The Messenger No. 145 - September 2011 - European Southern Observatory

Page created by Fernando Knight
 
CONTINUE READING
The Messenger No. 145 - September 2011 - European Southern Observatory
Studies for a massively-multiplexed spectrograph
Spectroscopy of Pluto and Triton
VISTA survey of Orion Belt region
VLT FLAMES Tarantula Survey
                                                                              The Messenger
                                                   No. 145 – September 2011
The Messenger No. 145 - September 2011 - European Southern Observatory
Telescopes and Instrumentation

TRAPPIST: TRAnsiting Planets and PlanetesImals Small
Telescope

Emmanuël Jehin1

                                                                                                                                                 E. Jehin/ESO
Michaël Gillon1
Didier Queloz 2
Pierre Magain1
Jean Manfroid1
Virginie Chantry1
Monica Lendl2
Damien Hutsemékers1
Stephane Udry2

1
  Institut d’Astrophysique de l’Université
  de Liège, Belgium
2
   Observatoire de l’Université de Genève,
  Switzerland

TRAPPIST is a 60-cm robotic telescope
that was installed in April 2010 at the
ESO La Silla Observatory. The project is
led by the Astrophysics and Image Pro-
cessing group (AIP) at the Department of        Figure 1. The TRAPPIST telescope in its 5-metre   time is obviously needed to monitor the
                                                enclosure at the La Silla Observatory, Chile.
Astrophysics, Geophysics and Ocean-                                                               activity of several comets with a fre­
ography (AGO) of the University of Liège,                                                         quency of a few times per week. Some
in close collaboration with the Geneva          TRAPPIST is an original project using a           comets are known, but others appear
Observatory, and has been funded by             single telescope that has been built and          serendipitously. For the latter, telescope
the Belgian Fund for Scientific Research        optimised to allow the study of those two         availability is crucial if we want to react
(F.R.S.-FNRS) and the Swiss National            aspects of the growing field of astrobiol­        rapidly to observe those targets at the
Science Foundation (SNF). It is devoted         ogy. It provides high quality photometric         appropriate moment and for several hours
to the detection and characterisation of        data of exoplanet transits and allows             or nights in a row; this strategy can pro­
exoplanets and to the study of comets           the gaseous emissions of bright comets            vide unique datasets impossible to obtain
and other small bodies in the Solar Sys-        to be monitored regularly. The project            otherwise.
tem. We describe here the goals of the          is centred on three main goals: (1) the
project and the hardware and present            detection of the transits of new exoplan­
some results obtained during the first six      ets; (2) the characterisation of known            Telescope and instrumentation
months of operation.                            transiting planets, in particular the pre­
                                                cise determination of their size; and (3)         For low cost operations and high flexibil­
                                                the survey of the chemical composition of         ity, TRAPPIST (see Figure 1) had to be
The science case                                bright comets and the evolution of their          a robotic observatory. The observation
                                                activity during their orbit.                      programme, including the calibration
The hundreds of exoplanets known today                                                            plan, is prepared in advance and submit­
allow us to place our own Solar System                                                            ted daily to a specific software installed
in the broad context of our own Galaxy.         A dedicated robotic telescope                     on the computer controlling the obser­
In particular, the subset of known exo­                                                           vatory. This computer controls all the
planets that transit their parent stars are     The basic project concept is a robotic tel­       technical aspects of the obser­vations:
key objects for our understanding of            escope fully dedicated to high precision          dome control, pointing, focusing, image
the formation, evolution and properties of      exoplanet and comet time-series pho­              acquisition, astrometry and software
planetary systems. The objects of the           tometry, providing the large amount of            guiding, calibrations, data storage... It is
Solar System are, and will remain, exqui­       observing time requested for those                in sleep mode during daytime and wakes
site guides for helping us understand           research projects. Exoplanet transits typi­       up one hour before sunset, opening the
the mechanisms of planetary formation           cally last several hours, up to a full night.     dome and starting to cool the CCD. This
and evolution. Comets, in particular, are       There are now many known transiting               process is made possible thanks to a
most probably remnants of the initial           planets, and many more candidates found           ­collection of computer programs working
population of planetesimals of the outer        by transit surveys which need to be                together and interacting with the tele­
part of the protoplanetary disc. Therefore      ­confirmed and characterised. Moreover             scope, dome, CCD camera, filter wheels
the study of their physical and chemical         these targets need to be observed at              and meteorological station. Such a
properties allows the conditions that            very specific times, during eclipses, put­        ­complete and rapid integration, using
prevailed during the formation of the four       ting even more constraints on telescope            mostly off-the-shelf solutions, would have
giant planets to be probed.                      availability. Similarly a lot of observing         been impossible a few years ago and

2          The Messenger 145 – September 2011
The Messenger No. 145 - September 2011 - European Southern Observatory
WASP—43b TRAPPIST I+z

                                                        1

                                                     0.99

                                              Flux
                                                     0.98

                                                     0.97
                                                                                                                               σ = 0.0003

                                                     0.96
                                                               – 0.04       – 0.02              0                0.02                 0.04
                                                                                            dT (days)

                                              aluminium components, it weighs only           Figure 3. TRAPPIST I + z transit photometry of the
                                                                                             planet WASP-43b, period-folded and binned per two
                                              65 kg and was allied to a compact Ger­
                                                                                             minute intervals, with the best-fit transit model
                                              man equatorial mount, the New Technol­         superimposed. The residuals of the fit, shifted along
                                              ogy Mount NTM-500, from the same               the y-axis for the sake of clarity, are shown below
                                              company. This robust mount uses direct         and their standard deviation is 300 parts per million
                                                                                             (ppm). This light curve results from the global analy­
                                              drive technology to avoid the well-known
                                                                                             sis of 20 transits observed by TRAPPIST for this exo­
                                              periodic errors found on the usual equa­       planet.
Figure 2. Close-up of the 60-cm TRAPPIST      torial mounts for small telescopes and
telescope.
                                              therefore permits accurate pointing and
                                              tracking. The accuracy of the tracking         (1.3 arcseconds per pixel) and a 10 %
allowed us to set up the experiment in        allows an exposure time of four minutes        accuracy are B-band 16.2, V-band
less than two years.                          maximum, which is usually enough for           16.4, Rc-band 16.4, Ic-band 15.5 and
                                              our bright targets. Each frame is cali­        I + z-band 15.6; and in 200 seconds,
The observatory is controlled through a       brated in right ascension and declination      B-band 19.7, V-band 19.4, Rc-band 19.2
VPN (Virtual Private Network) connection      and software guiding runs continuously to      and I­c-band 18.1.
between La Silla and Liège University.        keep the target centred on the same few
The telescope and each individual sub­        pixels for the whole exposure sequence.        The camera is fitted with a double filter
system can be used from anywhere in                                                          wheel specifically designed for the pro­
the world, provided an internet connec­       The CCD camera was built by Finger             ject and allowing a total of 12 different
tion is available. In case of a low-level     Lakes Instrumentation, with thermo-­           5 × 5 cm filters and one clear position.
mechanical failure, we can count on the       electric cooling and a CCD of the latest       One filter wheel is loaded with six broad­
help of the Swiss technician on site or       generation. This is a thinned broad-           band filters (Johnson-Cousins BVRcIc,
the La Silla staff.                           band backside-illuminated Fairchild chip       Sloan z’, and a special I + z filter for exo­
                                              with 2048 × 2048 15-µm pixels providing        planet transits) and the other filter wheel
Hundreds of images, amounting to              a field of view of 22 by 22 arcminutes         is loaded with six narrowband filters
2–15 GB, are produced every night.            and a plate scale of 0.6 arcseconds per        for the comet programme. The comet
Reduction pipelines run on a dedicated        pixel. The sensitivity is excellent over       ­filters were designed by NASA for the
computer installed in the control room.       all the spectral range, with a peak of 98 %     international Hale–Bopp campaign
For the exoplanet programme, only tables      at 750 nm, declining to around 80 %             ­(Farnham et al., 2000). Four filters iso­
and plots with the final results are trans­   at 550 nm and 60 % at 300 nm. It is opti­        lating the main molecular emission lines
ferred to Liège, while for the comet pro­     mised for low fringe level in the far red        present in cometary spectra (OH [310 nm],
gramme, it is often necessary to transfer     and achieves a sensitivity of 40 % at            CN [385 nm], C3 [405 nm], C2 + NH2
dozens of frames in order to perform          950 nm. The gain is set to 1.1 e-/ADU.           [515 nm]) are permanently mounted,
more interactive tasks on the images.         There are three different readout modes:         while the two other filters of the set
Every third month, a backup disk is sent      a low noise readout mode (readout noise          (CO+ [427 nm] and H2O+ [705 nm]) are
to Belgium and transferred to the archive     [RON] 9.7 e- in 8s), a fast mode (RON            also available. In addition two narrow­
machine.                                      14 e- in 4s) and a very fast readout of 2s       band filters, isolating “continuum win­
                                              using two quadrants. The cooling is              dows” (BC [445 nm] and GC [525 nm]) for
The telescope is a 60-cm f/8 Ritchey–         –55 deg below ambient, usual operation           the estimation of the solar spectrum
Chrétien design built by the German           being at –35 °C with a dark count of             reflected by the dust of the comet, are
ASTELCO company (see Figure 2). Owing         0.11 e-/s/pixel. Typical magnitudes              mounted.
to its open design with carbon fibre and      reached in 20s with a 2 × 2 binning

