2023A&A...673A..14C


Query : 2023A&A...673A..14C

2023A&A...673A..14C - Astronomy and Astrophysics, volume 673A14 (2023/5-1)

Optical and near-infrared stellar activity characterization of the early M dwarf Gl 205 with SOPHIE and SPIRou.

CORTES-ZULETA P., BOISSE I., KLEIN B., MARTIOLI E., CRISTOFARI P.I., ANTONIADIS-KARNAVAS A., DONATI J.-F., DELFOSSE X., CADIEUX C., HEIDARI N., ARTIGAU E., BELLOTTI S., BONFILS X., CARMONA A., COOK N.J., DIAZ R.F., DOYON R., FOUQUE P., MOUTOU C., PETIT P., VANDAL T., ACUNA L., ARNOLD L., ASTUDILLO-DEFRU N., BOURRIER V., BOUCHY F., CLOUTIER R., DALAL S., DELEUIL M., DEMANGEON O.D.S., DUMUSQUE X., FORVEILLE T., GOMES DA SILVA J., HARA N., HEBRARD G., HOYER S., HUSSAIN G., KIEFER F., MORIN J., SANTERNE A., SANTOS N.C., SEGRANSAN D., STALPORT M. and UDRY S.

Abstract (from CDS):

Context. The stellar activity of M dwarfs is the main limiting factor in the discovery and characterization of the exoplanets orbiting them, because it induces quasi-periodic radial velocity (RV) variations.
Aims. We aim to characterize the magnetic field and stellar activity of the early, moderately active M dwarf Gl 205 in the optical and near-infrared (NIR) domains.
Methods. We obtained high-precision quasi-simultaneous spectra in the optical and NIR with the SOPHIE spectrograph and SPIRou spectropolarimeter between 2019 and 2022. We computed the RVs from both instruments and the SPIRou Stokes V profiles. We used Zeeman-Doppler imaging (ZDI) to map the large-scale magnetic field over the time span of the observations. We studied the temporal behavior of optical and NIR RVs and activity indicators with the Lomb-Scargle periodogram and a quasi-periodic Gaussian process regression (GPR). In the NIR, we studied the equivalent width of Al I, Ti I, K I, Fe I, and He I. We modeled the activity-induced RV jitter using a multi-dimensional GPR with activity indicators as ancillary time series.
Results. The optical and NIR RVs show similar scatter but NIR shows a more complex temporal evolution. We observe an evolution of the magnetic field topology from a poloidal dipolar field in 2019 to a dominantly toroidal field in 2022. We measured a stellar rotation period of Prot = 34.4 ± 0.5 days in the longitudinal magnetic field. Using ZDI, we measure the amount of latitudinal differential rotation (DR) shearing the stellar surface, yielding rotation periods of Peq = 32.0 ± 1.8 days at the stellar equator and Ppol = 45.5 ± 0.3 days at the poles. We observed inconsistencies in the periodicities of the activity indicators that could be explained by these DR values. The multi-dimensional GP modeling yields an RMS of the RV residuals down to the noise level of 3 m s–1 for both instruments while using Hα and the BIS in the optical and the full width at half maximum (FWHM) in the NIR as ancillary time series.
Conclusions. The RV variations observed in Gl 205 are due to stellar activity, with a complex evolution and different expressions in the optical and NIR revealed thanks to an extensive follow-up. Spectropolarimetry remains the best technique to constrain the stellar rotation period over standard activity indicators, particularly for moderately active M dwarfs.

Abstract Copyright: © The Authors 2023

Journal keyword(s): techniques: radial velocities - techniques: polarimetric - stars: activity - stars: low-mass - planets and satellites: detection

Simbad objects: 18

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Number of rows : 18
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 1326 PM* 00 18 22.8849799680 +44 01 22.637951588   9.61 8.14 7.3   M2V 602 0
2 HD 9407 PM* 01 34 33.2647932084 +68 56 53.289515638   7.21   6.1   G6.5V 175 0
3 BD+47 612b Pl 02 22 14.6437562448 +47 52 48.104862600           ~ 12 0
4 HD 36395 PM* 05 31 27.3957852161 -03 40 38.024004501 10.626 9.443 7.968 6.996 5.913 M1.5Ve 574 0
5 NGC 2682 OpC 08 51 23.5 +11 48 54           ~ 2528 0
6 BD+48 1829b Pl 10 02 21.7516616950 +48 05 19.685202030           ~ 6 0
7 HD 89269 PM* 10 18 51.9477652368 +44 02 53.954220509   7.31   6.2   G4V 160 0
8 V* AD Leo PM* 10 19 36.2808181226 +19 52 12.010446571   10.82 9.52 9.19   dM3 1469 1
9 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
10 V* DS Leo BY* 11 02 38.3420210088 +21 58 01.700013360 12.246 11.049 9.572 8.638 7.634 M1.0Ve 269 0
11 HD 95735b Pl 11 03 20.1948195942 +35 58 11.576182057           ~ 38 1
12 BD+11 2576 PM* 13 29 59.7858994351 +10 22 37.784532575 11.728 10.524 9.029 8.07 7.013 M1.0V 313 0
13 G 180-60 LM* 16 31 18.7890584283 +40 51 51.705530284   16.5   14.550   M6V 87 0
14 BD+18 3421 PM* 17 37 53.3468417549 +18 35 30.164096453 12.315 11.109 9.577 8.599 7.525 M1.5V 257 0
15 NAME Barnard's star BY* 17 57 48.4984700685 +04 41 36.113879676 12.497 11.24 9.511 8.298 6.741 M4V 907 2
16 * sig Dra PM* 19 32 21.5902098601 +69 39 40.235805206 5.860 5.460 4.680 4.04 3.63 K0V 691 0
17 HD 197481 BY* 20 45 09.5324974119 -31 20 27.237889841   10.05 8.627 9.078 6.593 M1VeBa1 1344 0
18 HD 209290 PM* 22 02 10.2750978279 +01 24 00.832158070 11.838 10.616 9.146 8.213 7.245 M0.5V 285 0

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