2014A&A...564A..36B


Query : 2014A&A...564A..36B

2014A&A...564A..36B - Astronomy and Astrophysics, volume 564A36-36 (2014/4-1)

Pulsating red giant stars in eccentric binary systems discovered from Kepler space-based photometry. A sample study and the analysis of KIC 5006817.

BECK P.G., HAMBLETON K., VOS J., KALLINGER T., BLOEMEN S., TKACHENKO A., GARCIA R.A., OSTENSEN R.H., AERTS C., KURTZ D.W., DE RIDDER J., HEKKER S., PAVLOVSKI K., MATHUR S., DE SMEDT K., DEREKAS A., CORSARO E., MOSSER B., VAN WINCKEL H., HUBER D., DEGROOTE P., DAVIES G.R., PRSA A., DEBOSSCHER J., ELSWORTH Y., NEMETH P., SIESS L., SCHMID V.S., PAPICS P.I., DE VRIES B.L., VAN MARLE A.J., MARCOS-ARENAL P. and LOBEL A.

Abstract (from CDS):

The unparalleled photometric data obtained by NASA's Kepler Space Telescope has led to improved understanding of red giant stars and binary stars. Seismology allows us to constrain the properties of red giants. In addition to eclipsing binaries, eccentric non-eclipsing binaries that exhibit ellipsoidal modulations have been detected with Kepler. We aim to study the properties of eccentric binary systems containing a red giant star and to derive the parameters of the primary giant component. We applied asteroseismic techniques to determine the masses and radii of the primary component of each system. For a selected target, light and radial velocity curve modelling techniques were applied to extract the parameters of the system and its primary component. Stellar evolution and its effects on the evolution of the binary system were studied from theoretical models. The paper presents the asteroseismic analysis of 18 pulsating red giants in eccentric binary systems, for which masses and radii were constrained. The orbital periods of these systems range from 20 to 440 days. The results of our ongoing radial velocity monitoring programme with the Hermes spectrograph reveal an eccentricity range of e=0.2 to 0.76. As a case study we present a detailed analysis of KIC5006817, whose rich oscillation spectrum allows for detailed seismic analysis. From seismology we constrain the rotational period of the envelope to be at least 165d, which is roughly twice the orbital period. The stellar core rotates 13 times faster than the surface. From the spectrum and radial velocities we expect that the Doppler beaming signal should have a maximum amplitude of 300ppm in the light curve. Fixing the mass and radius to the asteroseismically determined values, we find from our binary modelling a value of the gravity darkening exponent that is significantly larger than expected. Through binary modelling, we determine the mass of the secondary component to be 0.29±0.03M☉. For KIC5006817 we exclude pseudo-synchronous rotation of the red giant with the orbit. The comparison of the results from seismology and modelling of the light curve shows a possible alignment of the rotational and orbital axis at the 2σ level. Red giant eccentric systems could be progenitors of cataclysmic variables and hot subdwarf B stars.

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Journal keyword(s): stars: solar-type - binaries: general - stars: rotation - Sun: oscillations - stars: individual: KIC5006817 - asteroseismology

Simbad objects: 27

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Number of rows : 27
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NAME Magellanic Clouds GrG 03 00 -71.0           ~ 7988 0
2 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
3 * ksi Hya ** 11 33 00.1149306166 -31 51 27.447975478 5.17 4.47 3.54 2.84 2.36 G7IIIb 269 0
4 * alf Boo RG* 14 15 39.67207 +19 10 56.6730 2.46 1.18 -0.05 -1.03 -1.68 K1.5IIIFe-0.5 2417 1
5 * eps Oph PM* 16 18 19.2902245358 -04 41 33.047349888 4.95 4.21 3.23 2.54 2.05 G9.5IIIbFe-0.5 246 0
6 * eta Ser PM* 18 21 18.6004923875 -02 53 55.780691633 4.84 4.19 3.25 2.55 2.05 K0III-IV 390 0
7 KOI-7872 RG* 18 43 05.3027289192 +44 11 19.486992516   12.413 11.384 11.127   G6V 27 0
8 2MASS J18444602+4331298 EB* 18 44 46.0310511264 +43 31 29.848015308           ~ 13 0
9 2MASS J18473047+4401477 EB* 18 47 30.4720367856 +44 01 47.726464692           ~ 12 0
10 TYC 3130-2385-1 EB* 18 48 38.0888392752 +44 29 09.855904776   12.18 11.33     ~ 61 0
11 KOI-2659 EB* 18 59 11.2579653744 +45 05 56.661130968   14.219 13.263 12.981   K2III 39 0
12 KOI-6877 RG* 19 09 30.3904574928 +43 00 34.058927988   12.49 11.29     K1IV 54 0
13 KOI-3853 SB* 19 09 52.2909179328 +37 57 59.926091076   11.77 11.01 10.65   ~ 41 0
14 KOI-5112 RG* 19 21 49.4321812440 +40 08 44.635544808   12.39 11.15     K2IV 58 0
15 2MASS J19224440+4534060 RG* 19 22 44.4159668208 +45 34 06.039444720           K5II 31 0
16 2MASS J19235299+4358149 EB* 19 23 52.9889888736 +43 58 14.907231516           K2IV 22 0
17 TYC 3134-36-1 RG* 19 26 40.4816709552 +37 42 14.724305784   11.90 10.74     K3III 41 0
18 TYC 3146-611-1 RG* 19 28 19.0903164432 +44 19 18.595247268   13.35 11.71     G6V 64 0
19 2MASS J19315497+3754393 RG* 19 31 54.9712442064 +37 54 39.243676032           ~ 32 0
20 2MASS J19335837+4559153 EB* 19 33 58.3795906536 +45 59 15.317420676           ~ 25 0
21 TYC 3557-2118-1 EB* 19 41 20.9933729592 +45 30 17.199878004   10.67 9.82     G5 31 0
22 HD 187091 EB* 19 46 15.5312943504 +43 56 51.341798220   8.53 8.39     kA3hA5mA5(IV)sAm: 98 0
23 KOI-1807 EB* 19 47 42.9096949536 +47 52 58.874768148   11.04 9.98     ~ 28 0
24 TYC 3557-221-1 SB* 19 48 08.1620215896 +46 11 54.564197784   12.75 12.44     G6V 56 0
25 TYC 3561-481-1 RG* 19 51 46.7863903560 +48 33 27.988889904   12.91 11.93     G3V 34 0
26 2MASS J19533622+4010197 RG* 19 53 36.2226918648 +40 10 19.876118952           G9IIIb 28 0
27 TYC 3558-2210-1 SB* 20 00 16.3910995440 +45 06 05.887773324   12.94 11.80     G6V 23 0

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