LIRIS
Long-slit Intermediate Resolution Infrared Spectrograph for the WHT |
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LIRIS is an Instituto de Astrofísica de
Canarias (IAC) project that consist a near-infrared (0.9-2.4 microns) intermediate
resolution spectrograph (R=1000-3000), conceived as a common user instrument
for the WHT at the Observatorio del Roque de los Muchachos (ORM La Palma).
LIRIS will have imaging, long-slit and multi-object
spectroscopy, coronography and polarimetry working modes. Coronography
and polarimetry, will be upgrades not available at first phase. Image capability
will allow easy target acquisition.
The optical system is based on a classical collimator/camera
design. Grisms are used as the dispersion elements. The plate scale (0.25
arsec/pixels) matches the median seeing (0.5
arcsec in the K band) at the ORM. The detector is a Hawaii 1024x1024 HgCdTe
array operating at 65 K.
The collected light beam passes through a fused Silica window. The telescope focal plane lays inside the cryostat, where the cold aperture masks are located.
OPTICS MECHANICS MECHANISM CONTROL DETECTOR SOFTWARE
OPTICS
The optics of LIRIS are all refractive, with the exception of a single folding flat mirror in the collimator assembly. The expected throughput (averaged across the wavelength range) for the optics is 80% and 64% in imaging and spectroscopic modes, respectively. The grism transmission is assumed to be 80%.
- A slit wheel is introduced at the telescope focal plane for spectroscopy.
- A refractive collimator forms an image of the primary mirror near the last element and produces a collimated beam where the filters, grisms and Wollaston prisms are inserted.
- A cold stop: The entrance pupil of LIRIS is the primary mirror of the telescope, given the fact that the secondary is oversized with respect to the primary in the WHT, contrary to an optimized infrared telescope.
- The collimated beam passes through the pupil.
- A refractive camera is used to focus the light onto the detector.
The mechanical design is based on a modular concept, integrated by the following modules: the aperture wheel (slit wheel), the collimator assembly, the central wheel assembly (formed by two filter wheels, the pupil wheel and the grism wheel), the camera wheel and finally the detector assembly with its focusing mechanism.
Slit wheelCollimator Pupil wheel Camera LIRIS schematic of the optical train (provided by UKATC/ROE)
The slit wheel contains 16 positions:
1 blank position, 5 long slits (widths 0.65”, 0.75”, 1”, 2.5” and 5” )
plus 10 multislit positions.
The two filter wheels contains 12
positions each, and will hold the filters and the Wollaston prisms.
The pupil wheel contains 12 positions
and will hold the pupil masks, plus an optional apodization mask with rotation
mechanism for coronography capabilites.
The grims wheel has 10 positions for grisms.
The camera wheel will carry the camera
and the optics to image the reimage the pupil onto the detector plane.
The detector will be mounted in a cold translation
mechanism (focus mechanism) to compensate for non-achromaticity
along the observing spectral range.
The vacuum vessel is a welded cylindrical vessel.
It is made in three sections, a central ring and two end covers. The front
cover is a circular plate which carries the window and its mounting and
a cover over the port giving access to the entrance wheel. It is not necessary
to remove the front cover to change focal plane masks. The rear cover could
be removed to gain access to all the other internal modules of the instrument.
It has an auxiliary access port to facilitate the first integration &alignment
steps without detector.
The center section carries all the semi-permanent
access ports. These carry ports for electrical wiring, cooling and vacuum
pumping
The optical bench is an aluminium welded structure,
supported from the front ring of the central section of the vacuum vessel
by three trusses made from G10 glass-epoxy composite. It has a cylindrical
shape and its plates acts as a reference surfaces and mounting for all
the cold modules. The bench will be also used as a tank for LN2 for pre-cooling
the instrument. The front plate supports the entrance wheel. The rear plate
supports the rest of the cold parts. The optical bench is fitted with a
panel heater to allow a controlled warm-up while still under vacuum.
The instrument is precooled with LN2, and the cooling system is a closed-cycle refrigerator (CTI model 1050C), which works on the Gifford-McMahon cycle. There two stages which provides cooling powers of 45W at 60K and 4W at 15K. The first stage cools all the internal parts, except for the detector and its housing. The second stage mantains cool the detector at the working temperature of 65K. The detector temperature is stabilized using the commercial PID controller Lakeshore 340.
External schematic view
The LIRIS mechanism are driven by cryogenic stepper motors. The control system is based on a VME system with a Motorola CPU card running VxWorks operating system and two Oregon Micro Systems stepper motor controller boards, allowing a total number of twelve motors to be controlled, each one of them with its own home, limits and power off signals. The VME system is connected to the SUN through an Ethernet network and an RS232 line. An additional 19" 3U rack with the motor drivers are installed under the VME rack. The drivers are from the same manufacturer as the motors' Phytron.
MECHANISM CONTROL
An agreement has been established between the IAC and the ING to develop jointly the Mechanism Control Software and the detector control system for the two infrared instruments (LIRIS/IAC and INGRID/ING).
The detector is a Rockwell Hawaii 1024x1024 HgCdTe array. The pixel size is 18.5 mm, which corresponds to a plate scale of 0.25 arcsecond on the sky.The controller system uses the SDSU controller,
which is a commercial product developed by the San Diego State University
(SDSU) and supplied by IRLabs (Tucson, AZ). It is based on the 56200 DSP
by Motorola. The current code was developed by P. Moore of the Isaac Newton
Group for the INGRID project. The detector is read through four channels
at a rate of 3 msecs/pixel, leading to a time
of 0.9 seconds for a complete frame readout. The SDSU controller communicates
with the control computer through optical fibers.
The available read out modes are double correlated
(DC), Multiple non destructive reads (MNDR) and reading up the ramp.
A temperature controller is required due to the
strong dependence of the signal offset level of the detector with
the substrate temperature. For this reason the detector temperature has
to be stabilized below 0.005K. The temperature controller Lakeshore
340 has been selected, which guarantees a stabilization below
0.005K, sufficient to constrain the offset variation to 0.1e- RMS.