2018A&A...618A.143N


Query : 2018A&A...618A.143N

2018A&A...618A.143N - Astronomy and Astrophysics, volume 618A, 143-143 (2018/1-0)

PACS and SPIRE range spectroscopy of cool, evolved stars.

NICOLAES D., GROENEWEGEN M.A.T., ROYER P., LOMBAERT R., DANILOVICH T. and DECIN L.

Abstract (from CDS):

Context. At the end of their lives AGB stars are prolific producers of dust and gas. The details of this mass-loss process are still not understood very well. Herschel PACS and SPIRE spectra which cover the wavelength range from ∼55 to 670µm almost continuously, offer a unique way of investigating properties of AGB stars in general and the mass-loss process in particular as this is the wavelength region where dust emission is prominent and molecules have many emission lines.
Aims. We present the community with a catalogue of AGB stars and red supergiants (RSGs) with PACS and/or SPIRE spectra reduced according to the current state of the art.
Methods. The Herschel interactive processing environment (HIPE) software with the latest calibration is used to process the available PACS and SPIRE spectra of 40 evolved stars. The SPIRE spectra of some objects close to the Galactic plane require special treatment because of the weaker fluxes in combination with the strong and complex background emission at those wavelengths. The spectra are convolved with the response curves of the PACS and SPIRE bolometers and compared to the fluxes measured in imaging data of these sources. Custom software is used to identify lines in the spectra, and to determine the central wavelengths and line intensities. Standard molecular line databases are used to associate the observed lines. Because of the limited spectral resolution of the PACS and SPIRE spectrometers (∼1500), several known lines are typically potential counterparts to any observed line. To help identifications in follow-up studies the relative contributions in line intensity of the potential counterpart lines are listed for three characteristic temperatures based on local thermodynamic equilibrium (LTE) calculations and assuming optically thin emission.
Results. The following data products are released: the reduced spectra, the lines that are measured in the spectra with wavelength, intensity, potential identifications, and the continuum spectra, i.e. the full spectra with all identified lines removed. As simple examples of how this data can be used in future studies we have fitted the continuum spectra with three power laws (two wavelength regimes covering PACS, and one covering SPIRE) and find that the few OH/IR stars seem to have significantly steeper slopes than the other oxygen- and carbon-rich objects in the sample, possibly related to a recent increase in mass-loss rate. As another example we constructed rotational diagrams for CO (and HCN for the carbon stars) and fitted a two-component model to derive rotational temperatures.

Abstract Copyright: © ESO 2018

Journal keyword(s): stars: AGB and post-AGB - stars: mass-loss - infrared: stars

VizieR on-line data: <Available at CDS (J/A+A/618/A143): table2.dat splist.dat lines.dat sp/*>

