2022A&A...661A..63W


Query : 2022A&A...661A..63W

2022A&A...661A..63W - Astronomy and Astrophysics, volume 661A63-63 (2022/5-1)

Precise radial velocities of giant stars. XVI. Planet occurrence rates from the combined analysis of the Lick, EXPRESS, and PPPS giant star surveys.

WOLTHOFF V., REFFERT S., QUIRRENBACH A., JONES M.I., WITTENMYER R.A. and JENKINS J.S.

Abstract (from CDS):


Context. Radial velocity surveys of evolved stars allow us to probe a higher stellar mass range, on average, compared to main-sequence samples. Hence, differences between the planet populations around the two target classes can be caused by either the differing stellar mass or stellar evolution. To properly disentangle the effects of both variables, it is important to characterize the planet population around giant stars as accurately as possible.
Aims. Our goal is to investigate the giant planet occurrence rate around evolved stars and determine its dependence on stellar mass, metallicity, and orbital period.
Methods. We combine data from three different radial velocity surveys targeting giant stars: the Lick giant star survey, the radial velocity program EXoPlanets aRound Evolved StarS (EXPRESS), and the Pan-Pacific Planet Search (PPPS), yielding a sample of 482 stars and 37 planets. We homogeneously rederived the stellar parameters of all targets and accounted for varying observational coverage, precision and stellar noise properties by computing a detection probability map for each star via injection and retrieval of synthetic planetary signals. We then computed giant planet occurrence rates as a function of period, stellar mass, and metallicity, corrected for incompleteness.
Results. Our findings agree with previous studies that found a positive planet-metallicity correlation for evolved stars and identified a peak in the giant planet occurrence rate as a function of stellar mass, but our results place it at a slightly smaller mass of (1.68 ± 0.59) M☉. The period dependence of the giant planet occurrence rate seems to follow a broken power-law or log-normal distribution peaking at (718 ± 226) days or (797 ± 455) days, respectively, which roughly corresponds to 1.6 AU for a 1 M☉ star and 2.0 AU for a 2 M☉ star. This peak could be a remnant from halted migration around intermediate-mass stars, caused by stellar evolution, or an artifact from contamination by false positives. The completeness-corrected global occurrence rate of giant planetary systems around evolved stars is 10.7–1.6+2.2% for the entire sample, while the evolutionary subsets of RGB and HB stars exhibit 14.2–2.7+4.1% and 6.6–1.3+2.1%, respectively. However, both subsets have different stellar mass distributions and we demonstrate that the stellar mass dependence of the occurrence rate suffices to explain the apparent change of occurrence with the evolutionary stage.

Abstract Copyright: © ESO 2022

Journal keyword(s): planets and satellites: detection - techniques: radial velocities - brown dwarfs - planetary systems

