@article{9b2a3da88ae544739ca529a44e52716f,
title = "JWST/MIRI coronagraphic performances as measured on-sky",
abstract = "Context. Characterization of directly imaged exoplanets is one of the most eagerly anticipated science functions of the James Webb Space Telescope. MIRI, the mid-IR instrument, has the capability to provide unique spatially resolved photometric data points in a spectral range never before achieved for such objects. Aims. We aim to present the very first on-sky contrast measurements of the MIRI coronagraphs. In addition to a classical Lyot coronagraph at the longest wavelength, this observing mode implements the concept of the four-quadrant phase mask for the very first time in a space telescope. Methods. We observed single stars together with a series of reference stars to measure raw contrasts as they are delivered on the detector, as well as reference-subtracted contrasts. Results. The MIRI coronagraphs achieve raw contrasts better than 10-3 at the smallest angular separations (within 1) and about 10-5 farther out (beyond 5 6). Subtracting the residual diffracted light left behind the coronagraph has the potential to bring the final contrast down to the background-and detector-limited noise floor at most angular separations (a few times 10-5 at less than 1). Conclusions. The MIRI coronagraphs behave as expected from simulations. In particular, the raw contrasts for all four coronagraphs are fully consistent with the diffractive model. Contrasts obtained by subtracting reference stars also meet expectations and are fully demonstrated for two four-quadrant phase masks (F1065C and F1140C). The worst contrast, measured at F1550C, is very likely due to a variation in the phase aberrations at the primary mirror during the observations, and not an issue with the coronagraph itself. We did not perform reference star subtraction with the Lyot mask at F2300C, but we anticipate that it would bring the contrast down to the noise floor.",
keywords = "Instrumentation: high angular resolution, Planetary systems, Techniques: high angular resolution, Techniques: image processing",
author = "A. Boccaletti and C. Cossou and P. Baudoz and Lagage, {P. O.} and D. Dicken and A. Glasse and Hines, {D. C.} and J. Aguilar and O. Detre and B. Nickson and A. Noriega-Crespo and Andras Gaspar and A. Labiano and C. Stark and D. Rouan and Reess, {J. M.} and Wright, {G. S.} and G. Rieke and {Garcia Marin}, M. and C. Lajoie and J. Girard and M. Perrin and R. Soummer and L. Pueyo",
note = "Funding Information: The work presented is the effort of the entire MIRI team and the enthusiasm within the MIRI partnership is a significant factor in its success. We would like to thank Scott Rhorbach for his invaluable assistance and modelling to resolve the cause of the glowsticks issue, and the JWST and MIRI commissioning teams for their support in the execution of MIRI commissioning. The following National and International Funding Agencies funded and supported the MIRI development: NASA; ESA; Belgian Science Policy Office; Centre Nationale d{\textquoteright}Etudes Spatiales (CNES); Danish National Space Centre; Deutsches Zentrum fur Luft-und Raumfahrt (DLR); Enterprise Ireland; Ministerio De Economi{\'a} y Competividad; Netherlands Research School for Astronomy (NOVA); Netherlands Organisation for Scientific Research (NWO); Science and Technology Facilities Council; Swiss Space Office; Swedish National Space Board; and UK Space Agency. MIRI draws on the scientific and technical expertise of the following organizations: Ames Research Center, USA; Airbus Defence and Space, UK; CEA-Irfu, Saclay, France; Centre Spatial de Li{\`e}ge, Belgium; Consejo Superior de Investigaciones Cientficas, Spain; Carl Zeiss Optronics, Germany; Chalmers University of Technology, Sweden; Danish Space Research Institute, Denmark; Dublin Institute for Advanced Studies, Ireland; European Space Agency, Netherlands; ETCA, Belgium; ETH Zurich, Switzerland; Goddard Space Flight Center, USA; Institute d{\textquoteright}Astrophysique Spatiale, France; Instituto Nacional de T{\'e}cnica Aeroespacial, Spain; Institute for Astronomy, Edinburgh, UK; Jet Propulsion Laboratory, USA; Laboratoire d{\textquoteright}Astrophysique de Marseille (LAM), France; Leiden University, Netherlands; Lockheed Advanced Technology Center (USA); NOVA Opt-IR group at Dwingeloo, Netherlands; Northrop Grumman, USA Max Planck Institut f{\"u}r Astronomie (MPIA), Heidelberg, Germany; Laboratoire d{\textquoteright}Etudes Spatiales et d{\textquoteright}Instrumentation en Astrophysique (LESIA), France; Paul Scherrer Institut, Switzerland; Raytheon Vision Systems, USA; RUAG Aerospace, Switzerland; Rutherford Appleton Laboratory (RAL Space), UK Space Telescope Science Institute, USA; Toegepast-Natuurwetenschappelijk Onderzoek (TNOTPD), Netherlands; UK Astronomy Technology Centre UK; University College London, UK; University of Amsterdam, Netherlands University of Arizona, USA; University of Bern, Switzerland; University of Cardiff, UK; University of Cologne, Germany; University of Ghent; University of Groningen, Netherlands; University of Leicester, UK; University of Leuven Belgium; University of Stockholm, Sweden; Utah State University, USA. A portion of this work was carried out at the Jet Propulsion Laboratory, California Institute of Technology, under a contract with the National Aeronautics and Space Administration. Publisher Copyright: {\textcopyright} 2022 EDP Sciences. All rights reserved.",
year = "2022",
month = nov,
day = "1",
doi = "10.1051/0004-6361/202244578",
language = "English (US)",
volume = "667",
journal = "Astronomy and Astrophysics",
issn = "0004-6361",
publisher = "EDP Sciences",
}