2018A&A...619A...9S


Query : 2018A&A...619A...9S

2018A&A...619A...9S - Astronomy and Astrophysics, volume 619A9-9 (2018/11-1)

SPHERE/ZIMPOL high resolution polarimetric imager. I. System overview, PSF parameters, coronagraphy, and polarimetry.

SCHMID H.M., BAZZON A., ROELFSEMA R., MOUILLET D., MILLI J., MENARD F., GISLER D., HUNZIKER S., PRAGT J., DOMINIK C., BOCCALETTI A., GINSKI C., ABE L., ANTONIUCCI S., AVENHAUS H., BARUFFOLO A., BAUDOZ P., BEUZIT J.L., CARBILLET M., CHAUVIN G., CLAUDI R., COSTILLE A., DABAN J.-B., DE HAAN M., DESIDERA S., DOHLEN K., DOWNING M., ELSWIJK E., ENGLER N., FELDT M., FUSCO T., GIRARD J.H., GRATTON R., HANENBURG H., HENNING T., HUBIN N., JOOS F., KASPER M., KELLER C.U., LANGLOIS M., LAGADEC E., MARTINEZ P., MULDER E., PAVLOV A., PODIO L., PUGET P., QUANZ S.P., RIGAL F., SALASNICH B., SAUVAGE J.-F., SCHUIL M., SIEBENMORGEN R., SISSA E., SNIK F., SUAREZ M., THALMANN C., TURATTO M., UDRY S., VAN DUIN A., VAN HOLSTEIN R.G., VIGAN A. and WILDI F.

Abstract (from CDS):


Context. The SPHERE "planet finder" is an extreme adaptive optics (AO) instrument for high resolution and high contrast observations at the Very Large Telescope (VLT). We describe the Zurich Imaging Polarimeter (ZIMPOL), the visual focal plane subsystem of SPHERE, which pushes the limits of current AO systems to shorter wavelengths, higher spatial resolution, and much improved polarimetric performance.
Aims. We present a detailed characterization of SPHERE/ZIMPOL which should be useful for an optimal planning of observations and for improving the data reduction and calibration. We aim to provide new benchmarks for the performance of high contrast instruments, in particular for polarimetric differential imaging.
Methods. We have analyzed SPHERE/ZIMPOL point spread functions (PSFs) and measure the normalized peak surface brightness, the encircled energy, and the full width half maximum (FWHM) for different wavelengths, atmospheric conditions, star brightness, and instrument modes. Coronagraphic images are described and the peak flux attenuation and the off-axis flux transmission are determined. Simultaneous images of the coronagraphic focal plane and the pupil plane are analyzed and the suppression of the diffraction rings by the pupil stop is investigated. We compared the performance at small separation for different coronagraphs with tests for the binary α Hyi with a separation of 92mas and a contrast of Δm~=6m. For the polarimetric mode we made the instrument calibrations using zero polarization and high polarization standard stars and here we give a recipe for the absolute calibration of polarimetric data. The data show small (<1mas) but disturbing differential polarimetric beam shifts, which can be explained as Goos-Hahnchen shifts from the inclined mirrors, and we discuss how to correct this effect. The polarimetric sensitivity is investigated with non-coronagraphic and deep, coronagraphic observations of the dust scattering around the symbiotic Mira variable R Aqr.
Results. SPHERE/ZIMPOL reaches routinely an angular resolution (FWHM) of 22-28mas, and a normalized peak surface brightness of SB0-mstar~–6.5mag/arcsec2 for the V-, R- and I-band. The AO performance is worse for mediocre ≥1.0'' seeing conditions, faint stars mR> 9m, or in the presence of the "low wind" effect (telescope seeing). The coronagraphs are effective in attenuating the PSF peak by factors of > 100, and the suppression of the diffracted light improves the contrast performance by a factor of approximately two in the separation range 0.06''-0.20''. The polarimetric sensitivity is Δp<0.01% and the polarization zero point can be calibrated to better than Δp~=0.1%. The contrast limits for differential polarimetric imaging for the 400 s I-band data of R Aqr at a separation of ρ=0.86'' are for the surface brightness contrast SBpol(ρ)-mstar~=8mag/arcsec2 and for the point source contrast mpol( ρ)-mstar~=15m and much lower limits are achievable with deeper observations.
Conclusions. SPHERE/ZIMPOL achieves imaging performances in the visual range with unprecedented characteristics, in particular very high spatial resolution and very high polarimetric contrast. This instrument opens up many new research opportunities for the detailed investigation of circumstellar dust, in scattered and therefore polarized light, for the investigation of faint companions, and for the mapping of circumstellar Hα emission.

