2022A&A...663A.160B


Query : 2022A&A...663A.160B

2022A&A...663A.160B - Astronomy and Astrophysics, volume 663A, 160-160 (2022/7-1)

The polar orbit of the warm Neptune GJ 436b seen with VLT/ESPRESSO.

BOURRIER V., ZAPATERO OSORIO M.R., ALLART R., ATTIA O., CRETIGNIER M., DUMUSQUE X., LOVIS C., ADIBEKYAN V., BORSA F., FIGUEIRA P., GONZALEZ HERNANDEZ J.I., MEHNER A., SANTOS N.C., SCHMIDT T., SEIDEL J.V., SOZZETTI A., ALIBERT Y., CASASAYAS-BARRIS N., EHRENREICH D., LO CURTO G., MARTINS C.J.A.P., DI MARCANTONIO P., MEGEVAND D., NUNES N.J., PALLE E., PORETTI E. and SOUSA S.G.

Abstract (from CDS):

GJ 436b might be the prototype of warm Neptunes that have undergone late migration induced by an outer companion. Precise determination of the orbital architecture of such systems is critical to constraining their dynamical history and evaluating the role of delayed migration in the exoplanet population. To this purpose we analyzed the Rossiter-McLaughlin (RM) signal of GJ 436 b in two transits - recently observed with ESPRESSO - using three different techniques. The high level of precision achieved in radial velocity (RV) measurements allows us to detect the deviation from the Keplerian orbit, despite the slow rotation of the M dwarf host (v sin i* = 272.0–34.0+40.0 m s–1), and to measure the sky-projected obliquity (λ = 102.5–18.5+17.2°). The Reloaded RM technique, which allows the stellar RV field along the transit chord to be analyzed, yields λ = 107.5–19.3+26.6° and v sin i* = 292.9–49.9+41.9 m s–1. The RM Revolutions technique, which allows us to fit the spectral profiles from all planet-occulted regions together, yields λ = 114.1–17.8+22.8° and v sin i* = 300.5–57.0+45.9 m s–1. The consistent results between these three techniques, and with published results from HARPS/HARPS-N data, confirm the polar orbit of GJ 436b and support the hypothesis that its origin lies in Kozai migration. Results from a joint RM Revolutions analysis of the ESPRESSO, HARPS, and HARPS-N datasets (λ = 113.5–17.3+23.3°; v sin i* = 293.5–52.2+43.7 m s–1) combined with a revised stellar inclination (i* = 35.7–7.6+5.9° or 144.2–5.9+7.6°) lead us to constrain the 3D obliquity Ψ to 103.2–11.5+12.8°.

Abstract Copyright: © ESO 2022

Journal keyword(s): methods: data analysis - techniques: spectroscopic - planets and satellites: individual: GJ436b

Simbad objects: 6

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Number of rows : 6
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 HD 3167b Pl 00 34 57.5242131960 +04 22 53.284093032           ~ 65 0
2 NAME LP 424-4b Pl 07 59 05.8395356736 +15 23 29.236065000           ~ 301 1
3 Ross 905b Pl 11 42 11.0933350978 +26 42 23.650782778           ~ 810 1
4 Ross 905 PM* 11 42 11.0933350978 +26 42 23.650782778   12.06 10.613 10.272 8.24 M3V 645 1
5 K2-235b Pl 12 33 32.8441110816 -10 08 46.225572324           ~ 170 0
6 BD+47 2936b Pl 19 50 50.2472976936 +48 04 51.101390496           ~ 416 1

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