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CCD News (1Jun92) (from CTIO, NOAO Newsletter No. 30, 1 June 1992) In June we will begin the conversion from operating our CCDs with the VEB controllers to using the new Arcon controllers. This change-over process will continue for some 18-24 months by which time all our CCDs and some of the IR arrays will be operated by the Arcons, and much ancient hardware (VEBs, LSIs) and software (Forth) will have been retired. As far as the CCDs are concerned, the conversion is complicated by the VEBs being telescope-based whereas the Arcons are dewar-based. Thus, if we wish to retire a VEB off some specific telescope, we must ensure that all the CCDs we want to use on that telescope are first converted to Arcons, or else accept some smaller number of options. In addition, we do not want to impair significantly the rate at which we are able to commission new detectors, since over this period we are expecting another Tektronix 2048, a Reticon 1200 x 400, and several Loral CCDs. As we proceed, we will retire the last of our EEV (GEC) CCDs and the Thomson 1024s. At the moment, we are operating a Thomson CCD at the Schmidt telescope (see Newsletter No. 29, page 15) with the prototype Arcon 2.1. This system is being shared for development work, but shortly the R&D will move to Arcon 3.1, which will also use a Thomson CCD. The latter will be a lab system only, employed for testing and verifying boards for the Arcons as they are produced. Arcon 3.2 will operate a Tek 1024, and Arcon 3.3 a Tek 2048. Both these CCDs have four low noise amplifiers and will benefit greatly from the quad readout capability of the Arcons. The change-over will also eliminate the difficulty of operating these mega-pixel arrays with the LSI 11/73 computers. Arcon 3.4 is destined for the NICMOS III HgCdTe IR array. As soon as Arcon 3.2 is operating, we will retire the 0.9-m VEB, which will then become a spare for the VEBs remaining at the 1.5-m and 4-m telescopes. As a consequence, for a period of about two months next semester the Tek 1024 CCD will be the only CCD available at the 0.9-m, except for programs where U band sensitivity is paramount or where there is a clash with the 1.5-m or 4-m schedules. For these cases we will schedule the Thomson CCD from the Schmidt. We will try to juggle the 0.9-m schedule with the exact date of the VEB removal so that there is as little conflict as possible with people's programs. At the end of this two month period, the Tek 2048 will have also been converted to use an Arcon and will thus become available at the 0.9-m. However, users should be aware that TI and Tek 512 CCDs will not be usable at the 0.9-m for at least a year. We are sure that present users of the Tek 512 will be more than happy with the Tek 1024/2048 due to the much improved region-of-interest handling and the quad readout compensating for the longer readout time of the bigger CCDs. The TI CCDs are presently only used for the few programs where the U band sensitivity is of the utmost importance. There will unfortunately be a period of time where we will not be able to offer a CCD at the 0.9-m which has as good a UV QE as the TIs. Nearer the change-over time we will be contacting any observers who have requested a different CCD from the one which we will actually be scheduling. Alistair Walker
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