2018A&A...613A..40K


Query : 2018A&A...613A..40K

2018A&A...613A..40K - Astronomy and Astrophysics, volume 613A, 40-40 (2018/5-1)

Herschel-PACS photometry of faint stars for sensitivity performance assessment and establishment of faint FIR primary photometric standards.

KLAAS U., BALOG Z., NIELBOCK M., MULLER T.G., LINZ H. and KISS C.

Abstract (from CDS):

Aims. Our aims are to determine flux densities and their photometric accuracy for a set of seventeen stars that range in flux from intermediately bright (≤2.5Jy) to faint (≥5mJy) in the far-infrared (FIR). We also aim to derive signal-to-noise dependence with flux and time, and compare the results with predictions from the Herschel exposure-time calculation tool. Methods. We obtain aperture photometry from Herschel-PACS high-pass-filtered scan maps and chop/nod observations of the faint stars. The issues of detection limits and sky confusion noise are addressed by comparison of the field-of-view at different wavelengths, by multi-aperture photometry, by special processing of the maps to preserve extended emission, and with the help of large-scale absolute sky brightness maps from AKARI. This photometry is compared with flux-density predictions based on photospheric models for these stars. We obtain a robust noise estimate by fitting the flux distribution per map pixel histogram for the area around the stars, scaling it for the applied aperture size and correcting for noise correlation. Results. For 15 stars we obtain reliable photometry in at least one PACS filter, and for 11 stars we achieve this in all three PACS filters (70, 100, 160µm). Faintest fluxes, for which the photometry still has good quality, are about 10-20mJy with scan map photometry. The photometry of seven stars is consistent with models or flux predictions for pure photospheric emission, making them good primary standard candidates. Two stars exhibit source-intrinsic far-infrared excess: β Gem (Pollux), being the host star of a confirmed Jupiter-size exoplanet, due to emission of an associated dust disk, and η Dra due to dust emission in a binary system with a K1 dwarf. The investigation of the 160µm sky background and environment of four sources reveals significant sky confusion prohibiting the determination of an accurate stellar flux at this wavelength. As a good model approximation, for nine stars we obtain scaling factors of the continuum flux models of four PACS fiducial standards with the same or quite similar spectral type. We can verify a linear dependence of signal-to-noise ratio (S/N) with flux and with square root of time over significant ranges. At 160µm the latter relation is, however, affected by confusion noise. Conclusions. The PACS faint star sample has allowed a comprehensive sensitivity assessment of the PACS photometer. Accurate photometry allows us to establish a set of five FIR primary standard candidates, namely α Ari, ε Lep, ω Cap, HD 41047 and 42 Dra, which are 2-20 times fainter than the faintest PACS fiducial standard (γ Dra) with absolute accuracy of <6%. For three of these primary standard candidates, essential stellar parameters are known, meaning that a dedicated flux model code may be run.

Abstract Copyright: © ESO 2018

Journal keyword(s): space vehicles: instruments - methods: data analysis - techniques: photometric - infrared: stars - stars: atmospheres - radiation mechanisms: thermal

VizieR on-line data: <Available at CDS (J/A+A/613/A40): stars.dat tablea3-5.dat tableb1-3.dat>

Simbad objects: 23

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Number of rows : 23
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 * alf Ari b Pl 02 07 10.40570 +23 27 44.7032           ~ 11 1
2 * alf Ari PM* 02 07 10.40570 +23 27 44.7032 4.29 3.17 2.01 1.15 0.54 K2-IIIbCa-1 622 2
3 * del Hyi PM* 02 21 44.9423652192 -68 39 33.906922488 4.17 4.12 4.09 4.05 4.04 A2V 111 0
4 * eps Lep PM* 05 05 27.6644072506 -22 22 15.724153311 6.41 4.64 3.18 2.08 1.27 K4III 157 0
5 HD 39608 * 05 49 36.4581598776 -60 40 34.657139244   8.91 7.35     K5III 18 0
6 HD 41047 * 06 01 16.2976481208 -33 54 42.608011716   7.102 5.524     K5III 36 0
7 * bet Gem PM* 07 45 18.94987 +28 01 34.3160 3.00 2.14 1.14 0.39 -0.11 K0IIIb 1101 2
8 * bet Gem b Pl 07 45 18.94987 +28 01 34.3160           ~ 33 1
9 * alf Vir bC* 13 25 11.57937 -11 09 40.7501 -0.20 0.74 0.97 1.06 1.30 B1V 855 2
10 HD 138265 * 15 27 51.4237531200 +60 40 12.796947012 9.030 7.350 5.900     K5III 40 0
11 * tet UMi V* 15 31 24.9136103328 +77 20 57.695859924   6.535 4.982     K5-IIICN0.5 117 0
12 * eta Dra PM* 16 23 59.4863284800 +61 30 51.155139060 4.35 3.65 2.74 2.12 1.66 G8-IIIab 298 0
13 HD 152222 * 16 47 04.6184032608 +67 16 00.529666644   8.55 7.03     K2III 15 0
14 NAME Draco Nebula RNe 16 52 +61.0           ~ 55 0
15 * e Her PM* 17 17 40.2531980520 +37 17 29.422635288 4.67 4.70 4.65 4.56 4.56 A2V 95 0
16 HD 159330 * 17 30 43.5747719616 +57 52 36.566848992 9.210 7.640 6.210     K2III 37 0
17 HD 168009 PM* 18 15 32.4633956040 +45 12 33.540706764   6.931 6.298     G1V 213 0
18 * 42 Dra PM* 18 25 59.1369601368 +65 33 48.531343788   6.005 4.823     K1.5IIIFe-1 167 1
19 * 42 Dra b Pl 18 25 59.1369601368 +65 33 48.531343788           ~ 21 1
20 * del Dra PM* 19 12 33.3013729052 +67 39 41.539165396 4.85 4.07 3.07 2.37 1.86 G9III 280 0
21 2MASS J19183293+4933528 G 19 18 32.9403438528 +49 33 52.836392016           ~ 5 0
22 HD 181597 * 19 18 37.8718847472 +49 34 10.037944416   7.442 6.317     K1III 59 0
23 * ome Cap V* 20 51 49.2905373888 -26 55 08.885443656 7.66 5.75 4.12 2.87 1.93 M0IIIBa0.5 100 0

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