VizieR on-line data: <Available at CDS (J/A+A/661/A63): table1.dat refs.dat>

Simbad objects: 65

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Number of rows : 65
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 5364 * 00 55 27.8202935136 -07 51 32.785557768   10.10 9.85     A1IV 11 0
2 * eta Cet c Pl? 01 08 35.3913324413 -10 10 56.151936084           ~ 7 0
3 * eta Cet HB* 01 08 35.3913324413 -10 10 56.151936084 5.80 4.61 3.45 2.61 2.03 K2-IIIb 239 0
4 * eta Cet b Pl? 01 08 35.3913324413 -10 10 56.151936084           ~ 6 0
5 HD 8541 * 01 24 48.1369846224 +28 51 25.004412468   9.34 8.22     K5 12 0
6 HD 9884 PM* 01 36 08.1488421384 -20 31 04.184453064   9.29 8.30     K0III 15 0
7 HD 11791 * 01 55 32.3210028888 -08 36 04.705113780   9.54 8.85     G5V 17 0
8 HD 16335 * 03 04 07.9677375264 +87 01 33.888152928   8.20 7.84     F0 14 0
9 HD 19011 PM* 03 04 49.8655413600 +39 32 12.917428044   9.04 8.64     F5 11 0
10 HD 20889 * 03 17 44.2298073408 -68 09 35.358080040   8.54 8.04     F5V 30 0
11 HD 24275 * 03 54 16.5465565152 +51 32 57.790773996   8.78 8.58     A3 15 0
12 HD 25723 * 04 04 22.7156192304 -12 47 32.268481764   6.688 5.611     K1III 49 0
13 * alf Tau LP? 04 35 55.23907 +16 30 33.4885 4.32 2.40 0.86 -0.37 -1.31 K5+III 1298 2
14 * k Tau PM* 04 58 09.3920531112 +25 03 01.464917904   5.803 5.785     A0V 74 0
15 HD 31674 * 05 03 47.5590780408 +70 04 19.117143264   9.74 8.79     G5 13 0
16 HD 33844b Pl 05 12 36.1003262136 -14 57 03.999312756           ~ 13 0
17 HD 33844c Pl 05 12 36.1003262136 -14 57 03.999312756           ~ 12 0
18 HD 33844 RG* 05 12 36.1003262136 -14 57 03.999312756   8.33 7.29     K0III 71 0
19 HD 34693 * 05 16 48.2330207400 -48 38 26.894649444   8.44 7.97     F5V 31 0
20 HD 36616 * 05 34 42.4721569416 +37 46 31.118095596   9.54 9.42     A0 5 0
21 HD 37826 Em* 05 41 06.2827602480 -04 58 10.717978332   9.99 9.32     G5V 7 0
22 HD 39177 ** 05 48 13.26275 -48 55 06.7536           A1V 17 0
23 HD 40526 * 05 56 01.3236582528 -55 59 07.337860260   9.96 9.39     F6V 14 0
24 HD 41704 * 06 02 09.9534057432 -63 32 43.193815260   9.336 8.845     F7V 22 0
25 HD 43803 * 06 17 18.1800338376 -21 44 33.075845664   9.17 8.21     G8III/IV 16 0
26 * nu.02 CMa b Pl 06 36 41.0376788353 -19 15 21.169452656           ~ 17 1
27 * nu.02 CMa PM* 06 36 41.0376788353 -19 15 21.169452656 5.96 5.011 3.91 3.13 2.61 K1.5III-IVFe1 282 1
28 * nu.02 CMa c Pl 06 36 41.0376788353 -19 15 21.169452656           ~ 6 0
29 HD 48455 * 06 43 07.3435604424 -08 29 38.622323220   10.20 10.24     B9Ib/II 4 0
30 HD 49129 * 06 45 54.4875157176 -25 53 58.443243144   10.15 10.08     A1/2(III) 9 0
31 HD 53261 * 07 04 41.9118252312 +05 55 32.700125604   8.99 7.88     K0 4 0
32 HD 56640 PM* 07 15 56.4620696662 -41 01 48.039876935   9.75 9.09     G3/5V 33 0
33 HD 60202 PM* 07 23 16.5651130848 -78 25 37.732799028   11.14 10.47     G5/8(IV) 5 0
34 HD 59686b Pl 07 31 48.4045109592 +17 05 09.764723724           ~ 19 1
35 HD 59686 PM* 07 31 48.4045109592 +17 05 09.764723724   6.574 5.442     K2III 130 1
36 HD 63242 * 07 48 04.0958789712 +05 11 58.690094568   9.40 9.38     A0 6 0
37 HD 65891 PM* 07 59 07.0602138096 -41 35 11.795455896   9.06 8.50     G0/2V 25 0
38 HD 67537 * 08 00 35.3405506488 -76 12 48.965399100   10.41 9.10     K0III 14 0
39 HD 67851 Em* 08 11 10.5644196960 +33 30 09.417452004   9.01 8.54     F8 7 0
40 * bet Cnc PM* 08 16 30.9209888482 +09 11 07.958245527 6.750 5.000 3.520 2.42 1.62 K4IIIBa0.5: 383 0
41 HD 70791 * 08 23 28.0249166640 -13 34 41.014376580   9.901 9.247     K2III 9 0
42 HD 74890 * 08 42 12.0223279056 -69 30 00.715481100   10.56 10.34     A5V 5 0
43 HD 75092 * 08 48 13.1004613224 +11 21 31.552108308   9.71 9.25     G 15 0
44 HD 75458 ** 08 49 17.79572 -26 25 27.9507           A0V 11 0
45 HD 76920b Pl 08 55 16.8171911352 -67 15 55.700929728           ~ 13 0
46 HD 79540 PM* 09 13 32.3436526368 -37 17 03.011425548   10.12 8.95     K1III 6 0
47 HD 84056 * 09 41 04.8446535504 -45 09 50.960659536   9.92 9.85     B9V 6 0
48 V* Y Dra Mi* 09 42 22.7374140072 +77 51 07.342357140   11.41 10.42     M5e 60 0
49 * 16 Sex * 10 09 14.8706760883 +06 10 15.237366354   7.93 6.58     K0 23 0
50 HD 90988 * 10 28 49.2824719632 -58 24 12.490134552   9.03 9.04     B9IV 14 0
51 * 44 UMa PM* 10 53 34.4520785448 +54 35 06.458632728   6.451 5.111     K3III 125 0
52 HD 95124 * 10 59 49.1817976344 +52 15 16.450681176 9.200 9.200 8.760     F5 17 0
53 HD 105854 PM* 12 11 03.6500716176 -50 00 32.927986296   9.19 8.68     F6V 29 0
54 HD 107089 * 12 18 47.4802967232 +10 06 13.924172808   9.62 9.18     F0 9 0
55 HD 107773 PM* 12 23 13.8898713539 -67 37 53.572986625   7.25 6.39     G8/K0IV 52 0
56 HD 108513 * 12 28 10.1335401072 -42 28 51.943225944   11.25 10.63     F5IV/V 5 0
57 HD 114933 * 13 14 00.2286252408 -08 48 43.141845456   10.96 10.13     K1V 12 0
58 V* V956 Cen pA* 13 14 08.2677843336 -54 41 34.639005336 9.83 9.66 9.23 8.96   F5Ia/ab 50 0
59 HD 116630 * 13 26 34.8190353840 -65 50 39.031875456   8.71 8.03     G2wF7V 29 0
60 HD 121056 RG* 13 53 52.0613118474 -35 18 51.691786471   7.21 6.19     K0III 96 0
61 * iot Dra b Pl 15 24 55.7746265 +58 57 57.834445           ~ 59 1
62 V* V Oph C* 16 26 43.7067710136 -12 25 35.816948688   12.91 7.30     C-N:4 154 0
63 * nu. Oph b Pl 17 59 01.5919129 -09 46 25.079852           ~ 16 1
64 * nu. Oph c Pl 17 59 01.5919129 -09 46 25.079852           ~ 18 1
65 * nu. Oph PM* 17 59 01.5922136612 -09 46 25.080976810 5.20 4.33 3.34 2.64 2.16 G9IIIa 226 1

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