2008A&A...477..839C


Query : 2008A&A...477..839C

2008A&A...477..839C - Astronomy and Astrophysics, volume 477, 839-852 (2008/1-3)

A search for mid-infrared molecular hydrogen emission from protoplanetary disks.

CARMONA A., VAN DEN ANCKER M.E., HENNING T., PAVLYUCHENKOV Y., DULLEMOND C.P., GOTO M., THI W.F., BOUWMAN J. and WATERS L.B.F.M.

Abstract (from CDS):

We report on a sensitive search for mid-infrared molecular hydrogen emission from protoplanetary disks. We observed the Herbig Ae/Be stars UX Ori, HD 34282, HD 100453, HD 101412, HD 104237 and HD 142666, and the T Tauri star HD 319139, and searched for H2 0-0 S(2) (J=4-2) emission at 12.278 micron and H2 0-0 S(1) (J=3-1) emission at 17.035 micron with VISIR, ESO-VLT's high-resolution mid-infrared spectrograph. None of the sources present evidence for molecular hydrogen emission at the wavelengths observed. Stringent 3σ upper limits to the integrated line fluxes and the mass of optically thin warm gas (T=150, 300 and 1000K) in the disks are derived. The disks contain less than a few tenths of Jupiter mass of optically thin H2 gas at 150K, and less than a few Earth masses of optically thin H2 gas at 300 K and higher temperatures. We compare our results to a Chiang & Goldreich (1997ApJ...490..368C, CG97) two-layer disk model of masses 0.02M and 0.11M. The upper limits to the disk's optically thin warm gas mass are smaller than the amount of warm gas in the interior layer of the disk, but they are much larger than the amount of molecular gas expected to be in the surface layer. If the two-layer approximation to the structure of the disk is correct, our non-detections are consistent with the low flux levels expected from the small amount of H2 gas in the surface layer. We present a calculation of the expected thermal H2 emission from optically thick disks, assuming a CG97 disk structure, a gas-to-dust ratio of 100 and Tgas = Tdust. We show that the expected H2 thermal emission fluxes from typical disks around Herbig Ae/Be stars are of the order of 10–16 to 10–17erg/s/cm2 for a distance of 140pc. This is much lower than the detection limits of our observations (5x10–15erg/s/cm2). H2 emission levels are very sensitive to departures from the thermal coupling between the molecular gas and dust in the surface layer. Additional sources of heating of gas in the disk's surface layer could have a major impact on the expected H2 disk emission. Our results suggest that in the observed sources the molecular gas and dust in the surface layer have not significantly departed from thermal coupling (Tgas/Tdust<2) and that the gas-to-dust ratio in the surface layer is very likely lower than 1000.

Abstract Copyright:

Journal keyword(s): stars: emission-line, Be - stars: pre-main sequence - planetary systems: protoplanetary disks

CDS comments: In paragraphe 5.3 L551 IRS5 is a misprint for Name LDN 1551 IRS 5, and the ref. Richter et al. 2004 is a misprint for Richter et al. 2002.

