2012A&A...538A.101V


Query : 2012A&A...538A.101V

2012A&A...538A.101V - Astronomy and Astrophysics, volume 538A101-101 (2012/2-1)

A mid-IR study of the circumstellar environment of Herbig Be stars.

VERHOEFF A.P., WATERS L.B.F.M., VAN DEN ANCKER M.E., MIN M., STAP F.A., PANTIN E., VAN BOEKEL R., ACKE B., TIELENS A.G.G.M. and DE KOTER A.

Abstract (from CDS):

The study of the formation of massive stars is complicated because of the short times scales, large distances, and obscuring natal clouds. There are observational and theoretical indications that the circumstellar environment of Herbig Be (HBe) stars is substantially different from that of their lower mass counterparts, the T Tauri and Herbig Ae stars. We map the spatial distribution and mineralogy of the warm circumstellar dust of a sample of HBe stars. We compare our results to a sample of less massive Herbig Ae stars. We used literature photometry to obtain optical extinctions and stellar parameters of the targets. We obtained N-band imaging and long-slit spectroscopic data with the VISIR instrument at the VLT and we analyzed these data. We performed photometry of the images and extracted spatial information. We corrected the spectra for extinction and performed mineralogical fits. We fitted Gaussian profiles to characterize the spatial extent of the spectra along the VISIR slit. We find that the mid-infrared (IR) emission of the HBe stars is typically characterized by a circumstellar disk that efficiently reprocesses a substantial portion of the stellar flux. The mid-IR flux levels, the spatial compactness, and the dust composition are quite similar to those of the Herbig Ae stars. We find upper limits to the full-width-at-half-maximum (FWHM) size of the mid-IR emission of ∼500AU. The main differences with the lower mass stars are the lower overall IR excess with a greater variety in shapes, the weaker PAH reprocessing power, and the lack of a silica-forsterite relation. The discrepancies between VISIR and IRAS photometry, the far-IR contributions and the large PAH sizes of HBe stars are attributed to natal clouds. Our results suggest that the Herbig Be disks are flatter than those around lower mass stars and they are likely truncated from the outside by photoevaporation.

Abstract Copyright: ∼

Journal keyword(s): stars: formation - stars: pre-main sequence - protoplanetary disks - stars: variables: T Tauri, Herbig Ae/Be - infrared: stars

