Pulsations and period variations of the δ Scuti star AN Lyncis in a possible three-body system

Abstract Observations for the δ Scuti star AN Lyn have been made between 2008 and 2016 with the 85-cm telescope at Xinglong station of National Astronomical Observatories of China, the 84-cm telescope at SPM Observatory of Mexico and the Nanshan One metre Wide field Telescope of Xinjiang Observatory...

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Veröffentlicht in:Monthly notices of the Royal Astronomical Society 2018-01, Vol.473 (1), p.398-411
Hauptverfasser: Li, Gang, Fu, Jianning, Su, Jie, Fox-Machado, Lester, Michel, Raul, Guo, Zhen, Liu, Jinzhong, Feng, Guojie
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container_title Monthly notices of the Royal Astronomical Society
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Fu, Jianning
Su, Jie
Fox-Machado, Lester
Michel, Raul
Guo, Zhen
Liu, Jinzhong
Feng, Guojie
description Abstract Observations for the δ Scuti star AN Lyn have been made between 2008 and 2016 with the 85-cm telescope at Xinglong station of National Astronomical Observatories of China, the 84-cm telescope at SPM Observatory of Mexico and the Nanshan One metre Wide field Telescope of Xinjiang Observatory of China. Data in V in 50 nights and in R in 34 nights are obtained in total. The bi-site observations from both Xinglong Station and SPM Observatory in 2014 are analysed with Fourier Decomposition to detect pulsation frequencies. Two independent frequencies are resolved, including one non-radial mode. A number of stellar model tracks are constructed with the mesa code and the fit of frequencies leads to the best-fitting model with the stellar mass of M = 1.70 ± 0.05 M⊙, the metallicity abundance of Z = 0.020 ± 0.001, the age of 1.33 ± 0.01 billion years and the period change rate 1/P · dP/dt = 1.06 × 10−9 yr−1, locating the star at the evolutionary stage close to the terminal age main sequence. The O−C diagram provides the period change rate of (1/P)(dP/dt) = 4.5(8) × 10−7 yr−1. However, the period change rate calculated from the models is smaller in two orders than the one derived from the O−C diagram. Together with the sinusoidal function signature, the period variations are regarded to be dominated by the light-travel time effect of the orbital motion of a three-body system with two low-luminosity components, rather than the stellar evolutionary effect.
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Data in V in 50 nights and in R in 34 nights are obtained in total. The bi-site observations from both Xinglong Station and SPM Observatory in 2014 are analysed with Fourier Decomposition to detect pulsation frequencies. Two independent frequencies are resolved, including one non-radial mode. A number of stellar model tracks are constructed with the mesa code and the fit of frequencies leads to the best-fitting model with the stellar mass of M = 1.70 ± 0.05 M⊙, the metallicity abundance of Z = 0.020 ± 0.001, the age of 1.33 ± 0.01 billion years and the period change rate 1/P · dP/dt = 1.06 × 10−9 yr−1, locating the star at the evolutionary stage close to the terminal age main sequence. The O−C diagram provides the period change rate of (1/P)(dP/dt) = 4.5(8) × 10−7 yr−1. However, the period change rate calculated from the models is smaller in two orders than the one derived from the O−C diagram. 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Together with the sinusoidal function signature, the period variations are regarded to be dominated by the light-travel time effect of the orbital motion of a three-body system with two low-luminosity components, rather than the stellar evolutionary effect.</abstract><pub>Oxford University Press</pub><doi>10.1093/mnras/stx2331</doi><tpages>14</tpages></addata></record>
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