                                                                                             The Messenger 145 – September 2011                  3
The Messenger No. 145 - September 2011 - European Southern Observatory
Telescopes and Instrumentation                    Jehin E. et al., TRAPPIST : TRAnsiting Planets and PlanetesImals Small Telescope

Installation, first light and start of            allowing us to constrain its bulk compo­         Characterisation of known transiting
operations                                        sition. Furthermore, the special geometry        planets
                                                  of the orbit makes the study of impor-           Once a transiting planet is detected, it is
The telescope was installed in April 2010         tant properties of the planet (e.g., atmos­      of course desirable to characterise it
in the T70 Swiss telescope building               pheric composition, orbital obliquity, etc)      thoroughly with high precision follow-up
belonging to Geneva University (Figure 1).        possible without the challenge of having         measurements. Assuming a sufficient
This facility had not been used since             to spatially resolve it from its host star.      precision, a transit light curve allows a
the 1990s and was completely refurbished          Transiting planets are thus key objects for      number of parameters to be thoroughly
in early 2010. The old 5-metre dome               our understanding of the vast planetary          constrained: (i) the planet-to-star radius
(­AshDome) was equipped with new azi­             population hosted by the Galaxy.                 ratio; (ii) the orbital inclination; (iii) the
muth motors and computer control. A                                                                ­stellar limb-darkening coefficients; and
Boltwood II meteorological station with a         Discovery of more transiting planets is           (iv) the stellar density (assuming the
cloud sensor and an independent rain              important to assess the diversity of plan­        orbital period is known). This last quantity
sensor was installed on the roof to record        etary systems, to constrain their forma­          can be used with other measured stellar
the weather conditions in real time. In           tion and the dependence of planetary              quantities to deduce, via stellar model­
case of bad conditions (clouds, strong            properties on external conditions (orbit,         ling, the mass of the star, which leads
wind, risk of condensation, rain or snow),        host star, other planets, etc.). TRAPPIST         finally to the stellar and planet radii (Gillon
the dome is automatically closed and              is participating in this effort through sev­      et al., 2007; 2009). So far, we have
the observations interrupted to guarantee         eral different projects.                          ­gathered many high precision light curves
the integrity of the telescope and equip­                                                            for two dozen transiting planets. These
ment. An uninterruptable power supply             Detection of new transiting planets                data will not only allow us to improve our
(UPS) keeps the observatory running for           On account of its extended temporal                knowledge of these planets (size, struc­
45 minutes during an electrical power             availability and high photometric preci­           ture), but also to search for transit timing
cut and an emergency shutdown is trig­            sion, TRAPPIST has very quickly become             variations that could reveal the presence
gered at the end of this period. Several          an important element for the transit               of other planets in the system. Since
webcams inside and outside the building           ­surveys WASP2 and CoRoT3. It is used to           TRAPPIST is dedicated to this research
help us to check what is going on in the           confirm the candidate transits detected           project, it can monitor dozens of tran-
observatory if needed. After two months            by these surveys and to observe them              sits of the same planet, leading to an
of commissioning on site, TRAPPIST                 with better time resolution and precision         exquisite global precision, as shown in
“first light” took place remotely on 8 June        to discriminate eclipsing binaries from           Figure 3.
2010, together with a press conference             planetary transits. TRAPPIST observa­
at Liège University1. Technical tests, fine        tions have so far rejected more than            Transit search around ultra-cool dwarf
tuning of the software as well as the first        30 WASP candidates as being eclipsing           stars (UCDs)
scientific observations were performed             binaries. It has confirmed, and thus co-        We have selected a sample of ten rela­
in remote control mode until November              discovered, ten new transiting planets          tively bright late-M stars and brown
2010. The fully robotic operation then             (e.g., Triaud et al., 2011; Csizmadia et al.,   dwarfs. For each of them, we have started
started smoothly in December with sev­             2011; Gillon et al., 2011).                     an intense monitoring campaign (several
eral months of superb weather until the                                                            full nights) to search for the transits of
start of the winter.                              The search for transits of the planets           the ultra-short period (less than one day)
                                                  detected by the radial velocity (RV) tech­       terrestrial planets that are expected by
The two scientific aspects of this dedi­          nique is another important science driver        some planetary formation theories. The
cated telescope and the first results are         for TRAPPIST. RV surveys monitor stars           photometric variability of these UCDs
described below.                                  significantly brighter than the transit sur­     brings a lot of information on their atmos­
                                                  veys. The few RV planets that were               pheric and magnetic properties, and
                                                  revealed afterwards to be transiting, have       the by product of this TRAPPIST project
Survey of transiting exoplanets                   brought improved knowledge of exo­               will thus be a significant contribution
                                                  planet properties because a thorough             to the understanding of these fascinating
The transit method used by TRAPPIST is            characterisation is possible (e.g., Deming       UCDs that dominate the Galactic stellar
an indirect technique, based on the               & Seager, 2009). These planets thus              population.
measurement of the apparent brightness            play a major role in exoplanetology. In this
of a star. If a planet passes in front of         context, TRAPPIST is used to search for
the star, there is a slight observable            the possible transits of the planets             Survey of the chemical composition of
decline in the apparent luminosity, as the        detected by the HARPS (Mayor et al.,             comets
planet eclipses a small fraction of the           2003) and CORALIE (Queloz et al., 2000)
stellar disc. Recording this periodic event       Doppler surveys. For the late M-dwarfs           TRAPPIST is the only telescope in the
allows the radius of the planet to be             observed by HARPS, TRAPPIST is even              southern hemisphere equipped with
measured. Combined with the radial                able to detect the transit of a massive          the instrumentation to detect gaseous
velocity method, the transit method pro­          rocky planet.                                    comet emissions on a daily basis. As
vides the mass and density of the planet,                                                          recently outlined during a NASA work­

4            The Messenger 145 – September 2011
The Messenger No. 145 - September 2011 - European Southern Observatory
OH                                                     CN                                              C3

