2024A&A...686A..65B


Query : 2024A&A...686A..65B

2024A&A...686A..65B - Astronomy and Astrophysics, volume 686A65 (2024/6-1)

Short-period pulsating hot subdwarf stars observed by TESS II. Northern ecliptic hemisphere.

BARAN A.S., CHARPINET S., OSTENSEN R.H., REED M.D., VAN GROOTEL V., LYU C., TELTING J.H. and NEMETH P.

Abstract (from CDS):

We present the results of an extension of our Transiting Exoplanet Survey Satellite (TESS) search for short-period pulsations in compact stellar objects observed during the second and fourth years of the TESS mission, which targeted the northern ecliptic hemisphere. For many of the targets, we exploited unpublished spectroscopic data to confirm or re-evaluate the object's spectral classification. From the TESS photometry, we identified 50 short-period hot-subdwarf pulsators, including 35 sdB and 15 sdOB stars. The sample contains 26 pulsators that were unknown prior to the TESS mission. Nine stars show signals at both low and high frequencies and have been categorized as “hybrid” pulsators. For each pulsator, we report the list of prewhitened frequencies, along with and their amplitude spectra calculated from the TESS data. We attempt to identify possible multiplets caused by stellar rotation and we report five candidates with rotation periods between 11 and 46 d. With the search for p-mode pulsating hot subdwarfs in TESS Sectors 1-60 complete, we discuss the completeness of the study, as well as the instability strip and the evolutionary status of the stars we found. We also compare the distribution of pulsation periods as a function of effective temperature and surface gravity with theoretical predictions. We find that the percentage of undetected pulsators in the TESS mission increases with decreasing brightness measurements of stars, reaching 25% near the 15th magnitude. When comparing the distribution of hot subdwarfs in the log g - Teff plane with stellar models, we underline the importance of a proper treatment of the hydrogen-rich envelope composition (strongly affected by microscopic diffusion processes). We also emphasize that the stellar mass is a significant factor in understanding the instability strip. The p-mode instability strip is confirmed to be narrower than predicted by prior non-adiabatic calculations based on models incorporating equilibrium between gravitational settling and radiative levitation for iron. This implies that competing mixing processes ignored in these models must play a role in reducing the amount of levitating iron in the stellar envelope. Interestingly, we find that the coolest p-mode pulsators with Teff ≲ 30 000 K (including the hybrid ones) tend to cluster around the terminal age of the extreme horizontal branch of canonical mass (TAEHB at ∼0.47 M⊙). This trend is expected from the non-adiabatic pulsation calculations. Otherwise, the overall pulsation period distributions tend to reproduce the predicted trends in Teff and log g.

