2023A&A...675A.114C


Query : 2023A&A...675A.114C

2023A&A...675A.114C - Astronomy and Astrophysics, volume 675A114 (2023/7-1)

Chasing extreme planetary architectures I. HD 196885 Ab, a super-Jupiter dancing with two stars?

CHAUVIN G., VIDELA M., BEUST H., MENDEZ R., CORREIA A.C.M., LACOUR S., TOKOVININ A., HAGELBERG J., BOUCHY F., BOISSE I., VILLEGAS C., BONAVITA M., DESIDERA S., FARAMAZ V., FORVEILLE T., GALLENNE A., HAUBOIS X., JENKINS J.S., KERVELLA P., LAGRANGE A.-M., MELO C., THEBAULT P., UDRY S. and SEGRANSAN D.

Abstract (from CDS):

Context. Planet(s) in binaries are unique architectures for testing predictions of planetary formation and evolution theories in very hostile environments. Their presence in such a highly perturbed region poses a clear challenge from the early phase of planetesimals accretion to the dynamical evolution and stability through a very long period of time (several Gyrs in some case).
Aims. The combination of radial velocity, speckle interferometry, high-contrast imaging and high-precision astrometry with interfer-ometry, offers a unique and unprecedented set of observable to push the exploration of the extreme planetary system HD 196885. By dissecting the physical and orbital properties of each component, we aim at shedding light on its global architecture and stability.
Methods. We used the IRDIS dual-band imager of SPHERE at VLT, and the speckle interferometric camera HRCAM of SOAR, to acquire high-angular resolution images of HD 196885 AB between 2015 and 2020. Radial velocity observations started in 1983 with CORAVEL at OHP have been extended with a continuous monitoring with CORALIE at La Silla, and ELODIE and SOPHIE at OHP over almost 40 yr extending the radial velocity measurements HD 196885 A and resolving both the binary companion and the inner giant planet HD 196885 Ab. Finally, we took advantage of the exquisite astrometric precision of the dual-field mode of VLTI/GRAVITY (down to 30 µas) to monitor the relative position of HD 196885 A and B to search for the 3.6 yr astrometric wobble of the circumpri-mary planet Ab imprinted on the binary separation.
Results. Our observations enable to accurately constrain the orbital properties of the binary HD 196885 AB, seen on an inclined and retrograde orbit (iAB = 120.43 deg) with a semi-major axis of 19.78 au, and an eccentricity of 0.417. The GRAVITY measurements confirm for the first time the nature of the inner planet HD 196885 Ab by rejecting all families of pole-on solutions in the stellar or brown dwarf masses. The most favored island of solutions is associated with a Jupiter-like planet (MAb = 3.39 MJup), with moderate eccentricity (eAaAb = 0.44), and inclination close to 143.04 deg. This results points toward a significant mutual inclination (Ф = 24.36 deg) between the orbital planes (relative to the star) of the binary companion B and the planet Ab. Our dynamical simulations indicate that the system is dynamically stable over time. Eccentricity and mutual inclination variations could be expected for moderate von Zipele Kozai Lidov cycles that may affect the inner planet.

Abstract Copyright: © The Authors 2023

Journal keyword(s): planet-star interactions - binaries close - planets and satellites: dynamical evolution and stability - instrumentation: high angular resolution - instrumentation: adaptive optics - instrumentation: spectrographs

Simbad objects: 25

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Number of rows : 25
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 2638 ** 00 29 59.8721784936 -05 45 50.396133276   10.33 9.38 9.10 9.19 K1V 108 1
2 HD 7449 PM* 01 14 29.3222869752 -05 02 50.614788804   8.08 7.48     F9.5V 137 2
3 HD 13445 PM* 02 10 25.9181700303 -50 49 25.465181208   6.945 6.117     K1.5V 484 1
4 HD 13445b Pl 02 10 25.9181700303 -50 49 25.465181208           ~ 110 1
5 V* GG Tau Or* 04 32 30.3506925552 +17 31 40.494063144 14.84 14.78 13.40 11.54   M0e+M2.0e 793 1
6 HD 41004 PM* 05 59 49.6501762752 -48 14 22.888358520   9.49 8.62     K1IV 221 1
7 HD 41004B * 05 59 49.6531151 -48 14 23.428302   13.85 12.33     M 67 1
8 HD 42936 SB* 06 06 29.8472551465 -72 30 45.567406069   10.00 9.09     K0IV/V 72 0
9 HD 59686 PM* 07 31 48.4045109592 +17 05 09.764723724   6.574 5.442     K2III 130 1
10 HD 87646 ** 10 06 40.7699030736 +17 53 42.278595144   8.73 8.07     G2V 78 0
11 MOA 2013-BLG-260 ** 17 52 07.49 -29 50 46.0           ~ 45 0
12 Kepler-693 Er* 18 53 00.8527467384 +40 21 29.620083492           ~ 51 0
13 HD 176051 SB* 18 57 01.60985 +32 54 04.5723 5.85 5.82   4.9   F9V+K1V 272 1
14 Kepler-1063 Ro* 19 22 06.418032 +38 08 34.72908   13.15 12.44 12.21   G5 44 0
15 Kepler-420 Ro* 19 24 54.0364030656 +44 55 38.524017504   15.830 14.867     G5V 66 0
16 Kepler-1505 Ro* 19 28 00.4859832288 +41 47 13.063606620           G0.5V 56 0
17 Kepler-1229 Er* 19 49 56.8076265768 +46 59 48.103495728       15.830   M0 62 0
18 HD 196885b Pl 20 39 51.8748403032 +11 14 58.700231052           ~ 50 1
19 HD 196885 SB* 20 39 51.8748403032 +11 14 58.700231052   6.92 6.385 6.32   F8V 220 1
20 HD 196885B * 20 39 51.90 +11 14 59.0     13.0     M1V 15 1
21 TYC 1096-637-1 * 20 39 53.2600568520 +11 18 00.676788732   10.95 10.55     ~ 2 0
22 HD 196895 * 20 41 36.5012278896 -37 47 40.957245132   9.35 8.87     F5V 7 0
23 HD 213885 PM* 22 35 56.3150949216 -59 51 52.075466892   8.56 7.94     G0/2V 72 0
24 * gam Cep b Pl 23 39 20.9104133784 +77 37 56.510781384           ~ 90 1
25 * gam Cep SB* 23 39 20.9104133784 +77 37 56.510781384 5.190 4.250   2.6   K1III-IVCN1 626 1

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