   C2                                                     GC                                              H 2O

Figure 4. Comet 103P/Hartley 2 imaged with             calibration, image analysis can reveal          follow-up of split comets and of special
­T RAPPIST through the different cometary filters on
                                                       coma features (jets, fans, tails), that could   outburst events is possible very shortly
 5 November 2010: OH, CN, C 3, C2, green continuum
 (GC) and H2O+. Note the different shapes and inten­   lead to the detection of active regions         after an alert is given and can thus pro­
 sities of the cometary coma in each filter.           and determination of the rotation period        vide important information on the nature
                                                       of the nucleus. Such regular measure­           of comets. Light curves from these data
                                                       ments are rare because of the lack of tel­      are useful to assess the gas and dust
shop 4, the huge amount of data col­                   escope time on larger telescopes, yet are       activity of a given comet in order, for
lected by T ­ RAPPIST will bring crucial               very valuable as they show how the gas          instance, to prepare more detailed obser­
new information on comets and will                     production rate of each species evolves         vations with larger telescopes, espe-
­rapidly increase statistics, allowing com­            with respect to the distance to the Sun.        cially the southern ESO telescopes. Hun­
 ets to be classified on the basis of their            These observations will allow the compo­        dreds of photometric and astrometric
 chemical composition. Linking those                   sition of the comets and the chemical           measurements of all the moving targets in
 chemical classes to dynamical types (for              class to which they belong (rich or poor in     our frames are reported each month to
 instance short period comets of the                   carbon chain elements for instance) to          the IAU Minor Planet Center. Two new
 Jupiter family and new long period com­               be determined, possibly revealing the ori­      asteroids were found during a laboratory
 ets from the Oort Cloud) is a funda­                  gin of those classes. Indeed with about         session with students of Liège University.
 mental step in understanding the forma­               five to ten bright comets observed each         The observatory code attributed by the
 tion of comets and the Solar System.                  year, this programme will provide a good        IAU is I40.
                                                       statistical sample after a few years.
For relatively bright comets (V ≤ 12 mag),                                                             Our first target was periodic comet 103P/
about twice a week, we measure gase­                   Broadband photometry is also performed          Hartley 2, which made a close approach
ous production rates and the spatial dis­              once a week for fainter comets, usually         to Earth in October 2010 and was
tribution of several molecular species,                far from the Sun, in order to measure the       observed in great detail during the NASA
including OH, CN, C2, and C3 (see Fig­                 dust production rate from the R-band,           EPOXI spacecraft flyby on 4 November.
ure 4 for an example). In addition to pro­             to catch outbursts and find interesting         We monitored this small (2 km) but very
viding the production rates of the differ­             targets for the main programme. Owing           active comet roughly every other night for
ent species through a proper photometric               to the way the telescope is operated, the       four months and collected ~ 4000 frames

                                                                                                       The Messenger 145 – September 2011      5
The Messenger No. 145 - September 2011 - European Southern Observatory
Telescopes and Instrumentation                      Jehin E. et al., TRAPPIST : TRAnsiting Planets and PlanetesImals Small Telescope

                                                    ­ steroid Belt and not the result of
                                                    A                                               key asset for confirming and characteris­
                                                    cometary activity (Jehin et al., 2010).         ing these planets.

                                                    Among other related projects we joined          Further information and the latest news
                                                    an international collaboration whose            about TRAPPIST can be found on our
                                                    goal is to catch rare stellar occultations      web page 6.
                                                    by large trans-Neptunian objects (TNOs).
                                                    This technique provides the most accu­
                                                    rate measurements of the diameter of            Acknowledgements
                                                    these very remote and poorly constrained        We would like to thank the following: Grégory
                                                    icy bodies (provided at least two chords        ­L ambert of the Geneva Observatory for the continu­
                                                    are observed). About one to two events           ous technical support on site and Vincent Megevand
                                                    per month are expected for a dozen big           when he was in charge; Michel Crausaz, Nigel
                                                                                                     ­Evershed, Jean-Francois Veraguth, Francesco Pepe,
                                                    TNOs. On 6 November 2010, a unique                Charles Maire, and Michel Fleury from Geneva
                                                    observation was performed. A faint star           Observatory for the refurbishment phase of the T70
                                                    was occulted by the dwarf planet Eris             building; Andrew Wright and Alexis Thomas from
                                                    for 29 seconds. Eris is the most distant          ESO and Pierre Demain from Liège University for the
                                                                                                      set-up of VPN at each site; Karina Celedon from
Figure 5. The TRAPPIST image of the the activated   object known in the Solar System by               ESO for the very efficient work and great help in the
asteroid (596) Scheila taken on 18 December 2010.
                                                    far (three times the distance of Pluto) and       delivery of the many telescope parts to Chile and
                                                    supposedly the biggest TNO — it was               the La Silla Observatory; David Schleicher from
                                                    even named the tenth planet for a few             ­Lowell Observatory for having recovered and lent
                                                                                                       one c   ­ omplete set of NASA cometary filters and Alain
through ten different filters. Our contribu­        months in 2006. This was the third posi­           ­G illiotte from ESO for the optical characterisation
tion to the worldwide campaign on this              tive occultation by a TNO ever recorded             of those fi­ lters; Sandrine Sohy and Robert Sip from
comet was recently published in Meech               and it allowed a very accurate radius               Liège University for setting up all the computers
et al. (2011). The quality of the data              for Eris (to a few kilometres) to be derived,       and backup procedures and Sandrine for being the
                                                                                                        webmaster.
allowed us to observe periodic variations           providing a huge improvement in the
in the gaseous flux of the different spe­           determination of its size (previously known     We would finally like to pay special thanks to the
cies from which we could determine the              to within about 400 km). The surprise           whole staff of La Silla, and especially Gerardo Ihle and
rotation of the nucleus and show that               was to discover that Eris is a twin of Pluto    Bernardo Ahumada, for their constant help and sup­
                                                                                                    port, most particularly during the installation phase.
the rotation was slowing down by about              and that it is not much bigger — remem­
one hour in 100 days (Jehin et al., 2010).          ber that Pluto was demoted as a planet in        M. Gillon and E. Jehin are FNRS Research Associ­
This behaviour had never been so clearly            2006 because Eris was found to be big­           ates, J. Manfroid is an FNRS Research Director and
observed before. The long-term monitor­             ger — both then received the new status          D. Hutsemékers is an FRNS Senior Research
                                                                                                    ­A ssociate.
ing of the production rates of the different        of dwarf planets! A paper describing
species is nearly completed and will be             these results has been accepted for pub­
combined with high-resolution spectro­              lication in Nature (Sicardy et al., 2011).      References
scopic data in the visible and infrared that
                                                                                                    Csizmadia, Sz. et al. 2011, A&A, 531, 41
we obtained at the ESO Very Large Tele­                                                             Deming, D. & Seager, S. 2009, Nature, 462, 301
scope (VLT) to provide a clear picture of           Perspectives                                    Farnham, T. L. et al. 2000, Icarus, 147, 180
the chemical composition of this unusu­                                                             Gillon, M. et al. 2011, A&A (accepted)
ally active comet from the Jupiter family.          After only six months of robotic opera­         Gillon, M. et al. 2007, A&A, 466, 743
                                                                                                    Gillon, M. et al. 2009, A&A, 496, 259
                                                    tions, TRAPPIST is already recognised           Hsieh, H. & Jewitt D. 2006, Science 312, 561
On account of the fast reaction time                in the exoplanet and comet communities          Jehin, E. et al. 2010, CBET #2589
(a few hours), TRAPPIST is an invaluable            as a unique tool on account of, among           Jehin, E. et al. 2010, CBET, #2632
instrument for catching rare and short-             other things, the large amount of tele­         Mayor, M. et al. 2003, The Messenger, 114, 20
                                                                                                    Meech, K. et al. 2011, ApJL, 734, L1
term events. As an example, the night               scope time available under photometric          Queloz, D. et al. 2000, A&A, 354, 99
after the announcement that asteroid                conditions for performing time-consuming        Sicardy, B. et al. 2011, Nature, accepted
(596) Scheila was behaving like a comet             research. In particular, TRAPPIST has           Triaud, A. et al. 2011, A&A, 513, A24
and could be a new Main Belt comet                  very quickly become a key element in the
(only five of them are known — Hsieh &              follow-up effort supporting WASP. In            Links
Jewitt, 2006), we began a programme                 future, TRAPPIST will play a similar role
to monitor the expanding coma and the               for the successor of WASP, the Next             1
                                                                                                       ESO PR on TRAPPIST: http://www.eso.org/public/
brightness of the nucleus every night               Generation Transit Survey (NGTS)5, a pro­       2
                                                                                                       news/eso1023/
                                                                                                      Superwasp: http://www.superwasp.org
­during a period of three weeks (see Fig­           ject led by Geneva Observatory and sev­         3
                                                                                                        C oRoT: http://smsc.cnes.fr/COROT/index.htm
 ure 5 for one of the images). From imag­           eral UK universities, that will be installed    4
                                                                                                         C omet Taxonomy, NASA workshop held 12–16
 ing with TRAPPIST and spectroscopy                 at ESO Paranal Observatory in 2012.                March 2011, Annapolis, USA
                                                                                                    5
 with the ESO VLT we concluded that this            NGTS will focus on detecting smaller                  N ext Generation Transit Survey: http://www.
                                                                                                       ngtransits.org/
 behaviour was the result of a collision            planets than WASP, and the high photo­          6
                                                                                                           T RAPPIST web page: http://www.ati.ulg.ac.be/
 with a smaller asteroid in the Main                metric precision of TRAPPIST will be a             TRAPPIST/Trappist_main/Home.html