Abstract Copyright: © ESO 2018

Journal keyword(s): instrumentation: adaptive optics - instrumentation: high angular resolution - instrumentation: polarimeters - instrumentation: detectors - planetary systems - circumstellar matter

Simbad objects: 27

goto Full paper

goto View the references in ADS

Number of rows : 27
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 * zet Tuc PM* 00 20 04.2586334956 -64 52 29.257190108 4.82 4.80 4.23 3.73 3.40 F9.5V 415 0
2 2MASS J00235692-7205325 RG* 00 23 56.9331774048 -72 05 32.561039436   13.398 11.775   9.858 ~ 12 0
3 2MASS J00235767-7205296 pA* 00 23 57.5724564864 -72 05 29.439254436     11.368   9.916 ~ 9 0
4 Cl* NGC 104 R 1 * 00 23 58.1989264392 -72 05 30.394828464   13.593 10.73   10.43 B8III: 20 1
5 NGC 104 GlC 00 24 05.359 -72 04 53.20     4.09     ~ 4158 0
6 * alf Eri Be* 01 37 42.84548 -57 14 12.3101 -0.36 0.30 0.46 0.49 0.60 B6Vpe 495 1
7 * alf Hyi PM* 01 58 46.1385834212 -61 34 11.359751511 3.33 3.13 2.84 2.55 2.39 F0IV 225 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 376 0
9 V* Z CMa Ae* 07 03 43.1599411656 -11 33 06.209065836 10.51 9.99 8.80     B5/8eq+F5/7 601 3
10 HD 79186 s*b 09 11 04.3980934536 -44 52 04.448548776 4.65 5.22 5.00 4.71 4.49 B5Ia 149 0
11 * alf Hya * 09 27 35.24270 -08 39 30.9583 5.14 3.42 1.97 0.93 0.16 K3IIIa 455 1
12 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
13 HD 98143 * 11 15 16.9024812240 -77 31 06.120737796   8.12 7.61     B8III 42 0
14 HD 100457 * 11 33 37.8193152216 -06 32 13.015333392   8.78 7.67     K0III 14 0
15 HD 111613 sg* 12 51 17.9760267672 -60 19 47.240368104 6.00 6.10 5.72 5.32 5.03 B9.5Iab 123 0
16 * alf Cen B PM* 14 39 35.06311 -60 50 15.0992 2.89 2.21 1.33     K1V 1092 2
17 * mu. Vir PM* 14 43 03.6239867612 -05 39 29.524956308 4.25 4.26 3.88 3.48 3.26 F2V 239 0
18 HD 135344B Or* 15 15 48.4460065200 -37 09 16.024369824   9.21 8.708     F8V 548 0
19 HD 142527 Ae* 15 56 41.8882637904 -42 19 23.248281828   9.04 8.34     F6III 741 1
20 HD 146897 Ro* 16 19 29.2418869104 -21 24 13.272759216   9.58 9.11     F2/3V 115 0
21 * omi Sco V* 16 20 38.1737722092 -24 10 09.495477665 5.99 5.40 4.57 3.69 2.93 A5II 269 0
22 HD 154445 * 17 05 32.2587926880 -00 53 31.437713328 5.10 5.73 5.61 5.39 5.34 B1V 276 0
23 * 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
24 V* PZ Tel BY* 18 53 05.8735056984 -50 10 49.897437168   9.22 8.342   7.464 G9IV 364 0
25 HD 183143 s*b 19 27 26.5636061496 +18 17 45.193019136 8.25 8.08 6.86 5.74 4.79 B7Ia+ 464 0
26 HD 218396 El* 23 07 28.7157209544 +21 08 03.310767492   6.21 5.953     F0+VkA5mA5 1285 0
27 V* R Aqr Sy* 23 43 49.4634303216 -15 17 04.176349872   8.823 7.683 9.37   M6.5-8.5e 823 0

To bookmark this query, right click on this link: simbad:objects in 2018A&A...619A...9S and select 'bookmark this link' or equivalent in the popup menu