2014A&A...564A..93M


Query : 2014A&A...564A..93M

2014A&A...564A..93M - Astronomy and Astrophysics, volume 564A93-93 (2014/4-1)

On the structure of the transition disk around TW Hydrae.

MENU J., VAN BOEKEL R., HENNING T., CHANDLER C.J., LINZ H., BENISTY M., LACOUR S., MIN M., WAELKENS C., ANDREWS S.M., CALVET N., CARPENTER J.M., CORDER S.A., DELLER A.T., GREAVES J.S., HARRIS R.J., ISELLA A., KWON W., LAZIO J., LE BOUQUIN J.-B., MENARD F., MUNDY L.G., PEREZ L.M., RICCI L., SARGENT A.I., STORM S., TESTI L. and WILNER D.J.

Abstract (from CDS):

For over a decade, the structure of the inner cavity in the transition disk of TW Hydrae has been a subject of debate. Modeling the disk with data obtained at different wavelengths has led to a variety of proposed disk structures. Rather than being inconsistent, the individual models might point to the different faces of physical processes going on in disks, such as dust growth and planet formation. Our aim is to investigate the structure of the transition disk again and to find to what extent we can reconcile apparent model differences. A large set of high-angular-resolution data was collected from near-infrared to centimeter wavelengths. We investigated the existing disk models and established a new self-consistent radiative-transfer model. A genetic fitting algorithm was used to automatize the parameter fitting, and uncertainties were investigated in a Bayesian framework. Simple disk models with a vertical inner rim and a radially homogeneous dust composition from small to large grains cannot reproduce the combined data set. Two modifications are applied to this simple disk model: (1) the inner rim is smoothed by exponentially decreasing the surface density in the inner ∼3AU, and (2) the largest grains (>100µm) are concentrated towards the inner disk region. Both properties can be linked to fundamental processes that determine the evolution of protoplanetary disks: the shaping by a possible companion and the different regimes of dust-grain growth, respectively. The full interferometric data set from near-infrared to centimeter wavelengths requires a revision of existing models for the TW Hya disk. We present a new model that incorporates the characteristic structures of previous models but deviates in two key aspects: it does not have a sharp edge at 4AU, and the surface density of large grains differs from that of smaller grains. This is the first successful radiative-transfer-based model for a full set of interferometric data.

Abstract Copyright: ∼

Journal keyword(s): protoplanetary disks - techniques: interferometric - stars: individual: TW Hya

Simbad objects: 15

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Number of rows : 15
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 EM* LkCa 15 Or* 04 39 17.7911622816 +22 21 03.390090984   13.01 12.03 11.61   K5:Ve 792 1
2 QSO J1051-3138 Bla 10 51 04.77754627 -31 38 14.3076867   18.5 19.4 19   ~ 61 1
3 V* QR Hya SB* 10 56 31.1510369784 -34 33 50.152797252   9.63 8.399   7.706 G1V 43 0
4 CD-34 7135 PM* 11 00 02.7856829376 -35 06 36.552195792   12.76 11.212 10.801   M0.5Vk 26 0
5 TYC 7208-265-1 * 11 00 17.5329727752 -35 29 22.439603256   13.39 11.80 11.48   ~ 4 0
6 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
7 UCAC4 278-060962 * 11 02 38.6198384856 -34 33 30.885002748   13.132 11.495 11.109   ~ 4 0
8 HD 96997 SB* 11 09 44.4983352504 -32 19 35.778977112   9.36 8.37     K0III 17 0
9 HD 100546 Be* 11 33 25.4408872296 -70 11 41.241297948   6.71 6.30   6.64 A0VaekB8_lB 894 1
10 V* T Cha Or* 11 57 13.5245085552 -79 21 31.530508884   10.00 11.86     K0e 304 1
11 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
12 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
13 HD 142527 Ae* 15 56 41.8882637904 -42 19 23.248281828   9.04 8.34     F6III 741 1
14 EM* AS 209 TT* 16 49 15.3034917000 -14 22 08.643317664   12.62 11.28     K4Ve 494 0
15 HD 169142 Ae* 18 24 29.7799891464 -29 46 49.327400568   8.42 8.16     F1VekA3mA3_lB? 535 0

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