6            The Messenger 145 – September 2011
The Messenger No. 145 - September 2011 - European Southern Observatory
Telescopes and Instrumentation

CalVin 3 — A New Release of the ESO Calibrator
Selection Tool for the VLT Interferometer

Markus Wittkowski1                             NIR instrument AMBER and the MIR               sions of CalVin, version 3.0 released in
Pascal Ballester1                              instrument MIDI, are supported by ESO in       January 2011 and version 3.1 released in
Daniel Bonneau2, 3                             the same way as any of the VLT instru­         July 2011, now offer major improvements
Alain Chelli2, 4                               ments of the Paranal observatory (c.f.         in terms of the number of available calibra­
Olivier Chesneau2, 3                           Wittkowski et al. [2005] for further general   tors, the functionality of the search tool, as
Pierre Cruzalèbes2, 3                          information on observing with the VLTI).       well as in performance and ease of use.
Gilles Duvert 2, 4
Christian Hummel1                               In particular, ESO supports the prepara­
Sylvain Lafrasse 2, 4                           tion of interferometric observations using    Number of available calibrators
Guillaume Mella 2, 4                            the AMBER and MIDI instruments with
Jorge Melnick1                                  the preparation tools VisCalc and ­CalVin1.   The underlying list of calibrators available
Antoine Mérand1                                VisCalc estimates visibility values for        with CalVin now incorporates the JMMC
Denis Mourard2, 3                              the expected intensity distribution of the     Stellar Diameter Catalog (JSDC2; Lafrasse
Isabelle Percheron1                            science target and the chosen VLTI             et al., 2010). This catalogue is based on
Stéphane Sacuto2, 5                            ­configuration to assess the feasibility of    a search of catalogues available at the
Klara Shabun1                                   an observation. CalVin may be used to         Centre de Données astronomiques de
Stan Stefl1                                     select calibration stars for a given sci­     Strasbourg (CDS) using the bright mode of
Jakob Vinther1                                  ence target based on an underlying list of    the JMMC calibrator search tool Search­
                                                calibrators and a number of user-defined      Cal3 (Bonneau et al., 2006) with the faint­
                                                criteria. Both tools are also offered in an   est limiting magnitudes that are offered for
1
  ESO                                           expert mode for the use of any arbitrary      the VLTI. The angular diameter estimates
2
  Jean-Marie Mariotti Center, France            observatory location, baseline configura­     and their errors given in the resulting table
3
  Université Nice Sophia Antipolis, CNRS,      tion and spectral wavelength band (for        are based on statistical estimates and
   Observatoire de la Côte d’ Azur, Nice,       CalVin B-, V-, R-, I-, J-, H-, or K-bands).   ­provide information on whether a star is a
   France                                                                                      suitable calibration source for a certain
4
   Université Joseph Fourier 1/CNRS-          Optical interferometers measure the             instrument and baseline configuration.
    INSU, Institut de Planetologie et          amplitude and phase of the interference
    d’Astrophysique de Grenoble, France        pattern. When normalised these quan­           The observer may need to study selected
5
    Department of Physics and Astronomy,      tities are the amplitude and phase of the      calibrators in more detail to obtain a
     Uppsala University, Sweden                complex visibility function, which is re­­     more precise estimate of their diameters
                                               lated to the intensity distribution by a       (c.f., for example, Cruzalèbes et al., 2010).
                                               Fourier transform. An unresolved point         Each calibrator is assigned a quality
Interferometric observations require           source theoretically has a visibility ampli­   grade depending on whether it is only
­frequent measurements of calibration          tude of unity. However, the measured           included in the JSDC catalogue or is also
 stars of known diameter to estimate           ­visibility amplitude of an infinitely small   in the catalogues by Bordé et al. (2002),
 the instrumental transfer function. ESO        target, also called the interferometric       Mérand et al. (2005) or Verhoelst (2005),
 offers the preparation tool CalVin to          transfer function, will be less than unity    which were used as the core underlying
 select suitable calibrators from an un­­       owing to losses introduced by the Earth’s     catalogues of CalVin 2, and whose prop­
 derlying list of calibrators. The latest       atmosphere and the instrument. These          erties are studied in more detail.
 version 3, first released in January 2011,     losses are time variable and need to be
 offers major improvements in the num-          frequently monitored. For this purpose,       The capacity of, for example, the NIR
 ber of available calibrators, the func-        the observer needs to select suitable         AMBER table is now 27 814 calibrators,
 tionality of the search tool, as well as in    ­calibration stars of known diameter, which   of the MIR MIDI table 27 989 calibrators,
 terms of performance and ease of use.           will be observed close in time to the sci­   and of arbitrary locations (expert version
 It has been developed in a collaboration        ence targets.                                of CalVin) 38 472 calibrators. Figure 1
 between ESO and the French Jean-                                                             shows the sky coverage of the underlying
 Marie Mariotti Center (JMMC).                 With the growing capabilities of the VLTI,     list of calibrators available for AMBER,
                                               the increasing number of instrument            highlighting two typical use cases, a
                                               modes, and the improving limiting mag­         bright calibrator case and a faint calibra­
The ESO VLT interferometer (VLTI) is an        nitudes, it has become clear that CalVin’s     tor case. The bright c  ­ alibrator case high­
optical interferometer that is offered as a    capabilities need to be improved beyond        lights calibrators of K magnitudes K < 3
general user facility. It enables the com­     those available when it was first offered      as they are required for observations using
munity to conduct near-infrared (NIR) and      in ESO Period 73. Starting with a work­        the 1.8-metre auxiliary telescopes (ATs)
mid-infrared (MIR) interferometric obser­      shop on interferometric calibrators held in    and moderate c   ­ onditions of 1.2-arcsec­
vations to obtain high spatial resolution      Nice, France, in March 2008, ESO and the       ond seeing. The faint case highlights cali­
measurements of celestial sources. The         French Jean-Marie Mariotti Center (JMMC)       brators of K magnitudes 5 < K < 7 as
instruments of the VLTI that are offered       have been collaborating on de­­veloping a      they are typically re­­quired for observations
to the community, currently including the      new version of CalVin. The two latest ver­     using the 8-metre unit telescopes (UTs).

