2014A&A...568A..10G


Query : 2014A&A...568A..10G

2014A&A...568A..10G - Astronomy and Astrophysics, volume 568A10-10 (2014/8-1)

Impact on asteroseismic analyses of regular gaps in Kepler data.

GARCIA R.A., MATHUR S., PIRES S., REGULO C., BELLAMY B., PALLE P.L., BALLOT J., BARCELO FORTEZA S., BECK P.G., BEDDING T.R., CEILLIER T., ROCA CORTES T., SALABERT D. and STELLO D.

Abstract (from CDS):

The NASA Kepler mission has observed more than 190 000 stars in the constellations of Cygnus and Lyra. Around 4 years of almost continuous ultra high-precision photometry have been obtained reaching a duty cycle higher than 90% for many of these stars. However, almost regular gaps due to nominal operations are present in the light curves on different time scales. In this paper we want to highlight the impact of those regular gaps in asteroseismic analyses, and we try to find a method that minimizes their effect on the frequency domain. To do so, we isolate the two main time scales of quasi regular gaps in the data. We then interpolate the gaps and compare the power density spectra of four different stars: two red giants at different stages of their evolution, a young F-type star, and a classical pulsator in the instability strip. The spectra obtained after filling the gaps in the selected solar-like stars show a net reduction in the overall background level, as well as a change in the background parameters. The inferred convective properties could change as much as ∼200% in the selected example, introducing a bias in the p-mode frequency of maximum power. When asteroseismic scaling relations are used, this bias can lead to a variation in the surface gravity of 0.05 dex. Finally, the oscillation spectrum in the classical pulsator is cleaner than the original one.

Abstract Copyright: ∼

Journal keyword(s): asteroseismology - methods: data analysis - stars: oscillations

Simbad objects: 18

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Number of rows : 18
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 BD+47 2683 * 18 43 42.4230433392 +47 56 16.009897416   9.85 9.26     G0V 96 0
2 2MASS J18485932+4606494 HB* 18 48 59.3222984304 +46 06 49.523749704           G5V: 27 0
3 2MASS J18575109+4516185 HB* 18 57 51.1010459616 +45 16 18.505068456           K1IV 32 0
4 HD 178509 * 19 06 55.9481056080 +42 40 19.342963020   9.39 8.86     F8IV 66 0
5 HD 178688 * 19 07 43.5917202168 +41 56 15.730146420   9.48 9.02     F6IV 58 0
6 HD 178971 * 19 09 01.9438328856 +38 53 59.485809012   8.79 8.36     F5IV-V 81 0
7 HD 234856 Em* 19 17 45.8018919144 +50 28 48.274775580   9.87 9.32     F9IV-V 94 0
8 UCAC4 686-068711 HS* 19 24 58.1497315488 +47 07 53.672050236   15.649 15.640 15.947   sdB 44 0
9 BD+36 3570 * 19 28 19.8441075024 +37 03 35.403120000   9.40 8.97     F8IV 74 0
10 TYC 3134-265-1 RG* 19 28 25.6366451688 +37 41 23.242481304   12.20 11.02     G8IIIb 45 0
11 TYC 3143-53-1 SB* 19 35 03.7372740120 +42 44 16.724850540   10.31 9.85     F8IV 83 0
12 2MASS J19395195+4614405 RG* 19 39 51.9580178280 +46 14 40.508035368           K1III 34 0
13 2MASS J19453627+4106268 dS* 19 45 36.2787090216 +41 06 26.837885628           A7III 11 0
14 ASAS J195305+4510.5 LP* 19 53 04.8070546512 +45 10 35.026123800   12.89 12.87   8.876 M1.5II-III 6 0
15 2MASS J19554378+4527330 HB* 19 55 43.7863182336 +45 27 33.048299484           ~ 27 0
16 2MASS J19570850+4550466 HB* 19 57 08.5134701688 +45 50 46.685924160           G8IIp 27 0
17 TYC 3558-2149-1 HB* 19 57 10.6127556000 +45 37 36.362308080   12.67 11.74     G6V 25 0
18 2MASS J19583141+4556503 HB* 19 58 31.4156928144 +45 56 50.268671628           ~ 24 0

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