4.3 Article

The Imaging Magnetograph eXperiment (IMaX) for the Sunrise Balloon-Borne Solar Observatory

Journal

SOLAR PHYSICS
Volume 268, Issue 1, Pages 57-102

Publisher

SPRINGER
DOI: 10.1007/s11207-010-9644-y

Keywords

Instrumentation and data management; Integrated Sun observations polarization; Magnetic fields; Velocity fields

Funding

  1. Bundesministerium fur Wirtschaft und Technologie through Deutsches Zentrum fur Luft- und Raumfahrt e.V. (DLR) [50 OU 0401]
  2. Max Planck Society (MPG)
  3. Spanish MICINN [ESP2006-13030-C06, AYA2009-14105-C06]
  4. National Science Foundation
  5. NASA [NNX08AH38G]
  6. Science and Technology Facilities Council [PP/E001173/1] Funding Source: researchfish
  7. STFC [PP/E001173/1] Funding Source: UKRI

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The Imaging Magnetograph eXperiment (IMaX) is a spectropolarimeter built by four institutions in Spain that flew on board the Sunrise balloon-borne solar observatory in June 2009 for almost six days over the Arctic Circle. As a polarimeter, IMaX uses fast polarization modulation (based on the use of two liquid crystal retarders), real-time image accumulation, and dual-beam polarimetry to reach polarization sensitivities of 0.1%. As a spectrograph, the instrument uses a LiNbO(3) etalon in double pass and a narrow band pre-filter to achieve a spectral resolution of 85 m. IMaX uses the high-Zeeman-sensitive line of Fe i at 5250.2 and observes all four Stokes parameters at various points inside the spectral line. This allows vector magnetograms, Dopplergrams, and intensity frames to be produced that, after reconstruction, reach spatial resolutions in the 0.15 -aEuro parts per thousand 0.18 arcsec range over a 50x50 arcsec field of view. Time cadences vary between 10 and 33 s, although the shortest one only includes longitudinal polarimetry. The spectral line is sampled in various ways depending on the applied observing mode, from just two points inside the line to 11 of them. All observing modes include one extra wavelength point in the nearby continuum. Gauss equivalent sensitivities are 4 G for longitudinal fields and 80 G for transverse fields per wavelength sample. The line-of-sight velocities are estimated with statistical errors of the order of 5 -aEuro parts per thousand 40 m s(-1). The design, calibration, and integration phases of the instrument, together with the implemented data reduction scheme, are described in some detail.

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