                                                                                              The Messenger 145 – September 2011          7
The Messenger No. 145 - September 2011 - European Southern Observatory
Telescopes and Instrumentation                  Wittkowski M. et al., Calvin 3

New functionality of the selection tool                30

CalVin’s selection tool includes a number              15
of new functionalities corresponding to
the increasing number of instrument
                                                        0
modes available. CalVin can now be used
to search for only those calibrators that
are suited to a user-defined instrument               –15
                                                DEC

mode in terms of the offered magnitude
range of the respective mode. Observa­                – 30
tions are offered in service mode and
­visitor mode, where, in visitor mode the             – 45
 day of observation is known beforehand,
 but in service mode it is not. CalVin now
 accepts time ranges of either Universal              – 60
 Time, local sidereal time, or hour angle.
 CalVin outputs the observability of the              – 75
 science target and of the calibrators for                   0                   6                       12                       18                       24
                                                                                                         RA
 the specified time interval taking into        Figure 1. Sky coverage of the underlying list of cali­
 account the target altitude, shadowing         brators available for the example of the NIR instru­
 constraints and the limited delay line         ment AMBER. Blue circles highlight bright calibrators
                                                as typically used with the ATs and moderate (1.2 arc­
 stroke. In the case of Universal Time, the     second) seeing conditions for which K < 3 mag. Red
 sun altitude is also taken into account.       circles mark faint calibrators as typically used for
 In order to assess the feasibility of a        observations with the UTs (5 < K < 7 mag).

                                                                                                         Figure 2. The use of CalVin is illustrated through
                                                                                                         screenshots of the input and output pages, the latter
                                                                                                         including some graphs.

8          The Messenger 145 – September 2011
The Messenger No. 145 - September 2011 - European Southern Observatory
­ alibrator observation, visibility ampli­
                  c                                             tors. We plan to add these using data           bases4, 5 as well as information on previ­
                  tudes are computed for the same time          from the AKARI/IRC mid-infrared all-sky         ous observations may be added to the
                  intervals at the wavelengths of observa­      survey (Ishiara et al., 2010). With upcom­      output result of CalVin in a future release.
                  tion and of the VLTI fringe tracker FINITO,   ing fainter limiting magnitudes for the
                  and magnitudes are given at the wave­         ­current VLTI instruments, and in particu­
                  lengths of the guiding camera IRIS and         lar for second generation VLTI instru­         References
                  the Coudé guiding camera. Figure 2             ments, the current underlying list may still   Beust, H. et al. 2011, MNRAS, 414, 108
                  shows for illustration some screenshots        not be sufficiently complete for the faint­    Bonneau, D. et al. 2006, A&A, 456, 789
                  of a query using CalVin.                       est magnitudes offered. The faint mode         Bonneau, D. et al. 2011, to appear in A&A
                                                                 of SearchCal (Bonneau et al., 2011) may        Bordé, P. et al. 2002, A&A, 393, 183
                                                                                                                Cruzalèbes, P. et al. 2010, A&A, 515, A6
                                                                 then be used to create a significantly         Ishihara, D. et al. 2010, A&A, 514, A1
                  Performance of CalVin                          larger underlying list of calibrators, which   Lafrasse, S. et al. 2010, VizieR Online Data
                                                                 would also impose stronger requirements           Catalog, 2300
                  The performance of CalVin, in particular       on the database technology. The addi­          Mérand, A. et al. 2006, A&A, 447, 783
                                                                                                                Verhoelst, T. 2005, PhD thesis K. U. Leuven, Belgium
                  in terms of response time, has been            tional use of the AKARI point source cat­      Wittkowski, M. et al. 2005, The Messenger, 119, 14
                  ­optimised using a new database technol­       alogue might then also allow a more
                   ogy and JavaScript-based visualisation        robust selection of calibrator sources to
                   technology to display the plots. The ease     be obtained. Astrometric observations          Links
                   of use has also been improved by opti­        using the upcoming VLTI facilities PRIMA       1
                                                                                                                   isCalc and CalVin are available from: http://www.
                                                                                                                  V
                   mising the layout of the query page, now      and GRAVITY may require further selec­           eso.org/observing/etc
                   including one single input page (Figure 2,    tion criteria, such as a low proper motion     2
                                                                                                                  T he JSDC catalogue: http://cdsarc.u-strasbg.fr/cgi-
                   left), compared to two pages in version 2.    of a phase reference calibrator, requir-          bin/VizieR?-source=II/300
                                                                                                                3
                                                                                                                   SearchCal is available at: http://www.jmmc.fr/
                                                                 ing additional information in the database         searchcal
                                                                 as well as additional search criteria. An      4
                                                                                                                    T he IAU Comm. 54 bad calibrators’ registry (BCR)
                  Future directions                              example of such a search for astrometric            is available at: http://www.eso.org/sci/observing/
                                                                 calibrators was recently described by               tools/catalogues/bcr.html
                                                                                                                5
                                                                                                                     T he bad calibrators’ database at JMMC: http://
                  The current underlying list of calibrators     Beust et al. (2011). Information on entries          apps.jmmc.fr/badcal
                  lacks MIR magnitudes for many calibra­         in the available bad calibrators’ data­
ESO/Y. Beletsky

                                                                                                                              One of the VLTI 1.8-metre Auxiliary
                                                                                                                              Telescopes (ATs) being replaced on its
                                                                                                                              tracks at Cerro Paranal after mirror re-
                                                                                                                              aluminising. Each AT has its own
                                                                                                                              transporter that lifts the telescope and
                                                                                                                              moves it from one observing position
                                                                                                                              to another on tracks. However the
                                                                                                                              transfer by road to and from the coat­
                                                                                                                              ing plant at the base camp relies on a
                                                                                                                              truck, as shown.

                                                                                                                The Messenger 145 – September 2011                   9
The Messenger No. 145 - September 2011 - European Southern Observatory
Telescopes and Instrumentation

