Max Planck Institute for Astronomy - Annual Report 2005
Max Planck Institute for Astronomy - Annual Report 2005
Max Planck Institute for Astronomy - Annual Report 2005
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multiple<br />
sodium LGS<br />
HL<br />
ELT<br />
An ELT Instrument <strong>for</strong> the Mid-Infrared Range<br />
LGS<br />
focus<br />
In collaboration with the University of Leiden, ASTRON<br />
(Dwingeloo) and ESO the T-OWL study was started at the<br />
beginning of <strong>2005</strong> on behalf of ESO to investigate possible<br />
concepts <strong>for</strong> a mid-IR instrument on a future 100 m<br />
telescope. At first, a list of astrophysical research projects<br />
<strong>for</strong> the wavelength range from 3.5 to 25 �m at the ELT<br />
was compiled from which the necessary specifications of<br />
such a mid-infrared instrument were derived and a design<br />
concept was developed. The first step was to simulate the<br />
atmospheric boundary conditions <strong>for</strong> different possible<br />
sites. Transmission and emission of the atmosphere,<br />
which limits the sensitivity of ground-based observations<br />
in the mid-infrared wavelength range, were calculated<br />
<strong>for</strong> spectral resolutions up to R � 50 000. Comparison<br />
of the derived sensitivity of a mid-infrared instrument<br />
at a 100 m telescope with other instruments <strong>for</strong> the midinfrared<br />
range – in particular with MIRI (JWST) – shows<br />
that a ground-based ELT is on par with satellite-based<br />
instruments in the mid-infrared range (Fig. IV.2.3). In<br />
some fields it is even vastly superior if one concentrates<br />
on extreme angular and/or high spectral resolution. An<br />
instrument <strong>for</strong> the mid-infrared at the ELT has to work<br />
diffraction limited (adaptive optics) and to provide optional<br />
high-resolution spectroscopy, preferably in combination<br />
with imaging optics.<br />
Specific technical issues and problems were investigated<br />
in the T-OWL study: pupil and field rotation, atmospheric<br />
dispersion and its possible correction, chopping,<br />
coronagraphy, polarimetry, detector selection, data flow,<br />
observing modes and so on. No severe incompatibilities<br />
with the OWL design were found.<br />
As planned, the study was completed with a report in<br />
September <strong>2005</strong>. Since then, the EC-funded study MIDIR<br />
has begun to continue the T-OWL study and, in particular,<br />
to study the consequences of a reduction of the primary<br />
mirror diameter from 100 m to between 30 and 60 m on<br />
the sensitivity and thus the feasibility of scientific projects<br />
and the instrumentation concept.<br />
GL<br />
infinity<br />
focus<br />
telecentric<br />
focus<br />
IV.2 Novel Concepts <strong>for</strong> an Extremely Large Telescope 97<br />
HL GL<br />
DM DM<br />
WFC HL<br />
WFC GL<br />
A Near-Infrared Camera <strong>for</strong> the ELT<br />
multiple<br />
masks relay lens CCD<br />
multiple<br />
rods<br />
HL<br />
CCD<br />
GL<br />
Fig IV.2.2: PIGS sensor as used in a Multi-Conjugated Adaptive<br />
Optics system based on the Layer Oriented approach.<br />
With colleagues at Arcetri, researchers at the MPIA<br />
also conducted a preliminary study <strong>for</strong> a near-IR camera<br />
on an ELT, called ONIRICA. An exploration of science<br />
cases yielded that a partial image correction (to 0�.1) over<br />
a wide field of view may be just as important as a full<br />
atmospheric correction over a smaller field.<br />
10 10<br />
10 9<br />
10 8<br />
10 7<br />
10 6<br />
10 5<br />
10 4<br />
10 3<br />
(Wolfgang Brandner, Wolfgang Gässler,<br />
Roland Gredel, Tom Herbst,<br />
Thomas Henning, Hans-Walter Rix,<br />
Stefan Kellner, Rainer Lenzen, Eva Meyer)<br />
Fig. IV.2.3: Comparison of the limiting magnitudes <strong>for</strong> one-hour<br />
exposure time (5 sigma) and the resolving power of various instruments<br />
<strong>for</strong> the mid-infrared through sub-millimeter range.<br />
detectivity 1 h 5 � [Jy Hz]<br />
point source detectivity<br />
SPITZER<br />
HERSCHEL<br />
JWST<br />
SAFIR<br />
ALMA<br />
30 m ELT<br />
1 10 100 1000<br />
wavelength [�m]