Simbad objects: 74

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Number of rows : 74
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 * tet Cet HB* 01 24 01.4032816333 -08 10 59.739230440 5.57 4.65 3.59 2.83 2.26 K0IIIb 206 0
2 * alf Hor PM* 04 14 00.1142226166 -42 17 39.726755131 5.97 4.96 3.86 3.00 2.41 K2III 150 0
3 * eps Lep PM* 05 05 27.6644072506 -22 22 15.724153311 6.41 4.64 3.18 2.08 1.27 K4III 169 0
4 V* WZ Dor LP* 05 07 34.0268609928 -63 23 58.847362584   6.776 5.205     M3III 50 0
5 HD 33554 * 05 11 41.5640776330 +16 02 44.429903368   6.703 5.163     K5III 71 0
6 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
7 EM* MWC 778 Y*O 05 50 13.8981046536 +23 52 17.846993280 13.45 13.72 12.80     BQ[] 30 1
8 HD 41047 * 06 01 16.2976481208 -33 54 42.608011716   7.102 5.524     K5III 42 0
9 HD 250550 Ae* 06 01 59.9892055464 +16 30 56.727549864   9.60 9.593 9.64   B9e 254 1
10 EM* LkHA 208 Ae* 06 07 49.5332003976 +18 39 26.487297072   11.78 11.30 11.39   F0Ve 129 1
11 EM* LkHA 339 Ae* 06 10 57.8449670232 -06 14 39.659250840   14.44 13.60 13.44 12.50 A1e 44 0
12 * eta Gem RG* 06 14 52.6452865329 +22 30 24.434377815 6.55 4.89 3.28 1.79 0.48 M2IIIa 267 0
13 EM* MWC 137 Ae* 06 18 45.5220873216 +15 16 52.244494608 12.89 13.30 13.759 11.67 10.31 sgB[e]d 259 1
14 * alf Car * 06 23 57.10988 -52 41 44.3810 -0.49 -0.59 -0.74 -0.96 -1.13 A9II 461 1
15 EM* LkHA 215 Ae* 06 32 41.7730499472 +10 09 34.209036180 11.41 11.28 10.70     B7IIne 135 0
16 HD 259431 Ae* 06 33 05.1906369144 +10 19 19.982565336 8.39 8.95 8.72     B6ep 299 1
17 V* R Mon Ae* 06 39 09.9542000448 +08 44 09.539482632 10.76 12.46 11.85 10.96 10.25 B8IIIe 525 0
18 * alf CMa SB* 06 45 08.91728 -16 42 58.0171 -1.51 -1.46 -1.46 -1.46 -1.43 A0mA1Va 1610 0
19 * 87 Gem * 06 51 59.9861723112 +23 36 06.199162452   7.142 5.671     K5III 52 0
20 * del CMa s*y 07 08 23.4840514 -26 23 35.518484 3.06 2.52 1.84 1.33 1.00 F8Ia 348 0
21 RAFGL 5223 Or* 07 08 38.7906809616 -04 19 04.847636136 12.48 12.71 12.06     B0 46 0
22 SS 103 Ae* 07 19 35.9395695288 -17 39 17.935943004 14.61 15.016 13.582 13.080   B2?e 63 0
23 HD 64315 EB* 07 52 20.2841727949 -26 25 46.683038109 8.76 9.49 9.24 9.63 8.86 O5.5Vz+O7V 124 1
24 * gam Pyx PM* 08 50 31.9225999562 -27 42 35.429733075 6.67 5.27 4.01 3.06 2.39 K2.5III 122 0
25 * alf Hya * 09 27 35.24270 -08 39 30.9583 5.14 3.42 1.97 0.93 0.16 K3IIIa 455 1
26 HD 85567 Be* 09 50 28.5375988920 -60 58 02.954048268 8.16 8.67 8.57     B5Vne 105 0
27 * q Car LP* 10 17 04.9755364660 -61 19 56.296709026   4.899 3.350     K2.5II 147 0
28 V* GZ Vel LP* 10 19 36.7527129364 -55 01 45.499187932   6.146 4.543     K2.5II 62 0
29 * eps Crt * 11 24 36.5912121144 -10 51 33.575503752   6.338 4.802     K4III 95 0
30 * e Cen PM* 12 53 06.9063292060 -48 56 35.926377300 7.28 5.70 4.33 3.35 2.60 K3/4III 57 0
31 * psi Vir LP* 12 54 21.1630369857 -09 32 20.360128902 7.94 6.39 4.80 3.23 1.95 M3-III 173 0
32 CD-48 7859 Be* 13 01 17.8030714320 -48 53 18.799911852   10.65 10.58     B5e 61 0
33 * pi. Hya PM* 14 06 22.2980035207 -26 40 56.501676257 5.45 4.41 3.28 2.40 1.85 K2-IIIFe-0.5 150 0
34 HD 133550 * 15 06 13.9341217488 -36 15 52.566911064   7.923 6.269     K5III 29 0
35 * ome Lup PM* 15 38 03.2069631593 -42 34 02.408479318 7.47 5.75 4.33 3.30 2.57 K3III 66 0
36 * 42 Lib * 15 40 16.8973226160 -23 49 05.101136148 7.80 6.29 4.96 4.00 3.32 K3-IIICN2 121 0
37 * alf Ser PM* 15 44 16.0741095811 +06 25 32.268792881 5.080 3.800 2.630 1.82 1.25 K2IIIbCN1 533 0