A New Massively-multiplexed Spectrograph for ESO

Suzanne Ramsay1                                  In 2010, ESO launched a call for proposals        Each panel was charged with commenting
Peter Hammersley1                                for the conceptual design of a multi-object       on the suitability of the proposals for fur­
Luca Pasquini1                                   spectroscopic (MOS) instrument/facility           ther study. The proposals were for six very
                                                 for carrying out public surveys. Up to two        powerful and very different instruments.
                                                 proposals were to be selected for a com­          These included slit- and fibre-based spec­
1
    ESO                                          petitive Phase A study. The call for pro­         trographs, covering the optical and near-
                                                 posals was very broad and stated that the         infrared wavelength ranges and were for
                                                 instrument should provide the ESO astro­          the VLT, VISTA and the NTT. Although
With the advent of many large-area               nomical community with the ability to             some of the projects were judged to be
imaging surveys in recent years, the             carry out original wide-field spectroscopic       very challenging and ambitious, no techni­
need for a new facility for spectroscopic        science. Beyond this requirement, the             cal show-stoppers were identified. The
surveys has become apparent. Follow-             instrument concept and the detailed sci­          scientific committee strongly endorsed the
ing a recommendation from the Science            entific goals were left open. Proposals           2017 delivery timescale envisaged for
and Technical Committee, ESO made a              were solicited for any ESO telescope: up­­        the instrument as being required for Gaia
call in 2010 for wide field spectroscopic        grades to existing instruments or com­            and eROSITA follow-up. The requirement
instrument proposals among its com-              pletely new instrument concepts were              for high spectral resolving power (λ/δλ >
munity. Two of the ten proposals were            both within the scope of the call. Even           10 000) for optimal exploitation of Gaia
selected for a competitive Phase A               proposals for non-ESO telescopes were             was stressed. The possible selection of
study. This article describes the selec-         permissible. In total, ten letters of interest,   Euclid at the end of 2011 by ESA is ex­­
tion process and two associated articles         describing in brief the proposal concept,         pected to have an important influence,
present the instrument concepts.                 were sent in by the community. Six teams          as the science goals of its spectroscopic
                                                 were invited to submit full proposals con­        instrument overlap with this project.
                                                 sisting of a scientific and technical report
Large-scale observational surveys are            and a management plan for the design              Overall, the science panel reached excel­
powerful tools for advancing many astro­         study.                                            lent agreement as to the most suitable
nomical fields, often opening up new                                                               proposals for further work. Finally, ESO
directions of research, whether the goal is      The final proposals were delivered on             management received the input from the
a statistical understanding of a particular      1 March 2011 and included over 30 institu­        two committees and selected the con­
class of source or the search for rare           tions and 160 contributors, demonstrating         cepts for study. Their recommendation
objects. In the optical and infrared many        the wide interest in such an instrument.          was presented to the Science and Tech­
new ground-based imaging surveys are             The quality of the submitted scientific and       nical Committee at its April 2011 meet-
underway (e.g., WFCAM, VISTA, Pan­               technical ideas was warmly appreciated            ing. The successful proposals are for
STARRS), are about to start (VST) or in          by ESO and the panels involved in the             MOONS — a fibre-fed infrared spectro­
the planning stages (Large Synoptic Sur­         evaluation of the instrument concepts.            graph designed for the VLT, led by Michele
vey Telescope, LSST). These imaging sur­                                                           Cirasuolo from the UK Astronomy Tech­
veys will yield catalogues of hundreds of        The proposals were reviewed from a tech­          nology Centre, and for 4MOST — a fibre-
millions of sources and target scientific        nical and scientific perspective by sepa­         fed optical spectrograph, led by Roelof
fields from gravitational lensing to the star    rate panels. The technical panel consisted        de Jong from the Leibniz-Institut für Astro­
formation history of the Galaxy, such as         of engineers and scientists from within           physik Potsdam. Conceptual designs for
for VISTA and VST (Arnaboldi et al., 2007).      ESO. The technical review addressed the           4MOST on both the VISTA and NTT tele­
In space, Gaia will provide an unprece­          quality of the technical case for the instru­     scopes will be explored by the team before
dented catalogue of positional and radio-        ment concept, including the level of risk         the selection is made at the midterm of
velocity information for about a billion         involved in the design, the quality of the        the design study. In the following two arti­
stars and the eRosita mission will explore       management plan and the experience of             cles the scientific and instrumental as­­pects
the nature of dark matter and dark energy        the team. The important factors of the            of the two proposals are summarised.
with an all-sky X-ray survey. These survey       impact on the telescope and the opera­
projects will deliver new results in the         tional model for the instrument were also         The Phase A for the two instruments will
­second half of this decade which will de­­      considered.                                       finish in February 2013. It is expected
 mand spectroscopic follow-up. The re­­                                                            that one of the instrument concepts will
 quirement for a highly-multiplexed spec­        The scientific panel was made up by a             then be recommended to the STC for
 trograph was identified in the ASTRONET         50:50 split of astronomers from the com­          detailed design and construction. ESO’s
 Infrastructure Roadmap (Bode, Cruz &            munity and from ESO. It commented                 goal is to offer a new spectroscopic facil-
 Molster, 2008) as a high priority for ex­­      on the major scientific questions to be an­­      ity on one of its telescopes around 2017.
 ploiting these, and other, missions and as      swered by the instrument, whether the
 a standalone facility. The ESO Science          science case would be interesting and
 and Technology Committee (STC) has              competitive on the timescales of 2016             References
 recommended that steps be taken to              and beyond and whether the instrument             Arnaboldi, M. et al. 2007, The Messenger, 127, 28
 improve the existing ESO capabilities in        ­concept presented would address those            Bode, M. F., Cruz, M. J. & Molster, F. J. 2008., The
 this field.                                      goals.                                             ASTRONET Infrastructure Roadmap, Astronet

10          The Messenger 145 – September 2011
Telescopes and Instrumentation

MOONS: The Multi-Object Optical and Near-infrared
Spectrograph

Michele Cirasuolo1, 2                                        Bologna; 9 CEA–Saclay, Paris; 10 Lund Observatory;     Galactic archaeology
                                                             11
                                                                INAF–Osservatorio Astronomico Roma; 12 Dark
José Afonso 3
                                                             Cosmology Centre, Copenhagen; 13 IASF–INAF,
Ralf Bender4, 5                                              Milano; 14 ETH Zürich; 15 Universitäts-Sternwarte      The study of resolved stellar populations
Piercarlo Bonifacio 6                                        München; 16 Max-Planck-Institut für Astrophysik;       of the Milky Way and other Local Group
Chris Evans1                                                 17
                                                                INAF–Osservatorio Astrofisico di Arcetri; 18 Max-   galaxies can provide us with a fossil
                                                             Planck-Institut für extraterrestrische Physik;
Lex Kaper 7                                                  19
                                                                                                                    record of their chemo-dynamical and star
                                                                NOVA-ASTRON; 20 INAF–Osservatorio Astronomico
Ernesto Oliva 8                                              Padova; 21 Durham University; 22 Leiden Observa­       formation histories over many-gigayear
Leonardo Vanzi 9                                             tory; 23 Kapteyn Astronomical Institute                timescales. Scheduled for launch in 2013,
                                                                                                                    the ESA Gaia mission will deliver new
                                                                                                                    insight into the assembly history of the
1	STFC United Kingdom Astronomy                             MOONS (Multi-Object Optical and                        Milky Way, but to exploit its full potential,
    Technology Centre, Edinburgh, United                     Near-infrared Spectrograph) is a large                 ground-based follow-up is required.
    Kingdom                                                  field (500 square arcminutes), multi-                  MOONS will provide this crucial follow-up
2	Institute for Astronomy, University of                    object (500 object + 500 sky fibres)                   for Gaia and for other ground-based sur­
    Edinburgh, United Kingdom                                instrument with spectral resolution of                 veys such as Pan-STARRS and UKIDSS,
3	Observatorio Astronomico de Lisboa,                       5000 and 20 000 proposed for the VLT                   and the surveys with VISTA, by measur­
    Portugal                                                 Nasmyth focus. The science case for                    ing accurate radial velocities, metallicities
4	Universitäts-Sternwarte, München,                         MOONS, covering Galactic structure                     and chemical abundances for several
    Germany                                                  and galaxy evolution up to the epoch                   ­million stars. Given the spectral resolu­
5	Max-Planck-Institut für extrater­                         of re-ionisation, is briefly outlined.                  tions (R ~ 5000 and R ~ 20 000) and its
    restrische Physik, München, Germany                                                                              ability to observe in the NIR, MOONS will
6	GEPI, Observatoire de Paris, CNRS,                        MOONS1 is a new conceptual design for                   perfectly complement the ongoing and
    Univ. Paris Diderot, France                              a Multi-Object Optical and Near-infrared                planned surveys (see Figure 1) including
7	Astronomical Institute Anton Pannekoek,                   Spectrograph, which will provide the                    the new large Gaia–ESO public spectro­
    Amsterdam, the Netherlands                               ESO astronomical community with a                       scopic survey. The unique features of
8	INAF–Osservatorio Astrofisico di                          powerful and unique instrument that is                  MOONS will allow us in particular to clar­
   ­Arcetri, Italy                                           able to serve a wide range of Galactic,                 ify the nature of the extincted regions of
9	Centre for Astro-Engineering at Univer­                   extragalactic and cosmological studies.                 the Bulge, but also to assess the chemo-
    sidad Catolica, Santiago, Chile                          The grasp of the 8.2-metre Very Large                   dynamical structure of the Galactic thin
                                                             Telescope (VLT) combined with the large                 and thick disc, understand the impor­
                                                             multiplex and wavelength coverage of                    tance of satellites and streams in the
 Team members:                                               MOONS — extending into the near-                        halo, ultimately creating an accurate 3D
 Miguel Abreu1, Eli Atad-Ettedgui2, Carine
                                                             infrared (NIR) — will provide the obser­                map of our Galaxy to provide essential
 ­Babusiaux 3, Franz Bauer4, Philip Best5, Naidu
  Bezawada 2, Ian Bryson2, Alexandre Cabral1, Karina         vational power necessary to study galaxy                insight into its origin and evolution.
  Caputi 5, Fanny Chemla3, Andrea Cimatti 6, Maria-          formation and evolution over the entire
  Rosa Cioni7, Gisella Clementini 8, Emanuele Daddi 9,       history of the Universe, from the Milky
  James Dunlop5, Sofia Feltzing10, Annette Ferguson5,
                                                             Way, through the redshift desert and up                The growth of galaxies
 Andrea Fontana11, Johan Fynbo12, Bianca Garilli13,
 Adrian Glauser14, Isabelle Guinouard 3, Francois            to the epoch of re-ionisation at z > 8–9.
 Hammer 3, Peter Hastings2, Hans-Joachim Hess15,             At the same time, the high spectral reso­              Tracing the assembly history of galaxies
 Rob ­Ivison2, Pascal Jagourel3, Matt Jarvis7, Guinivere     lution mode will allow astronomers to                  over cosmic time remains a primary
  Kauffmann16, Andy Lawrence 5, David Lee2, Gianluca
                                                             study chemical abundances of stars in                  goal for observational and theoretical
 Licausi11, Simon Lilly14, Dario Lorenzetti11, Roberto
 Maiolino11, Filippo Mannucci17, Ross McLure 5, Dante        our Galaxy, in particular in the highly                studies of the Universe. Even though, in
 Minniti4, David Montgomery 2, Bernard Muschielok15,         obscured regions of the Bulge, and pro­                recent years, large spectroscopic surveys
  Kirpal Nandra18, Ramón Navarro19, Peder Norberg5, 21,      vide the necessary follow-up of the Gaia               at optical wavelengths (0.3–1 μm) have
  Livia Origlia8, Nelson Padilla4, John Peacock5, Laura
                                                             mission.                                               provided key information on the formation
­Pentericci11, Mathieu Puech3, Sofia Randich17, Alvio
 Renzini20, Nils Ryde10, Myriam Rodrigues 3, Roberto                                                                and evolution of galaxies, NIR spec­
 Saglia15, 5, Ariel Sanchez18, Hermine Schnetler 2,                                                                 troscopy is now crucial to extend our
 David Sobral 5, 22, Roberto Speziali11, Eline Tolstoy 23,   Science objectives                                     knowledge beyond z ~ 1. In fact, at these
 Manuel Torres 4, Lars Venema 21, Fabrizio Vitali11,
                                                                                                                    ­redshifts almost all the main spectral
 Michael Wegner15, Martyn Wells2, Vivienne Wild 5,
 Gillian Wright 2                                            MOONS will be a versatile, world-leading                ­features are shifted at λ > 1 μm. Exploit­
                                                             instrument able to tackle some of the                    ing the large multiplex and wavelength
                                                             most compelling key questions in sci­                    coverage of MOONS, it will be possible to
1
   Centre for Astronomy & Astrophysics University of         ence: How do stars and galaxies form                     create the equivalent of the successful
 Lisboa; 2 United Kingdom Astronomy Technology               and evolve? Do we understand the                         Sloan Digital Sky Survey, but at z > 1 (see
 Centre; 3 GEPI, Observatoire de Paris; 4 Centre for
                                                             extremes of the Universe? Here we briefly                Figure 2). This will provide an unparal­-
 Astro-Engineering, Universidad Catolica; 5 Institute
 for Astronomy, Edinburgh; 6 Università di Bologna –         highlight some of the main science cases                 leled resource to study the physical pro­
 Dipartimento di Astronomia; 7 University of                 that are driving the design of MOONS.                    cesses that shape galaxy evolution
­H ertfordshire; 8 INAF–Osservatorio Astronomico                                                                      and determine the key relations between

