CFHT, Instruments,
Spectroscopy,
OASIS, Instrument
Overview


Welcome to the world of OASIS and... Enjoy!

The first engineering run at CFHT (photo1, photo2) was completed in April 1997 although very bad weather conditions did not allow any astronomical observations. But on August 10th, OASIS saw its first light at CFHT! During this run, numerous mechanical and optical tests were performed for the f/20 mode and the software for data acquisition was implemented. In January 1998, two engineering nights, used to install a more elaborated user's interface, were followed by four nights of commissioning by a team of external experts (photo3). Tests performed with the upgraded Gumball calibration system revealed a clear improvement in the exposure times needed to obtain good calibration frames. During that period, the data reduction software was also locally implemented and a preliminary reduction performed by the observers was very successful. This software, entirely supported by Lyon, became available for different platforms worldwide in March 1998.
Many observing runs were scheduled for the end of March 1998. Although the observations were again affected by periods of very bad seeing, good science data have been obtained. Two nights of engineering were also used to test the instrument in the f/8 mode and a new beamsplitter for the AOB. This beamsplitter considerably improved the total efficiency of the instrument in the I-band. OASIS has been used in November 1998 (again during bad whether conditions) and in December 1998. During this last run, atmospheric conditions were finally very good and spectacular data were gathered on diverse objects (T Tauri stars, proto-stellar disks in the Orion nebula, M31 nucleus, AGNs, etc.). In 1999, many runs with OASIS were again compromised by bad weather but some nights were also extremely productive. At the beginning of 2000, a long 20 nights run has been very successful.
Despite the fact that OASIS was designed to support six observing modes, only two (imaging and TIGER) will be available for the current year. Further implementation of the other modes is under study at the moment.
In time of writing (June 2000), six new filters have been delivered allowing more spectral configurations. New beamsplitters (V and R bands) have also been delivered and are available for the observations. These devices result in an increase of the performance of OASIS by a factor of 2 in most spectral ranges! Finally, a new 2k x 4k CCD, EEV1, is now available for the visible configurations of OASIS (below 7000 Ang.). This device again improves the performance by a factor of 2, making OASIS a superb instrument for 2D spectroscopy of very faint structures.
OASIS is the result of many years of dedicated work by the Lyon team, supported by the CFHT staff. A list of all the people involved in this project can be found here.

OASIS is a multi-mode spectro-imager, working in the 0.43 µm
to 1 µm range and using a CFHT 2kx2k 15µm pixels
CCD (i.e. Loral3) or 2kx4k 13.5µm pixels (EEV1). It is operated
as a CFHT "guest" instrument. OASIS normally
make use of the corrected 90 arcsec diameter F/20 field given by the CFHT
Adaptative Optics Bonnette. It can also be used at the direct F/8 Cassegrain
focus as a backup mode and for science programs necessiting integral field
spectroscopy but with a coarser spatial sampling defined by the natural
seeing. (Note: This mode has now been fully tested. It is then
VERY important to bring a backup program in case of seeing worse than 1.2",
value for which the AO correction becomes inoperative. ).
For now, OASIS can be operated in the following modes:
This multi-mode/configuration approach has been chosen:
Due to the high complexity of the instrument, a special user's interface has been implemented in the current Pegasus sessions at CFHT. Instead of selecting the optical elements needed to achieve a specific optical configuration, the observer defines instead an observing ``scenario'' for which he/she specifies the specific instrumental requirements for the science program (e.g. spectral range, sky sampling, resolution)(form1, form2). Different optical elements are then moved automatically by software to achieve an instrumental configuration fulfilling these specifications.
Pointing Limits: OASIS being a long instrument, there are some
pointing limits to be taken into account while planning your observations.
These limits are implemented in the TCS software so collisions with the
telescope pier will be automatically avoided but some objects in your program
might not be accessible at all with OASIS! With Loral3 as the detector,
the pointing limits in declination are +67d59'15" and -35d54'49".
With the EEV1 detector, the limits are more severe because the dewar is
longer: +62d and -28d.
Detectors: Two detectors, Loral 3 and EEV1, are available for
OASIS, depending of the spectral range required for a science program. Loral3
is a thick 2k x 2k device with a very moderate quantum efficiency but remains
the detector to be used for programs requesting the red spectral domain
(that is, over 7000 Ang). Its characteristics can be found
here. The EEV1 is
a thinned 2k x 4.5k device with very
good quantum efficiency and low readout-noise, ideal for the visible range
of OASIS (i.e. 4200 - 7000 Ang). It should not be used for the red domain
because fringing is very important at about 35% at 8500 Ang.
Its characteristics can be found
here.
Another significant difference between both detectors is the size of the
pixels. Loral3 has 15µm pixels while EEV1 has 13.5µm pixels,
that is, 10% smaller. This results in a different spectral resolution
in the spectroscopic configurations, smaller field in one direction for the
EEV1, and different pixel scales for the imaging mode. These are noted in
the configuration tables below.
The readout time for Loral3 is about 165 seconds. For EEV1, it is about
50 seconds (raster of 2k x 2.5k, useful for OASIS).

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| Name | Grism | Useful wavelength limits | Dispersion Å/pixel |
Resolving power |
AOB beamsplitter |
|
|---|---|---|---|---|---|---|
| Lambda inf (Å) | Lambda sup (Å) | |||||
| LR2 | R150 | 8650 | 10370 | 4.74 | 1000 | I |
| Name | Grism | Useful wavelength limits | Dispersion Å/pixel |
Resolving power |
AOB beamsplitter |
|
|---|---|---|---|---|---|---|
| Lambda inf (Å) | Lambda sup (Å) | |||||
| MR0 | O300 | 4150 | 4930 | 2.13 | 1059 | 50-50 |
| MR1 | O300 | 4760 | 5558 | 2.15 | 1210 | V |
| MR2 | R300 | 6210 | 7008 | 2.17 | 1525 | R |
| MR3 | R300 | 8346 | 9152 | 2.23 | 1965 | I |
| MR4 | O300 | 5502 | 6324 | 2.16 | 1375 | R |
| MR5 | R300 | 6940 | 7764 | 2.19 | 1710 | R |
| MR6 | R300 | 7685 | 8455 | 2.21 | 1880 | I |
| MR7 | R300 | 9150 | 9896 | 2.25 | 2220 | I |
| Name | Grism | Useful wavelength limits | Dispersion Å/pixel |
Resolving power |
AOB beamsplitter |
|
|---|---|---|---|---|---|---|
| Lambda inf (Å) | Lambda sup (Å) | |||||
| HR1 | B600 | 4852 | 5196 | 0.99 | 2530 | V |
| HR2 | B600 | 5118 | 5484 | 1.00 | 2650 | V |
| HR3 | O600 | 6209 | 6549 | 0.99 | 3215 | R |
| HR4 | O600 | 6492 | 6838 | 1.00 | 3335 | R |
| HR5 | R600 | 8435 | 8749 | 0.87 | 4295 | I |
1) Note that the dispersion is smaller by 10% if the EEV1 is used.
2) Note that the resolution is lowered by about 10% if the f/8 focus - 0.4" sampling is used.
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