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Annual Report 2011 Max Planck Institute for Astronomy

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IV.3 MatiSSe – Interferometric Imaging in the Mid-Infrared<br />

MatiSSe – the Multi Aperture Mid-Infrared SpectroScopic<br />

Experiment – is one of two second generation instruments<br />

which had been selected by eSo <strong>for</strong> the VLTI at<br />

Paranal. Thus MatiSSe is in a sense the successor of<br />

Midi, the Mid-Infrared Interferometric Instrument, which<br />

has been built at MPIA and which is working on Paranal<br />

since 2003.<br />

Matisse will combine the beams of up to four of the 8 m<br />

UTs (Unit Telescopes) or of up to four of the 1.8 m ATs<br />

(Auxiliary Telescopes) and thus will be able to measure<br />

in “closure phase mode”, i.e. it offers an efficient capability<br />

<strong>for</strong> image reconstruction with a spatial resolution<br />

of up to 7 milliarcsec. The instrument will work at three<br />

wavelength bands: L (3.2 – 3.9 μm), M (4.5 – 5 μm), and<br />

N (8 – 13 μm), where the L and M band observations are<br />

per<strong>for</strong>med simultaneously to the N band.<br />

With the three different spectroscopic resolutions in<br />

the range of R 30 – 1500 it will provide the basis <strong>for</strong><br />

a fundamental analysis of the composition of gas and<br />

dust grains in various astrophysical environments. Key<br />

science programs <strong>for</strong> the ATs cover <strong>for</strong> example the <strong>for</strong>mation<br />

and evolution of planetary systems, the birth of<br />

massive stars as well as the observation of the highcontrast<br />

environment of hot and evolved stars. With the<br />

UTs selected astrophysical programs such as the study<br />

of Active Galactic Nuclei and Extrasolar Planets shall<br />

be possible.<br />

Matisse is developed and built by a collaboration<br />

of the Observatoire de la Cote d’Azure, the MPIA, the<br />

MPI <strong>for</strong> Radio <strong>Astronomy</strong> in Bonn and two institutions<br />

(astron/Dwingeloo and Leiden University) from the<br />

Netherlands. In this consortium MPIA is responsible <strong>for</strong><br />

the cryogenics system, the entire control electronics, and<br />

the instrument control software.<br />

After the successful Preliminary Design Review<br />

(PDR) in December 2010 the year <strong>2011</strong> was dominated<br />

by the preparations <strong>for</strong> the first part of the Final Design<br />

Fig. IV.3.1: Pulse tube cooler PTC 410 from Cryomech. The two<br />

copper plates mark the two stages.<br />

Fig. IV.3.2: Head of Pulse tube cooler with damping system on<br />

test set-up.<br />

Review (FDR) in September <strong>2011</strong>, where the cryogenic system and the design of the optics were reviewed by<br />

eso. For the development of the cryostats several tests<br />

Table. IV.3.1: The characteristic parameters of Matisse.<br />

Number of beams/<br />

telescopes<br />

4 (2 or 3 possible)<br />

Field of view 2 arcsec<br />

Spectral resolution L/M N<br />

Low 20 R 40 20 R 40<br />

Medium 200 R 400 200 R 400<br />

High 750 R 1250<br />

Spatial resolution 0.007 arcsec 0.02 arcsec<br />

had to be per<strong>for</strong>med. By using an auxiliary cryostat we<br />

specified the characteristics of the selected Pulse Tube<br />

Cooler PT410 from Cryomech (Fig. IV.3.1). With using<br />

such a device the induced vibrations are typically factors<br />

of 10–50 lower than with normal Closed Cycle Coolers<br />

of similar cooling power.<br />

Besides the vibrations inside and outside of the test<br />

cryostat we also tested <strong>for</strong> the minimum temperatures to<br />

be reached with this kind of cooler at its first and second<br />

stage and <strong>for</strong> the temperature variations caused by the<br />

cooler when connected to a dummy cold optical bench<br />

(first stage) and a dummy detector (second stage). Here<br />

the copper braid used <strong>for</strong> this connection had to be opti-<br />

Credit: U. Graser<br />

Credit: U. Graser<br />

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