2025A&A...704A.283J


Query : 2025A&A...704A.283J

2025A&A...704A.283J - Astronomy and Astrophysics, volume 704A283 (2025/12-1)

Sub-Jupiter gas giants orbiting giant stars uncovered using a Bayesian framework.

JENKINS J.S., JONES M.I., VINES J.I., RUBENSTEIN R.I., PENA ROJAS P.A., WITTENMYER R., BRAHM R., TALA PINTO M. and CARSON J.

Abstract (from CDS):

Giant stars have been shown to be rich hunting grounds for those aiming to detect giant planets orbiting beyond ∼0.5 AU. Here we present two planetary systems around bright giant stars, found by combining the radial-velocity (RV) measurements from the EXPRESS and PPPS projects, and using a Bayesian framework. HIP 18606 is a naked-eye (V = 5.8 mag) KOIII star, and is found to host a planet with an orbital period of ∼675 days, and to have a minimum mass (m sini) of 0.8 MJ and a circular orbit. HIP 111909 is a bright (V = 7.4 mag) K1III star, and hosts two giant planets on circular orbits with minimum masses of m sini=1.2 MJ and m sini=0.8 MJ, and orbital periods of ∼490 d and ∼890 d, for planets b and c, respectively, strikingly close to the 5:3 orbital period ratio. An analysis of the 11 known giant star planetary systems arrive at broadly similar parameters to those published, whilst adding two new worlds orbiting these stars. With these new discoveries, we have found a total of 13 planetary systems (including three multiple systems) within the 37 giant stars that comprise the EXPRESS and PPPS common sample. Periodogram analyses of stellar activity indicators present possible peaks at frequencies close to the proposed Doppler signals in at least two planetary systems, HIP 24275 and HIP 90988, calling for more long-term activity studies of giant stars. Even disregarding these possible false positives, extrapolation leads to a fraction of 25-30% of low-luminosity giant stars hosting planets. We find that the mass function exponentially rises towards the lowest planetary masses; however, there exists a ∼93% probability that a second population of giant planets with minimum masses in the range 4-5 MJ is present, worlds that could have formed by the gravitational collapse of fragmenting protoplanetary disks. Finally, our noise modelling reveals a lack of statistical evidence for the presence of correlated noise at these RV precision levels, meaning white noise models are favoured for such datasets. However, different eccentricity priors can lead to significantly different results, advocating for model grid analyses such as those applied here to be regularly performed. By using our Bayesian analysis technique to better sample the posteriors, we are helping to extend the planetary mass parameter space to below 1 MJ, building the first vanguard of a new population of super-Saturns orbiting giant stars.

Abstract Copyright: © The Authors 2025

Journal keyword(s): planets and satellites: detection - planets and satellites: dynamical evolution and stability - planets and satellites: formation - planets and satellites: fundamental parameters - planets and satellites: gaseous planets - planet-star interactions

VizieR on-line data: <Available at CDS (J/A+A/704/A283): table1.dat table2.dat>

Simbad objects: 33

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Number of rows : 33
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 HD 11343c Pl 00 15 34.8933029664 -05 00 22.085150868           ~ 2 0
2 HD 11343 RG* 01 50 06.3304429512 -54 27 53.862367716   8.98 7.88     K2III/IV 39 0
3 HD 11343b Pl 01 50 06.3304429512 -54 27 53.862367716           ~ 8 0
4 HD 25069 RG* 03 58 52.3939149216 -05 28 11.811149040   6.848 5.833     K0/1III 86 0
5 HIP 18606b Pl 03 58 52.3939149216 -05 28 11.811149040           ~ 1 0
6 HIP 24275d Pl 05 12 36.1003262136 -14 57 03.999312756           ~ 1 0
7 HD 33844b Pl 05 12 36.1003262136 -14 57 03.999312756           ~ 13 0
8 HD 33844c Pl 05 12 36.1003262136 -14 57 03.999312756           ~ 12 0
9 HD 33844 RG* 05 12 36.1003262136 -14 57 03.999312756   8.33 7.29     K0III 71 0
10 HD 100939 RG* 11 36 48.1836900744 -37 02 20.660084772   9.02 7.93     K1III 27 0
11 HD 100939b Pl 11 36 48.1836900744 -37 02 20.660084772           ~ 6 0
12 HD 121056 RG* 13 53 52.0613118474 -35 18 51.691786471   7.21 6.19     K0III 96 0
13 HIP 67851d Pl 13 53 52.0613118474 -35 18 51.691786471           ~ 1 0
14 HD 135760b Pl 15 18 17.3304339000 -41 25 14.061113436           ~ 5 0
15 HD 135760 RG* 15 18 17.3304339000 -41 25 14.061113436   8.10 7.03     K1IIICNII 42 0
16 HD 136295 RG* 15 20 41.4181562928 -25 59 25.398360024   8.15 7.11     K0III 30 0
17 HIP 75092c Pl 15 20 41.4181562928 -25 59 25.398360024           ~ 1 0
18 HD 136295b Pl 15 20 41.4181562928 -25 59 25.398360024           ~ 4 0
19 HD 155233 RG* 17 11 04.3642247304 -20 39 16.446365136   7.843 6.818     K1III 43 0
20 HD 155233b Pl 17 11 04.3642247304 -20 39 16.446365136           ~ 7 0
21 * 42 Dra PM* 18 25 59.1369601368 +65 33 48.531343788   6.005 4.823     K1.5IIIFe-1 190 1
22 HIP 90988c Pl 18 33 33.3861526536 -50 12 41.747735484           ~ 1 0
23 HD 170707 RG* 18 33 33.3861526536 -50 12 41.747735484   8.81 7.76     K1III 30 0
24 HD 170707b Pl 18 33 33.3861526536 -50 12 41.747735484           ~ 5 0
25 HIP 95124b Pl 19 21 04.2304823448 -23 37 10.450151292           ~ 1 0
26 HD 181342 RG* 19 21 04.2304823448 -23 37 10.450151292   8.566 7.55   8.62 K0III 65 1
27 HIP 111909b Pl 22 40 07.1808004200 -49 35 53.755655460           ~ 1 0
28 HIP 111909c Pl 22 40 07.1808004200 -49 35 53.755655460           ~ 1 0
29 HD 214573 RG* 22 40 07.1808004200 -49 35 53.755655460   8.40 7.37     K1III 24 0
30 HD 219553 RG* 23 16 49.7046539400 -21 12 11.138418288   8.29 7.25     K0III 35 0
31 HD 219553b Pl 23 16 49.7046539400 -21 12 11.138418288           ~ 4 0
32 HD 222076b Pl 23 38 07.9443947544 -70 54 12.082254516           ~ 6 0
33 HD 222076 RG* 23 38 07.9443947544 -70 54 12.082254516   8.51 7.48     K1III 44 0

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