Simbad objects: 33

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Number of rows : 33
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 * gam Eri LP? 03 58 01.7658213057 -13 30 30.653301544 6.52 4.54 2.94 1.68 0.68 M0III-IIIb 189 0
2 V* DG Tau Or* 04 27 04.6921275888 +26 06 16.060169268 13.57 13.97 10.50 12.28   K6Ve 1024 1
3 RAFGL 5123 Y*O 04 31 34.07736 +18 08 04.9020           K3V/M3III 863 0
4 V* GG Tau Or* 04 32 30.3506925552 +17 31 40.494063144 14.84 14.78 13.40 11.54   M0e+M2.0e 736 1
5 EM* LkCa 15 Or* 04 39 17.7911622816 +22 21 03.390090984   13.01 12.03 11.61   K5:Ve 690 1
6 V* AB Aur Ae* 04 55 45.8458932216 +30 33 04.292077032 7.20 7.16 7.05 6.96 6.70 A0Ve 1067 2
7 HD 31648 Ae* 04 58 46.2655706952 +29 50 36.987625680 7.84 7.78 7.62 7.76 7.43 A5Vep 518 0
8 V* UX Ori Ae* 05 04 29.9878898040 -03 47 14.286732072 10.25 10.93 8.70 9.62 9.43 A4IVe 363 1
9 V* V1366 Ori Ae* 05 16 00.4765181328 -09 48 35.393784012 10.19 10.16 9.84 9.77 9.63 B9.5V 209 0
10 V* GW Ori Or* 05 29 08.3928710640 +11 52 12.666457092   10.83 10.10 9.52   G5/8Ve 351 0
11 * 31 Ori V* 05 29 43.9820095248 -01 05 32.058334392   6.28 4.71     K4III 91 0
12 HD 36112 Ae* 05 30 27.5285630040 +25 19 57.076288752   8.57 8.27     A8Ve 469 0
13 V* CQ Tau Ae* 05 35 58.4666264136 +24 44 54.091450572 11.290 10.780 10.000   8.33 F5IVe 310 0
14 * q Car LP* 10 17 04.9755364660 -61 19 56.296709026   4.899 3.350     K2.5II 138 0
15 HD 91056 * 10 28 52.5748022328 -64 10 20.207849736   7.11 5.27   8.65 M0III 41 0
16 * gam Cha V* 10 35 28.1055499388 -78 36 28.038741243 7.65 5.70 4.12 2.86 1.88 K4III 79 0
17 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 1892 1
18 Ass Cha T 2-21 TT* 11 06 15.3471261840 -77 21 56.720362608   12.58 11.01   9.35 G5Ve 131 0
19 IRAS 11057-7706 Y*O 11 07 09.19896 -77 23 04.9920           ~ 63 0
20 HD 97048 Ae* 11 08 03.3109731720 -77 39 17.490777444 9.03 8.76 9.00   8.64 A0Vep 543 0
21 HJM C 1-8 Y*O 11 10 11.3918141448 -76 35 29.247545184         13.75 K5Ve 59 0
22 HD 100453 Ae* 11 33 05.5766482920 -54 19 28.547100696   8.09 7.79     F1Vn 284 1
23 HD 101412 Be* 11 39 44.4564911064 -60 10 27.719780304   9.465 9.288     A3VaekA0mA0_lB 139 0
24 V* DX Cha Ae* 12 00 05.0868602544 -78 11 34.565724312   6.81 6.60     A4V 344 0
25 HD 142666 TT* 15 56 40.0221861696 -22 01 40.005872148 9.41 9.37 8.82 8.31 8.01 F0V_sh 269 0
26 WRAY 16-203 Or* 16 08 29.7275063376 -39 03 11.024360496   16.26 15.91 15.38 15.69 K0: 171 1
27 HD 150193 Ae* 16 40 17.9243127240 -23 53 45.193372692 9.69 9.32 8.79 8.41   A3Va(e) 321 0
28 HD 163296 Ae* 17 56 21.2881851168 -21 57 21.871819008 7.00 6.93 6.85 6.86 6.67 A3VaekA1mA1 1111 0
29 HD 319139 SB* 18 14 10.4818675368 -32 47 34.516836060   11.47 10.68   9.11 K5+K7 357 0
30 * lam Sgr PM* 18 27 58.2407185 -25 25 18.114589 4.75 3.85 2.81 2.06 1.50 K1IIIb 277 0
31 2MASS J18295571+0114315 Y*O 18 29 55.711 +01 14 31.50           ~ 39 0
32 HBC 672 Em* 18 29 56.8848005064 +01 14 46.304766672   17.6       K8.0 102 0
33 [EC92] 95 Y*O 18 29 57.893 +01 12 46.25           K1.0 73 3

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