Abstract Copyright: © The Authors 2024

Journal keyword(s): stars: oscillations

Simbad objects: 71

goto Full paper

goto View the references in ADS

Number of rows : 71
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 HS 0039+4302 HS* 00 42 42.3970259304 +43 19 00.846907716   15.1       sdB 31 0
2 PG 0048+091 HS* 00 51 26.9371074840 +09 21 32.879383380   14.454 14.261 14.505   sdOB+F5V 37 0
3 GD 274 HS* 01 07 11.0202711624 +51 10 22.719103680   12.349 12.156 12.216   sdOB+F9.5VI 20 0
4 FBS 0117+396 HS* 01 20 22.9396883304 +39 50 59.434295604   15.15 15.34     sdB+dM 33 0
5 GD 1053 HS* 01 56 31.8993527208 -13 54 26.457259860   12.2   12.63 12.40 sdOB 25 0
6 V* BI Ari HS* 01 57 27.8862042360 +18 27 39.992930280   15.27       sdBO 21 0
7 HE 0230-4323 HS* 02 32 54.6772339416 -43 10 27.791218308     13.78     sdB 35 0
8 BPS CS 31064-0017 HS* 03 09 50.3919129744 -64 10 32.652350220 13.20 14.41 14.69 15.18   sdO 16 0
9 FBS 0315+417 HS* 03 18 23.0682070272 +41 55 21.761681628   14.57 14.62     sdB0.2He10+G/K 15 0
10 EC 03530-4024 HS* 03 54 46.5464099880 -40 15 32.569308288   14.518 14.721 15.251   sdB 11 0
11 GALEX J041550.2+015421 HS* 04 15 50.1643047048 +01 54 20.940589764   13.92 14.06 14.36   sdB 21 0
12 2MASS J04403897+7603264 HS* 04 40 38.9977667136 +76 03 26.329781700           sdB 8 0
13 KUV 04421+1416 HS* 04 44 56.8983457992 +14 21 50.176351836   15.28       sdB 46 0
14 GALEX J045515.2+130530 HS* 04 55 15.2317052592 +13 05 29.689559052   17.6   17.3   sdB 20 0
15 UCAC4 507-015874 HS? 05 52 59.9413351488 +11 18 45.983513988   13.367 13.384 13.534   ~ 9 0
16 GALEX J063952.0+515658 HS* 06 39 52.1822938800 +51 57 01.262380032   11.84 12.00     sdBHe1 21 0
17 HD 265435 HS* 06 53 24.3009681624 +33 03 34.242314004   11.84 11.78     sdOB 40 0
18 FBS 0658+627 HS* 07 03 31.7450624328 +62 36 26.335304244     13.10     sdB 15 0
19 V* DW Lyn HS* 07 07 09.7960158264 +60 38 50.159268348   14.7   15.34   sdB 61 1
20 FBS 0725+623 HS* 07 30 28.9983805440 +62 11 40.062237576     15.2     sdB 12 0
21 GALEX J074023.5+204938 HS* 07 40 23.5650807912 +20 49 37.041779316   15.391 15.552 15.872   sdB0.2He10 15 0
22 GALEX J074148.9+552451 HS* 07 41 49.1671783368 +55 24 50.690334924   14.549 14.688 14.903   sdB 9 0
23 UCAC4 568-042311 HS* 07 53 29.1133500312 +23 24 36.286991280   12.991 13.270 13.583   sdOB 10 0
24 Ton 4 HS* 08 01 27.5785740552 +25 57 42.942597804           sdB 9 0
25 GALEX J080656.7+152718 HS* 08 06 56.6844688416 +15 27 19.968237288   14.30 14.69 14.72 14.80 sdB 24 0
26 GALEX J081110.8+273420 HS* 08 11 10.8733468896 +27 34 20.501154840   13.02 12.42     sdB 6 0
27 2MASS J08124363+0600306 HS? 08 12 43.6398428784 +06 00 30.517170048           sd+K 11 0
28 GALEX J082116.5-082822 HS* 08 21 16.5160737624 -08 28 23.201898240   14.94 15.11 15.54   sdB 8 0
29 2MASS J08412266+0630294 HS* 08 41 22.6664257344 +06 30 29.639160936           sdO 11 0
30 2MASS J08515303+7901593 HS* 08 51 53.0485081008 +79 01 59.376320076           sdOB 10 0
31 GALEX J085649.3+170115 HS* 08 56 49.2697884816 +17 01 14.711098224     13.17     sdBHe2 29 0
32 GALEX J090204.5-072049 HS* 09 02 04.5196189416 -07 20 47.552714124   11.88 12.43     sdB 9 0
33 V* DT Lyn HS* 09 14 55.3780066224 +45 23 41.396157600   14.92       sdBO 34 0
34 PG 0958-116 HS* 10 00 41.8235310624 -11 51 34.585561008   15.01 15.26     sdB 27 0
35 V* UY Sex HS* 10 50 02.8265487864 -00 00 36.879009588 12.063 13.184 13.474 13.606 13.769 sdO9VIIHe6 175 0
