös et al 2005;Church et al 2009;Sepinsky et al 2010;Lajoie & Sills 2011a,b;van der Helm et al 2016;Bobrick et al 2017), as well as in (semi)analytical work (Sepinsky et al 2007b(Sepinsky et al , 2009(Sepinsky et al , 2010Veras et al 2011;Veras & Tout 2012;Veras et al 2013Veras et al , 2014Dosopoulou & Kalogera 2016a,b). Sepinsky et al (2007b) and Dosopoulou & Kalogera (2016b) in particular derived equations for the secular (i.e., orbit-averaged) changes of the orbital elements due to mass transfer in eccentric binaries.…”
Section: Introductionmentioning
confidence: 99%
“…However, it is not clear how to treat such cases. It seems that for some binary configurations RLOF may rather quickly circularize the orbit, while for others the eccentric periodic mass transfer at periastron may be a rather prolonged phase (Sepinsky et al 2010).…”
mentioning
confidence: 99%