Simbad objects: 57

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Number of rows : 57
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 V* AQ And C* 00 27 31.6830716856 +35 35 14.495266104   11.3 9.90     C-N5+ 113 0
2 IRC +10011 OH* 01 06 25.9879717848 +12 35 52.896392052   20.7   18.26 14.01 M8 420 0
3 V* R Scl C* 01 26 58.0939182720 -32 32 35.439234828 17.26 9.59 5.72 3.69 2.30 C-N5+ 332 0
4 OH 127.8-00.0 OH* 01 33 51.21048 +62 26 53.2032           O-rich 181 0
5 * omi Cet Mi* 02 19 20.79210 -02 58 39.4956   7.63 6.53 5.03   M5-9IIIe+DA 1528 0
6 V* R For C* 02 29 15.3077617632 -26 05 55.646585700   12.94 7.50 8.01   C4,3e 196 0
7 V* IK Tau OH* 03 53 28.8924743304 +11 24 21.895183368 16.99 14.463 16.171 14.101   M7-11 638 0
8 V* R Dor AB* 04 36 45.59127 -62 04 37.7974 7.84 6.98 5.40 2.71 -0.44 M8III:e 346 0
9 V* TX Cam Mi* 05 00 51.1627935408 +56 10 54.041462220       14.02   M9-9.5 350 0
10 * alf Ori s*r 05 55 10.30536 +07 24 25.4304 4.38 2.27 0.42 -1.17 -2.45 M1-M2Ia-Iab 1671 0
11 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1104 0
12 V* II Pup Mi* 08 03 25.7545924248 -27 55 26.036199552       11.51   M8-M9 12 0
13 IRAS 09425-6040 C* 09 44 01.6707336168 -60 54 25.639144812     12.6 11.81   C 60 0
14 V* R LMi OH* 09 45 34.2840467232 +34 30 42.809054724   9.442 8.443 9.024   M6.5-9e 325 0
15 IRC +10216 C* 09 47 57.40632 +13 16 43.5648           C9,5e 2343 0
16 V* RW LMi C* 10 16 02.2777043904 +30 34 19.045098516       15.27   C4,3e 396 0
17 V* U Ant C* 10 35 12.8510147472 -39 33 45.324020448 15.32 8.22 5.38 3.18 1.86 C-N3 153 0
18 V* V Hya C* 10 51 37.2615873024 -21 15 00.333928044   12.23 6.80 7.42   C-N:6 366 0
19 V* W Hya Mi* 13 49 02.0018313132 -28 22 03.532006894   8.97 7.70     M7.5-9e 640 0
20 WOS 48 C* 15 23 05.0730770544 -51 25 58.762691652   17.85 16.66 14.51 10.18 C 134 1
21 V* ST Her S* 15 50 46.6232210160 +48 28 58.850853780   9.09 7.75     M6S-M7SIII: 164 0
22 V* X Her AB* 16 02 39.1730141112 +47 14 25.265335956   7.64 6.58     M6III 237 0
23 * g Her AB* 16 28 38.5495839988 +41 52 54.044914927 7.70 6.53 5.01 2.49 0.26 M6-III 377 0
24 V* V438 Oph LP* 17 14 39.7815252576 +11 04 09.970384872   10.53 9.29     M8 54 0
25 RAFGL 5379 OH* 17 44 24.0074369832 -31 55 35.414175828           O-rich 88 0
26 OH 021.5+00.5 OH* 18 28 30.93720 -09 58 14.3184           O-rich 93 0
27 OH 026.5+00.6 OH* 18 37 32.50920 -05 23 59.1936           O-rich 301 1
28 V* KX Her Mi* 18 43 13.8494035944 +12 23 51.095124204     12.01     M8e 16 0
29 OH 030.7+00.4 OH* 18 45 52.39728 -01 46 42.4776           O-rich 69 1
30 OH 030.1-00.7 OH* 18 48 41.98728 -02 50 29.5080           O-rich 100 0
31 V* S Sct C* 18 50 20.0367791256 -07 54 27.429169356 13.93 9.89 6.80     C-N5 209 0
32 OH 032.0-00.5 OH* 18 51 26.25600 -01 03 52.3620           O-rich 68 0
33 OH 032.8-00.3 OH* 18 52 22.25472 -00 14 11.8428           O-rich 123 0
34 V* R Aql OH* 19 06 22.2510922392 +08 13 48.012661776 8.06 7.69 6.09     M6.5-9e 564 2
35 OH 042.3-00.1 OH* 19 09 08.32632 +08 16 33.6504           O-rich 87 0
36 V* W Aql S* 19 15 23.3572741560 -07 02 50.333886492   12.72 10.14 10.21   S6/6e 231 0
37 V* KW Aql Ir* 19 32 06.0909424920 +13 00 49.670889300           ~ 3 0
38 V* AQ Sgr C* 19 34 18.9945475487 -16 22 27.048908541 13.85 9.48 6.70     C-N5 119 0
39 V* TT Cyg C* 19 40 57.0158460384 +32 37 05.756696400   10.43 10.20     C-N5- 201 0
40 V* GY Aql Mi* 19 50 06.3301987896 -07 36 52.465065516   12.54 11.22     M8 118 0
41 * chi Cyg S* 19 50 33.9213430345 +32 54 50.575531294 7.02 6.06 4.24 1.81 -0.01 S6-9/1-2e 693 0
42 V* RR Aql Mi* 19 57 36.0616870728 -01 53 11.339520360     7.80 7.45   M7.5e 294 2
43 V* V1943 Sgr AB* 20 06 55.2441583872 -27 13 29.766501516   9.25 8.04     M7/8III 78 0
44 RAFGL 2513 C* 20 09 14.2555901784 +31 25 44.830603344           C-rich 49 0
45 IRC -10529 OH* 20 10 27.8731455576 -06 16 13.758742596         15.49 M: 141 0
46 V* KV Cyg EB* 20 15 38.1351110712 +36 47 36.786624216   11.78 11.23     B1V 33 0
47 V* RT Cap C* 20 17 06.5287791168 -21 19 04.466353512   12.92 8.90     C6,4 128 0
48 V* T Mic AB* 20 27 55.1897976672 -28 15 39.797839548   8.33 6.74     M7/8III 95 0
49 V* V Cyg C* 20 41 18.2676815496 +48 08 28.810980420   14.05 7.70 6.67   C7,4eJ 306 0
50 NML Cyg s*r 20 46 25.5392819088 +40 06 59.464289232           M7/8 508 0
51 V* T Cep Mi* 21 09 31.7834766408 +68 29 27.231070884 9.15 8.82 7.33     M6-9e 381 0
52 V* EP Aqr AB* 21 46 31.8494911920 -02 12 45.928582560   7.93 6.78     M7-III: 241 0
53 * pi.01 Gru S* 22 22 44.2083897000 -45 56 52.791160956 10.52 8.62 6.55 3.19 0.52 S5,7: 193 0
54 RAFGL 3068 C* 23 19 12.60744 +17 11 33.1332           C 270 0
55 IRC +40540 C* 23 34 27.5185864392 +43 33 01.323347256     15.12     C8,3.5eJ 179 0
56 V* R Aqr Sy* 23 43 49.4634303216 -15 17 04.176349872   8.823 7.683 9.37   M6.5-8.5e 784 0
57 V* R Cas Mi* 23 58 24.8682785040 +51 23 19.713029388 6.71 6.63 4.80     M6.5-9e 702 0

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