36 Feige 48 HS* 11 47 14.4978515760 +61 15 31.789400364   13.12 13.28     sdB 125 0
37 Ton 74 HS* 12 03 41.2128307056 +25 31 11.544746520   15.1 15.164     sdB+dM 18 0
38 [GGM2006] 2657877 EB* 12 06 19.7873093304 +57 10 35.159392164   10.54 10.047 9.837 9.566 F5 23 0
39 PG 1203+574 HS* 12 06 24.4168350552 +57 09 36.147081312   14.55 14.87 15.35   sdOBHe9 26 0
40 PG 1219+534 HS* 12 21 29.0914917288 +53 04 36.796062144   12.41       sdB 90 1
41 BD-07 3477 HS* 12 44 20.2386233232 -08 40 16.846099536   10.46 10.594 10.895   sdB2VIIHe3 303 1
42 PG 1315+645 HS* 13 16 58.3477586352 +64 15 22.497839748   14.87 14.98 15.31   sdB+G: 16 0
43 V* NY Vir HS* 13 38 48.1466908176 -02 01 49.207286748   13.43 13.66 13.75   sdB1VIIHe1 237 1
44 PG 1409+605 HS* 14 11 01.8266771016 +60 14 11.634069840   14.64 14.46 14.55   sdBO 15 0
45 PG 1419+081 HS* 14 21 38.1803253744 +07 53 19.619422692 13.93 15.03 15.10 15.34   sdB+G5 16 0
46 HE 1450-0957 HS* 14 53 24.1992983688 -10 09 21.837230352   15.10 15.27     sdB 13 0
47 PG 1455+501 HS* 14 56 57.7339920504 +49 53 10.794332616   15.31 15.31 15.35   sdB+F2?kA2 15 0
48 FBS 1539+355 HS* 15 40 57.7311116568 +35 18 34.347470976           sdOB 12 0
49 PG 1544+601 HS* 15 45 09.6195862920 +59 55 05.085295860   14.74 14.56     sdB1.5VIIHe1 19 0
50 PG 1613+426 HS* 16 14 46.9286241816 +42 27 35.946945648   13.99 14.39 14.76   sdOA 33 0
51 PG 1618+563 HS* 16 19 26.9188578888 +56 06 01.009178568       13.93   sdB0VIIHe8 31 2
52 PG 1656+553 HS* 16 57 51.5925082104 +55 11 32.586737964   15.38 15.52 15.93   sdB 11 0
53 PG 1657+416 HS* 16 58 41.8362739056 +41 31 15.512739888   16.07 16.23 16.45   sdB+G5 25 0
54 TYC 4427-1021-1 HS* 17 04 58.3764154176 +73 04 43.201031304   10.57 10.90     sdB 11 0
55 LS IV +06 5 HS* 19 01 18.9660223824 +06 14 57.720641100   12.45 13.24     sdB 14 0
56 UCAC4 386-133403 HS* 19 24 08.6247332652 -12 58 30.926275280       15.500   sdB 4 0
57 UCAC4 686-068711 HS* 19 24 58.1497315488 +47 07 53.672050236   15.649 15.640 15.947   sdB 44 0
58 KPD 1930+2752 HS* 19 32 14.8088063952 +27 58 35.445679608 12.80 13.75 13.82     sdB 167 0
59 PSO J294.6167+58.4043 HS* 19 38 28.0265924376 +58 24 15.799663440           sdB 4 0
60 GALEX J193832.5+560944 HS* 19 38 32.4834894312 +56 09 44.574150636           sdB 10 0
61 UCAC4 741-063887 HS* 19 52 50.8362328272 +58 08 37.093139916   14.099 14.538 14.742   sdOB 4 0
62 GALEX J201337.6+092801 HS* 20 13 37.6121506872 +09 28 01.414212024   12.02 12.23 12.82   sdOB 15 0
63 UCAC2 28287515 HS* 20 24 44.4634305408 -10 22 44.056413480   13.47 13.68 14.00 13.91 sdB 6 0
64 PG 2052-003 HS* 20 55 32.1825667296 -00 04 53.581006092   15.9 15.9     sdB 12 0
65 KPD 2109+4401 HS* 21 11 47.6445824136 +44 13 50.620755936 12.14 13.11 13.30 13.64   sdB 72 0
66 PHL 211 HS* 21 55 17.0882131392 -10 25 02.491989348   14.025 14.198 14.412   sdB 8 0
67 V* V391 Peg HS* 22 04 12.1045050096 +26 25 07.819080600   14.41 14.61 15.00   sdB 112 2
68 TIC 2041859698 * 22 58 09.2559348244 +46 14 51.988381607           ~ 1 0
69 GALEX J225810.7+461435 HS* 22 58 10.7887516056 +46 14 35.193303744           sdB 4 0
70 PG 2303+019 HS* 23 06 22.3561075224 +02 09 05.952751128   16.2 16.23 16.2   sdB 20 0
71 Balloon 90100001 HS* 23 15 21.4810390968 +29 05 01.433373360   11.90 12.30     sdB 98 0

To bookmark this query, right click on this link: simbad:objects in 2024A&A...686A..65B and select 'bookmark this link' or equivalent in the popup menu