2023A&A...669A..59G


Query : 2023A&A...669A..59G

2023A&A...669A..59G - Astronomy and Astrophysics, volume 669A59 (2023/1-1)

The GRAVITY young stellar object survey IX. Spatially resolved kinematics of hot hydrogen gas in the star-disk interaction region of T Tauri stars.

GRAVITY COLLABORATION, WOJTCZAK J.A., LABADIE L., PERRAUT K., TESSORE B., SOULAIN A., GANCI V., BOUVIER J., DOUGADOS C., ALECIAN E., NOWACKI H., COZZO G., BRANDNER W., CARATTI O GARATTI A., GARCIA P., GARCIA LOPEZ R., SANCHEZ-BERMUDEZ J., AMORIM A., BENISTY M., BERGER J.-P., BOURDAROT G., CASELLI P., CLENET Y., DE ZEEUW P.T., DAVIES R., DRESCHER A., DUVERT G., ECKART A., EISENHAUER F., EUPEN F., FORSTER-SCHREIBER N.M., GENDRON E., GILLESSEN S., GRANT S., GRELLMANN R., HEISSEL G., HENNING T., HIPPLER S., HORROBIN M., HUBERT Z., JOCOU L., KERVELLA P., LACOUR S., LAPEYRERE V., LE BOUQUIN J.-B., LENA P., LUTZ D., MANG F., OTT T., PAUMARD T., PERRIN G., SCHEITHAUER S., SHANGGUAN J., SHIMIZU T., SPEZZANO S., STRAUB O., STRAUBMEIER C., STURM E., VAN DISHOECK E., VINCENT F. and WIDMANN F.

Abstract (from CDS):


Context. Hot atomic hydrogen emission lines in pre-main sequence stars serve as tracers for physical processes in the innermost regions of circumstellar accretion disks, where the interaction between a star and disk is the dominant influence on the formation of infalls and outflows. In the highly magnetically active T Tauri stars, this interaction region is particularly shaped by the stellar magnetic field and the associated magnetosphere, covering the inner five stellar radii around the central star. Even for the closest T Tauri stars, a region as compact as this is only observed on the sky plane at sub-mas scales. To resolve it spatially, the capabilities of optical long baseline interferometry are required.
Aims. We aim to spatially and spectrally resolve the Brγ hydrogen emission line with the methods of interferometry in order to examine the kinematics of the hydrogen gas emission region in the inner accretion disk of a sample of solar-like young stellar objects. The goal is to identify trends and categories among the sources of our sample and to discuss whether or not they can be tied to different origin mechanisms associated with Brγ emission in T Tauri stars, chiefly and most prominently magnetospheric accretion.
Methods. We observed a sample of seven T Tauri stars for the first time with VLTI GRAVITY, recording spectra and spectrally dispersed interferometric quantities across the Brγ line at 2.16 µm in the near-infrared K-band. We used the visibilities and differential phases to extract the size of the Brγ emission region and the photocentre shifts on a channel-by-channel basis, probing the variation of spatial extent at different radial velocities. To assist in the interpretation, we also made use of radiative transfer models of magnetospheric accretion to establish a baseline of expected interferometric signatures if accretion is the primary driver of Brγ emission.
Results. From among our sample, we find that five of the seven T Tauri stars show an emission region with a half-flux radius in the four to seven stellar radii range that is broadly expected for magnetospheric truncation. Two of the five objects also show Brγ emission primarily originating from within the co-rotation radius, which is an important criterion for magnetospheric accretion. Two objects exhibit extended emission on a scale beyond 10 R*, one of them is even beyond the K-band continuum half-flux radius of 11.3 R*. The observed photocentre shifts across the line can be either similar to what is expected for disks in rotation or show patterns of higher complexity.
Conclusions. Based on the observational findings and the comparison with the radiative transfer models, we find strong evidence to suggest that for the two weakest accretors in the sample, magnetospheric accretion is the primary driver of Brγ radiation. The results for the remaining sources imply either partial or strong contributions coming from additional, spatially extended emission components in the form of outflows, such as stellar or disk winds. We expect that in actively accreting T Tauri stars, these phenomena typically occur simultaneously on different spatial scales. Through more advanced modelling, interferometry will be a key factor in disentangling their distinct contributions to the total Brγ flux arising from the innermost disk regions.

Abstract Copyright: © The Authors 2023

Journal keyword(s): stars: formation - techniques: interferometric - techniques: high angular resolution - infrared: stars - accretion, accretion disks - stars: variables: T Tauri, Herbig Ae/Be

Simbad objects: 24

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Number of rows : 24
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 V* DG Tau TT* 04 27 04.6921275888 +26 06 16.060169268 13.57 13.97 10.50 12.28   K6Ve 1092 1
2 HD 37491 * 05 38 55.2904417632 -01 10 12.723143520   8.66 7.54     K0III 12 2
3 HD 95470 * 11 00 48.0843372168 -34 49 59.643331968   9.94 8.67     K2/3III 12 0
4 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
5 HD 99264 * 11 24 11.1271526712 -72 15 23.789086920 5.08 5.585 5.583     B2V 90 0
6 HD 142448 * 15 56 06.8383263792 -39 51 51.708250800   6.149 6.028     B9V 36 0
7 V* RU Lup TT* 15 56 42.3108692112 -37 49 15.473946900 9.27 10.07 9.60     K7/M0e 528 0
8 HD 147578 SB* 16 23 45.3315788376 -29 08 04.479565380   11.24 9.88     K0/2(III) 10 0
9 HD 147701 Ro* 16 24 21.3184926168 -25 01 31.448678376 9.66 9.74 9.20   7.42 B5III 143 0
10 Haro 1-16 Or* 16 31 33.4634997336 -24 27 37.158728076   14.02 12.80     K3e 266 0
11 HD 149562 * 16 36 38.6701215480 -25 19 50.490558192   11.01 9.81     K1(III) 7 0
12 HD 162926 * 17 55 08.0316869184 -36 28 32.320078824   6.113 6.053     B9.5III 33 0
13 V* VV Ser Ae* 18 28 47.8620017808 +00 08 39.923474964 12.99 12.63 11.80 11.01 10.24 A5Ve 262 0
14 NAME Serpens Cloud SFR 18 29 49 +01 14.8           ~ 1195 1
15 LBN 028.77+03.43 HII 18 31 26.5 -02 04 22           ~ 255 2
16 NAME Aql Rift DNe 18 32 -01.0           ~ 355 1
17 V* S CrA A Or* 19 01 08.5923211008 -36 57 19.736351172           ~ 43 0
18 V* S CrA Or* 19 01 08.597088 -36 57 19.89504   11.76 10.91 11.41   G0Ve+K0Ve 286 0
19 V* S CrA B Y*O 19 01 08.6478545856 -36 57 20.880059148           ~ 32 0
20 V* VV CrA Or* 19 03 06.7410913704 -37 12 49.686912432   16.45 14.67 14.12 11.62 K7 133 0
21 HH 32 HH 19 20 30 +11 02.0           ~ 109 1
22 EM* AS 353 Or* 19 20 30.9918166680 +11 01 54.605482968   13.22 12.21     K5 197 1
23 HD 183442 * 19 29 30.0750295248 +03 05 23.597895480   8.14 8.08     B3II/III 21 0
24 HD 188787 PM* 19 58 13.3552062456 -36 41 12.936195096   7.30 6.95     F2V 34 0

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