2023A&A...679A.104B


Query : 2023A&A...679A.104B

2023A&A...679A.104B - Astronomy and Astrophysics, volume 679A104 (2023/11-1)

In search of gravity mode signatures in main sequence solar-type stars observed by Kepler.

BRETON S.N., DHOUIB H., GARCIA R.A., BRUN A.S., MATHIS S., PEREZ HERNANDEZ F., MATHUR S., DYREK A., SANTOS A.R.G. and PALLE P.L.

Abstract (from CDS):

Gravity modes (g modes), mixed gravito-acoustic modes (mixed modes), and gravito-inertial modes (gi modes) possess unmatched properties as probes for stars with radiative interiors. The structural and dynamical constraints that they are able to provide cannot be accessed by other means. While they provide precious insights into the internal dynamics of evolved stars as well as massive and intermediate-mass stars, their non-detection in main sequence (MS) solar-type stars make them a crucial missing piece in our understanding of angular momentum transport in radiative zones and stellar rotational evolution. In this work, we aim to apply certain analysis tools originally developed for helioseismology in order to look for g-mode signatures in MS solar-type stars. We select a sample of the 34 most promising MS solar-type stars with Kepler four-year long photometric time series. All these stars are well-characterised late F-type stars with thin convective envelopes, fast convective flows, and stochastically excited acoustic modes (p modes). For each star, we compute the background noise level of the Fourier power spectrum to identify significant peaks at low frequency. After successfully detecting individual peaks in 12 targets, we further analyse four of them and observe distinct patterns of surrounding peaks with a low probability of being noise artifacts. Comparisons with the predictions from reference models suggest that these patterns are compatible with the presence of non-asymptotic low-order pure g modes, pure p modes, and mixed modes. Given their sensitivity to both the convective core interface stratification and the coupling between p- and g-mode resonant cavities, such modes are able to provide strong constraints on the structure and evolutionary states of the related targets. Considering the granulation and activity background of the stars in our sample, we subsequently compute the corresponding mode velocity necessary to trigger a detectable luminosity fluctuation. We use it to estimate the surface velocity, ⟨vr⟩, of the candidate modes we have detected. In this case, we find ⟨vr⟩∼10 cm s–1. These results could be extremely useful for characterising the deep interior of MS solar-type stars, as the upcoming PLATO mission will considerably expand the size of the available working sample.

Abstract Copyright: © The Authors 2023

Journal keyword(s): asteroseismology - stars: rotation - stars: solar-type

Simbad objects: 36

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Number of rows : 36
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+46 2555 Em* 18 47 39.2486448504 +46 41 09.979229364   9.98 9.52     F6IV 63 0
2 HD 175226 * 18 52 16.4984285976 +43 42 35.801031636   7.91 7.42     F6IV 84 0
3 HD 175289 PM* 18 52 36.1604006928 +45 08 23.345639700   9.95 9.50 9.44   F6IV 126 0
4 BD+45 2796 PM* 18 56 21.2642726544 +45 30 53.234154468   9.80 9.29     G0.5IV 110 0
5 BD+48 2798 * 18 56 53.3642741311 +48 41 38.346037602   10.086 9.562 9.609   F2 27 0
6 KOI-268 ** 19 02 54.9120176040 +38 30 25.083958896   11.13 10.59 10.583   ~ 68 0
7 HD 177723 Em* 19 03 45.1355799960 +45 36 30.189464856   9.54 9.10     F8IV 75 0
8 TYC 3124-850-1 * 19 05 37.8739768272 +39 43 09.853287060   10.36 9.88     F5IV-V 34 0
9 Kepler-25 Er* 19 06 33.2141354736 +39 29 16.358725104   11.337 10.623 10.622   F6 192 1
10 HD 178509 * 19 06 55.9481056080 +42 40 19.342963020   9.39 8.86     F8IV 66 0
11 HD 178688 * 19 07 43.5917202168 +41 56 15.730146420   9.48 9.02     F6IV 58 0
12 HD 178971 * 19 09 01.9438328856 +38 53 59.485809012   8.79 8.36     F5IV-V 81 0
13 Kepler-1713 Er* 19 09 22.9787972016 +43 22 42.207634092   11.474 10.982 10.901   F6IV 82 0
14 HD 179260 V* 19 10 11.6372611944 +38 04 55.831675296   8.94 8.49     F5IV-V 80 0
15 HD 179732 * 19 11 53.4817713600 +42 06 27.748644156   9.19 8.74     F5IV-V 61 0
16 Kepler-50 Er* 19 12 24.2128368312 +50 02 01.374741852   11.02 10.54 10.387   F5 131 1
17 Kepler-126 Er* 19 17 23.3505657144 +44 12 30.709225008   11.182 10.566 10.515   F7IV 108 0
18 BD+48 2887 Em* 19 22 20.2267974168 +48 41 43.496977812   9.43 9.01     F5IV 59 0
19 BD+36 3533 Em* 19 23 33.2215229808 +37 05 21.732235080   10.06 9.57     F5IV 29 0
20 BD+36 3570 * 19 28 19.8441075024 +37 03 35.403120000   9.40 8.97     F8IV 74 0
21 BD+47 2846 Er* 19 28 59.3538826128 +47 58 10.217007804   10.97 10.48     F6V 343 1
22 BD+47 2846b Pl 19 28 59.3538826128 +47 58 10.217007804           ~ 415 1
23 TYC 3143-53-1 SB* 19 35 03.7372740120 +42 44 16.724850540   10.31 9.85     F8IV 83 0
24 BD+46 2729 Em* 19 35 05.1660121440 +46 58 29.518389696   10.35 9.81     F6IV 42 0
25 BD+44 3183 Em* 19 35 50.5739000112 +44 52 50.022974316   9.38 8.92     hF6mF2gF5V 70 0
26 HD 185457 * 19 37 27.6974454120 +40 35 19.915408284   8.93 8.42     F8IV 52 0
27 TYC 3135-416-1 * 19 38 10.6797868344 +38 31 00.667275996   10.20 9.72     F5IV-V 43 0
28 HD 186096 Em* 19 40 27.1755476736 +45 41 45.850613064   9.10 8.69     F5V 33 0
29 BD+45 2960 Er* 19 43 12.6574592352 +45 59 17.085937164   10.16 9.64 9.575   F6IV 90 0
30 HD 186700 PM* 19 43 39.6223173216 +48 55 43.808906244   8.86 8.47     F5IV-V 84 0
31 TYC 3557-1752-1 * 19 44 10.6859489280 +45 53 21.115385016   11.39 10.86     ~ 38 0
32 BD+43 3349 * 19 45 23.9642658792 +44 04 35.865815844   10.01 9.51     F6IV 53 0
33 HD 234998 PM* 19 46 37.7417153592 +51 01 13.527778440   9.16 8.75     F5 67 0
34 HD 187637 PM* 19 49 18.1388793264 +41 34 56.859084552       7.2   F8V 132 0
35 TYC 3148-521-1 * 19 49 28.8561901056 +43 25 46.431332256   11.22 10.89     F7IV 45 0
36 BD+47 2934 SB* 19 50 14.2728443568 +47 28 25.166654760   9.68 9.24     F5IV-V 59 0

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