There is currently more data available to astronomers than can be efficiently used. With the increasing complexity of instrumentation and the limited opportunities observers have to use instruments, reduction and analysis tools are the key to getting observations published, indeed reduction and analysis should be part of the instrument design (Bohannan, 2001). With such a backlog of data there is increasing pressure for observatories to supply pipe-line reduction (see Greimel et al., 2001).
Generally inherent in any automated procedures written will be the stage of “human intervention”, where it is far quicker and easier to manually interact with the reduction process than engineer software to carry out the same process, even though this quicker process may take weeks to accomplish. Even those astronomers who have the programming skills necessary to create such a complex package are resistant to do so due to the foreseeable time constraints in such an undertaking, which takes time away from their scientific research.
The model offered for pipe-line processing of the ING Wide Field Survey (WFS) images (Irwin and Lewis, 2001) is a model for all observations obtained in a standardised fashion (Bohannan, 2001). As such the following section will explore and contrast the infrastructure of the ING WFS PL with that of the LT PL.
The ING WFS PL is based on IRAF routines. The pipe-line is essentially a series of pipes linked together in a modular way to form the PL. This modular way of creating a software package increases the upgrade-ability and robustness of the PL. Any pipe can be rewritten and replaced without the rest of the PL being effected. This modular infrastructure is also the basis that the LT PL has been built around, it allows for much greater flexibility, upgrading the system is also easier when done in this modular fashion.
The camera used on the ING WFS has a mosaic of 5 CCDs with a current readout time of around 160s, which in practical terms leads to a dead-time of around 3mins between exposures. A typical nights data is between 5 and 10Gbytes of data, all of which must be transfered to the Institute of Astronomy, Cambridge, on DAT tape for reduction.
The LT contains only one CCD which produces an 8 Megabyte file per readout, Bode (1995) maintains that there could be several hundred such frames each night giving upwards of 5 Giga-bytes of data. This data will be reduced at the LT site leaving only a series of text files as the fully reduced data which can be efficiently transfered electronically (see McNerney and Steele, 2000).
Although most of the ING WFS processing is automatic, creating updating and maintaining master flats is difficult if not impossible to automate as there is no direct control over the survey, however flat-fields have been found to be stable for periods of around 1 week. (Irwin and Lewis, 2001).
The LT will also maintain a library of flat-field images, however algorithms developed at the Astrophysics Research Institute in Liverpool will allow these calibration frames to be automatically generated and updated.
The data processing system of the ING WFS is heavily dependent on the integrity of the FITS headers. They are also a repository of information derived and generated by the processing stages. We cannot emphasise enough the vital importance of following this information for automated PL processing (Irwin and Lewis, 2001).
This method of extracting information and recording necessary data to file is also used in the LT PL, with the name of each calibration file recorded to the FITS header. It this way it is possible to accurately repeat the reduction of data files at a much later date than it originally occurred.
The ING WFS PL follows these stages:
This effect has not, to date, been noticed on the LT bias frames, therefore a simple bias level subtraction will be used, however the capability exists to do full 2D bias removal should it become necessary.
The LT CCD has been tested and shown to be linear to >> 99% (Pittock, 1998), non-linearity therefore will not be an issue.
Time constraints for creating flat-fields will also affect the LT, however the scheduling algorithms will take into account the number of different filters to be used each night as part of its calculation, it is expected therefore that flats for each necessary filter will be observed each night. However with flat-fields being stable for ~ 1 week, the scheduler will ensure that flat-fields are taken for any filter, for which a flat has not previously been taken, within this time-scale.
The LT PL will create de-fringing frames for each image that requires it, the de-fringing being carried out using the techniques discussed in Section 2.4.4.
This technique is the same as that used in the LT PL, however the zeroth order WCS gained from the telescope pointing will be accurate to < 2arc-secs. The catalogue used to create a more accurate WCS will be the USNO-A2.0 (see Monet, 1998).
This process will also be used by the LT PL however, whilst initially the LT will use Landolt (1992) standards there will also be a catalogue of LT standards built up with the aim of improving accuracy.