38 HD 141926 HXB 15 54 21.7677373488 -55 19 44.310748620 8.71 9.47 9.13 9.38   B2IIIn 86 0
39 * chi Sco * 16 13 50.9062585128 -11 50 15.892301544   6.615 5.239     K3III 83 0
40 * del Oph PM* 16 14 20.7390218758 -03 41 39.572826363 6.30 4.34 2.75 1.46 0.43 M0.5III 377 0
41 V* V1068 Sco LP* 16 53 42.4241880264 -43 03 03.488496048   7.71 6.06     M3II/III 34 0
42 HD 152291 Em* 16 54 24.2008363200 -40 39 08.997983136 8.05 9.22 9.27 9.58   B1IIIe 47 0
43 * zet Ara * 16 58 37.2125360584 -55 59 24.499906233   4.701 3.076     K3III 108 0
44 CD-42 11721 Be* 16 59 06.7629322176 -42 42 08.404228224 12.16 12.28 11.00     B0IVe 179 0
45 CD-38 11837 Ae* 17 24 44.7035716704 -38 43 51.463262568 11.05 11.37 10.62 10.46   B1Ve 48 2
46 HD 319896 Or* 17 31 05.8510619376 -35 08 29.264228088   11.54 11.06     B4 29 0
47 HD 320156 Em* 17 37 58.5051513384 -35 23 04.256463300 10.52 10.61 9.78 9.85   B4Ibe 70 0
48 HD 316051 * 17 39 52.1833730208 -27 23 44.144263212   11.18 10.73     B8 10 1
49 IRAS 17367-2722 OH* 17 39 52.42344 -27 23 31.8228           O-rich 14 1
50 * bet Oph PM* 17 43 28.3519097803 +04 34 02.293206489 5.150 3.930 2.750 1.96 1.38 K2IIICN0.5 490 0
51 CD-24 13510 Ae* 17 49 10.1759810016 -24 14 21.276631032 10.12 10.62 9.96 10.01   B4Ve 35 0
52 HD 163376 V* 17 57 47.8025082499 -41 42 58.655766790   6.503 4.863     M0III 54 0
53 IRAS 17575-1647 Or* 18 00 30.3156836064 -16 47 25.864007244 15.67 15.54 14.42     B1 18 0
54 EM* AS 267 LP? 18 01 56.6510540592 -23 41 31.202836008 13.29 12.72 10.75 10.10   OB+ 18 0
55 V* V5098 Sgr Or* 18 02 50.8918954776 -24 16 17.182487568   13.80 13.12 13.28   ~ 8 0
56 HD 315028 * 18 03 22.9225986576 -24 14 25.432195884   10.5 10.2     F0 11 0
57 NGC 6530 180 Y*O 18 03 25.8391456344 -24 21 09.421047828   12.381 12.112     ~ 7 0
58 HD 164865 s*b 18 04 15.2161048560 -24 11 00.078860400 8.62 8.470 7.630 6.74 5.910 B9Ia 68 0
59 CD-24 13830 Ae* 18 04 22.7421765936 -24 22 09.724518840 9.41 10.183 10.016 10.11 9.624 B2Ve 50 0
60 EM* LkHA 115 Ae* 18 04 50.5999226472 -24 25 42.095461620   12.380 11.949   11.198 B7e 39 0
61 * gam02 Sgr PM* 18 05 48.4880988 -30 25 26.723458 4.77 4.00 2.99 2.26 1.75 K0+III 158 0
62 * eta Sgr LP? 18 17 37.6371989461 -36 45 42.084592381 6.37 4.67 3.11 1.55 0.23 M2III 149 0
63 V* EU Ser Ae* 18 19 09.3931184496 -13 50 41.201118528 14.934 14.697 14.158   12.923 Be 35 0
64 * del Sgr * 18 20 59.6428936493 -29 49 41.168145329   4.069 2.668     K2.5IIIaCN0.5 184 0
65 EM* MWC 297 Ae* 18 27 39.5265500160 -03 49 52.133050776 15.57 14.34 12.31 11.34   B1.5Ve 315 0
66 * lam Sgr PM* 18 27 58.2407185 -25 25 18.114589 4.75 3.85 2.81 2.06 1.50 K1IIIb 290 0
67 EM* AS 310 Ae* 18 33 21.1940364288 -04 58 05.976557796   13.58 12.52 12.62   B1e 136 1
68 IRAS 18454+0250 Ae* 18 48 00.6605683128 +02 54 17.127011628 15.03 14.397 12.395     B0.5Ib 30 0
69 * tau Sgr PM* 19 06 56.4031131168 -27 40 13.496293992 5.65 4.51 3.31 2.44 1.85 K1.5IIIb 164 0
70 V* V4419 Sgr LP* 19 32 28.5169569792 -30 52 10.078193892   8.17 6.66     M4III 26 0
71 * b Sgr * 19 56 56.8326894125 -27 10 11.629238513   5.980 4.528     K2.5IIb 69 0
72 * gam Sge PM* 19 58 45.4282303572 +19 29 31.726069716 6.97 5.04 3.47 2.27 1.35 M0-III 276 0
73 * zet Ind * 20 49 28.9625672064 -46 13 36.577128720   6.390 4.882     K5III 46 0
74 * 24 Cap PM* 21 07 07.6681598477 -25 00 21.069488053 8.04 6.11 4.50 3.22 2.24 M1-III 83 0

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