                                                                                                                    The Messenger 145 – September 2011        11
Telescopes and Instrumentation                                                                                  Cirasuolo M. et al., MOONS

Figure 1. Number den­                                                             Apogee R ≈ 20 000 Near-IR                                                                                                      stellar mass, star formation, metallicity
sity of stars in the vari­                                                                                                                                                       Bulge                           and the role of feedback. Filling a critical
ous components of the                                                         5                                                                                                                                  gap in discovery space, MOONS will be
                              Log (Cumulatif Number of Stars/square degree)

Milky Way shown as a                                                                HERMES RVS ≈ 30 000 Optical
                                                                                                                                                            s
function of V-band mag­                                                                                                                              te r                                                        a powerful instrument to unveil “the red­
                                                                                                                                               lus
                                                                                                                                          rc
nitude (figure adapted                                                               Gaia RVS ≈ 7500 Optical                      bu
                                                                                                                                     la                         MOONS                                            shift desert” (1.5 < z < 3, see Figure 2)
from Recio-Blanco, Hill &                                                                                                   Glo
                                                                              4                                                                                 > 1000 sq.deg.                                   and study this crucial epoch around the
Bienaymé, 2009). Gaia
will provide astrometry
                                                                                      RAVE R ≈ 7500 Optical                                                     > 2 million stars                                peak of star formation, the assembly
for all stars with V < 20,                                                                                                                                                                                       of the most massive galaxies, the effect
however the onboard                                                                                                                                                                                              of the environment and the connection
spectrometer (RVS) will                                                       3                                                                                                                                  with the initiation of powerful active
deliver chemical abun­
dance only for stars                                                                                                                                                                                             galactic nuclei. MOONS will also provide
brighter than magnitude                                                                                                                                                                                          the essential deep spectroscopic follow-
13 and radial velocities                                                                                                                                                                                         up of imaging surveys undertaken with
for stars brighter than 17.                                                   2
                                                                                                                                                                                                                 facilities in optical and near-IR (VISTA,
MOONS will perfectly
complement Gaia and                                                                                                                                                                                              UKIDSS, VST, Pan-STARRS, Dark Energy
the other spectroscopic                                                               Thin Disc        Thick Disc                                      Halo                                                      Survey, LSST) and facilities operating
surveys (e.g., Apogee,                                                        1                                                                                                                                  at other wavelengths (ALMA, Herschel in
Hermes, RAVE) provid­                                                          10                 12                 14                 16                            18                     20
                                                                                                                                   V mag                                                                         the infrared, eRosita in the X-ray and
ing chemical abun­
dances via high resolu­                                                             Chemical abundances                                                          Radial velocities and [Fe/H]                    LOFAR, WISE and ASKAP in the radio).
tion spectroscopy in the                                                            in NIR with R ≈ 20 000                                                       via CaT with R ≈ 5000–10 000
NIR (e.g., observing Ca,
Si, S, Fe, Ti lines) and
radial velocities via the
calcium triplet.                                                                                                                                                                                                  (O III)
                                                                                                                                                                              Lyα                      (O II)    Hβ
                                                                                                                                                                                                                                  Hα
                                                                                     1.
                                                                                       05

                                                                                                                                                                                                                                                               MOONS
                                                                                                                                                                                                                                                               z = 1.5
                                                                                              1.

                                                                                                                                                                                                             Gb
                                                                                                 20

                                                                                                                                                                                               Mg I         Bδ
                                                                                                                                                                                                                                             CaT
                                                                                                                                                                                               Mg II      H,K
                                                                                                         0.

                                                                                                            re
                                                                                                             90

                                                                                                               ds

                                                                                                                                                                                    0.5                    1                1.5          2               2.5
                                                                                                                    hi
                                                                                                                     ft

                                                                                                                                                                                                                  (O III)
                                                                                                                    0.
                                                                                                                     60

                                                                                                                                                                              Lyα                      (O II)    Hβ
                                                                                                                                                                                                                                  Hα
                                                                                                                             0.

                                                                                                                                                                                                                                                               Optical
                                                                                                                                 30

                                                                                                                                                                                                                                                               Spectrographs
                              MOONS                                                                                                                                                                          Gb                                                z = 1.5
                                                                                                                                                                                               Mg I         Bδ
                                                                                                                                                                                                                                             CaT
                                                                                                                                                                                               Mg II      H,K

                                                                                                                                                                                    0.5                    1                1.5          2               2.5
                                                                                                                                 31
                                                                                                                            3.

