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   <dc:title>Young and Eccentric: The Quadruple System HD 86588</dc:title>
   <dc:creator>Tokovinin, Andrei</dc:creator>
   <dc:creator>Corbett, Hank</dc:creator>
   <dc:creator>Fors Aldrich, Octavi</dc:creator>
   <dc:creator>Howard, Ward</dc:creator>
   <dc:creator>Law, Nicholas M.</dc:creator>
   <dc:creator>Moe, Maxwell</dc:creator>
   <dc:creator>Ratzloff, Jeffrey K.</dc:creator>
   <dc:creator>Walter, Frederick M.</dc:creator>
   <dc:subject>Espectroscòpia astronòmica</dc:subject>
   <dc:subject>Interferometria</dc:subject>
   <dc:subject>Estels</dc:subject>
   <dc:subject>Astronomical spectroscopy</dc:subject>
   <dc:subject>Interferometry</dc:subject>
   <dc:subject>Stars</dc:subject>
   <dc:description>High-resolution spectroscopy and speckle interferometry reveal the young star HD 86588 as a quadruple system with a three-tier hierarchy. The 0 3 resolved binary A,B with an estimated period around 300 years contains the 8-yr pair Aa,Abc (also potentially resolvable), where Ab,Ac is a double-lined binary with equal components, for which we compute the spectroscopic orbit. Despite the short period of 2.4058 days, the orbit of Ab,Ac is eccentric (e=0.086±0.003)). It has a large inclination, but there are no eclipses; only a 4.4 mmag light modulation apparently caused by star spots on the components of this binary is detected with Evryscope. Assuming a moderate extinction of AV=0.5 mag and a parallax of 5.2 mas, we find that the stars are on or close to the main sequence (age >10 Myr) and their masses are from 1 to 1.3 solar. We measure the strength of the lithium line in the visual secondary B which, together with rotation, suggests that the system is younger than 150 Myr. This object is located behind the extension of the Chamaeleon I dark cloud (which explains extinction and interstellar sodium absorption), but apparently does not belong to it. We propose a scenario where the inner orbit has recently acquired its high eccentricity through dynamical interaction with the outer two components; it is now undergoing rapid tidal circularization on a timescale of ∼1 Myr. Alternatively, the eccentricity could be excited quasi-stationary by the outer component Aa.</dc:description>
   <dc:date>2019-06-06T11:27:11Z</dc:date>
   <dc:date>2019-06-06T11:27:11Z</dc:date>
   <dc:date>2018-08-24</dc:date>
   <dc:date>2019-06-06T11:24:41Z</dc:date>
   <dc:type>info:eu-repo/semantics/article</dc:type>
   <dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
   <dc:identifier>0004-6256</dc:identifier>
   <dc:identifier>https://hdl.handle.net/2445/134583</dc:identifier>
   <dc:identifier>689252</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>Reproducció del document publicat a: https://doi.org/10.3847/1538-3881/aad694</dc:relation>
   <dc:relation>Astronomical Journal, 2018, vol. 156, num. 3, p. 120-128</dc:relation>
   <dc:relation>https://doi.org/10.3847/1538-3881/aad694</dc:relation>
   <dc:rights>(c) American Astronomical Society, 2018</dc:rights>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:format>9 p.</dc:format>
   <dc:format>application/pdf</dc:format>
   <dc:publisher>Institute of Physics (IOP)</dc:publisher>
   <dc:source>Articles publicats en revistes (Institut de Ciències del Cosmos (ICCUB))</dc:source>
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