                                                                                                                                                                                                       (O III)
                                                                                                                     e 58
                                                                                                                            )
                                                                                                                         yr

                                                                                                                                                                                                   Hβ
                                                                                                                t i m 5.
                                                                                                                      (G

                                                                                                                                                                                    (O II)
                                                                                                                                                                                                                             Hα
                                                                                                                ck
                                                                                                           ok 8
                                                                                                         lo 7.1
                                                                                                             ba
                                                                                               34
                                                                                             8.

                                                                                                                                                                                                                                                               SDSS at
                                                                                      19

                                                                                                                                                                                              Gb                                                               z = 0.1
                                                                                    9.

                                                                                                                                                                                             Hδ
      Survey              Redshift                                                           Volume                  #Objects                                      Fe II Mg I
                                                                                                                                                                                                                                                   CaT
                                                                                            (h – 3 Mpc 3)                                                             Mg II            H,K
       SDSS              0 < z < 0.2                                                          1 × 10 8                    10 6
     MOONS              0.8 < z < 1.8                                                         5 × 10 7               2.5 × 10 6                                            0.3           0.4            0.5           0.6          0.7       0.8         0.9
                                                                                                                                                                                                                   λREST (µm)

Figure 2. A medium-deep survey by MOONS at z > 1                                                                survey. As shown by the top right panels, the crucial                                            redshifted out of the optical range) and gained the
will provide a large number of spectra of similar qual­                                                         redshift range 1.5 < z < 2.5, encompassing the peak                                              nickname “redshift desert”. As shown MOONS
ity and over the same restframe wavelength range                                                                of star formation, has proved to be the hardest to                                               will cover this gap and properly trace the evolution
and co-moving volume as the low-redshift SDSS                                                                   explore spectrally (because the major features are                                               of galaxies throughout the redshift desert.

12             The Messenger 145 – September 2011
Figure 3. Left: The redshift–
                                                                                        MOONS 150 sq.deg.                             space correlation function for
                                                                                1       BOSS                                          the 2dFGRS, ξ(σ,π), plotted as
              20                                                                        VIPERS                                        a function of transverse (σ)
                                                                                        HETDEX                                        and radial (π) pair separation at
                                                                                                                                      z < 0.3 from the 2dF galaxy
                                                                                                                                      redshift survey (Peacock et al.,
                                                                                                                                      2001). This plot clearly displays
                                                                              0.8                                                     redshift space distortions, with

                                                          Growth rate fg(z)
                                                                                                                                      “fingers of God” elongations
π/h –1 Mpc

                                                                                                                                      on small scales and coherent
               0
                                                                                                                                      Kaiser flattening at large scales,
                                                                                                                2dFGRS
                                                                                                                                      the signature of the growth rate
                                                                                                                SDSS – LRG
                                                                              0.6                                                     of structure on galaxy cluster­
                                                                                                                VVDS
                                                                                                                                      ing measurements. Right:
                                                                                                                WiggleZ
                                                                                                                                      Comparison of growth rate-
                                                                                                                                      measurements, fg(z), for cur­
                                                                                                                                      rently available measurements
             – 20                                                                                  ΛCDM: Ωm = 0.325, Λ = 0.675
                                                                                                                                      (solid symbols, with 2dFGRS,
                                                                              0.4                  ΛCDM: Ωm = 0.225, Λ = 0.775
                                                                                                                                      SDSS-LRG, WiggleZ and
                                                                                                   ΛCDM: Ωm = 0.275, Λ = 0.725
                                                                                                                                      VVDS) and to projected meas­
                                                                                                                                      urements (open symbols) of
                    – 20        0               20                                  0      0.5       1          1.5           2       ongoing surveys (BOSS,
                           σ/h –1 Mpc                                                                Redshift                         VIPERS and HETDEX). Open
                                                                                                                                      triangles show the prediction
                                                                                                                                      for the growth rate measure­
                                                                                                                                      ment that will be obtained with
The first galaxies                              consists of currently unexplained dark
                                                                                                                                      MOONS using ~ 1 million gal­
                                                energy and dark matter, and less than                                                 axies over 150 square degrees.
The shining of the first galaxies, just a few   4 % is in the form of baryons. Under­                                                 No other ground-based survey
hundred million years after the Big Bang        standing the nature of these dark compo­                                              is able to probe the redshift
                                                                                                                                      range considered by MOONS.
(at redshift 7 < z < 12) is of enormous         nents — which dominate the global
importance in the history of the Universe       expansion and large-scale structure of
since these first galaxies hold the key         the Universe — is amongst the most
to furthering our understanding of cosmic       ­fundamental unsolved problems in sci­                           MOONS INSTRUMENT PERFORMANCE
reionisation. Although recent advances           ence. Complementary to other spectro­
obtained by deep NIR imaging have been           scopic surveys at z < 1 (e.g., Vipers,                          Telescope                   VLT
dramatic, very little is known about when       BOSS, W   ­ iggleZ, BigBOSS), the capabili­                      Field of view               500 sq. arcmin.
and especially how this re-ionisation           ties of MOONS will allow us to con-                              Number of targets           500 objects + 500 sky
­happened. The unique combination of            strain the cosmological paradigm of the                          Wavelength                  0.8(0.5)–1.8 μm
 8-metre aperture, wide area coverage           Λ Cold Dark Matter model by determin-                            Resolutions                 Medium = 5000
 and NIR spectroscopy (key since at z > 7       ing the dark matter halo mass function                                                       High = 20 000
 even the Lyα line is shifted to λ > 1 μm)      and obtain crucial constraints on the
 offered by MOONS, will p  ­ rovide accurate    nature of dark energy and gravity via
 distances, relative velocities and emis-       detailed measurements of the growth rate                         both a medium resolution (R ~ 5000)
 sion line diagnostics, without which the       of structure at z > 1, extending previous                        mode and a high-resolution (R ~ 20 000)
 power of these photometric surveys              determinations, such as that by the 2dF                         mode to allow detailed dynamical and
 is severely limited. The capabilities of        galaxy redshift survey at z < 0.3 (Peacock                      chemical studies. Such characteristics
 MOONS will give us the first realistic          et al., 2001) and shown in Figure 3.                            and versatility make MOONS the long-
 chance to perform a systematic, wide-                                                                           awaited workhorse NIR multi-object
 area spectroscopic study of the very high                                                                       spectrograph for the VLT, which will per­
 redshift galaxies and establish the phys­      Instrument specifications                                        fectly complement the optical spectros­
 ics of reionisation.                                                                                            copy performed by FLAMES and VIMOS.
                                                To address such fundamental science
                                                questions MOONS will exploit the full 500
Cosmology                                       square arcminute field of view offered                           References
                                                by the Nasmyth focus of the VLT and will                         Peacock, J. et al. 2001, Nature, 410, 169
Over the last two decades several obser­        cover the wavelength range 0.8 μm–1.8 μm,                        Recio-Blanco, A., Hill, V. & Bienaymé, O. 2009,
vational keystones have considerably            with a possible extension down to 0.5 μm.                        	Proc. French Society of Astron. & Astrophys.
changed our knowledge of the Universe.          A new pick-off system will allow a fast                            SF2A-2009
Measurements of the cosmic microwave            positioning of the fibres and the observa­
background, high-redshift supernovae            tion of 500 targets simultaneously, each                         Links
and large-scale structure have revealed         with its own dedicated sky fibre for opti­
                                                                                                                 1
that 96 % of the density of the Universe        mal sky subtraction. MOONS will have                                 MOONS: http://www.roe.ac.uk/~ciras/MOONS.html

                                                                                                                 The Messenger 145 – September 2011                 13
You can also read