10.1 Introduction

Both the FUV XDL and the NUV MAMA detectors are subject to damage or destruction by excessive illumination. An excessive local count rate can permanently reduce the sensitivity of the affected detector region. The most likely causes are a bright spectral emission line (XDL or MAMA) or a bright source observed in direct imaging (MAMA). A global over-illumination of the detector can result in its loss. To protect the detectors, onboard software monitors the local and global count rates. It shutters the instrument in case of a local violation and lowers the high voltage if a global count-rate violation is detected. The local rate is checked before an exposure is begun, while the global rate is monitored continuously during the exposure. Under certain circumstances damage can result despite the onboard safety measures, and in any event lowering the high voltage will disrupt the HST schedule and operations. Therefore, all proposed COS observations must meet count-rate screening limits with safety margins to allow for uncertainties. COS is currently the only HST instrument to use UV detectors for target acquisitions. Such acquisitions must be screened, as well, including special procedures for imaging acquisitions of extended sources; see Section 8.10.2. It is the responsibility of the observer to screen all proposed targets and fields during Phase II preparation, and of STScI to check and enforce these limits. The COS Bright Object Protection (BOP) policies and procedures are described in this chapter.

Table 10.1: COS Count-Rate Screening Limits.

DetectorSource typeType of limitLimiting count rate (counts/s)

FUV

predictable

global

15,000 per segment1

local

0.67 per pixel2

irregular

global

6,000 per segment1

local

0.67 per pixel2

NUV

predictable

global

170,000 (imaging) or 30,000 per stripe (spectroscopic)1

local

50 per pixel3 (imaging) or 70 per pixel (spectroscopic)

irregular

global

68,000 (imaging) or 12,000 per stripe (spectroscopic)1

local

50 per pixel (imaging) or 70 per pixel (spectroscopic)

1 The global data-rate limit for observations using TIME-TAG mode is 30,000 counts/s, as discussed in Section 5.2.1.

2 This local count-rate screening limit is not applicable to the 1055 and 1096 cenwaves of the COS G130M grating. For these modes the limiting count rate is 0.2 count/s/pixel for both source types.

3 For imaging acquisitions, a count rate of 360 count/s in the 9 × 9-pixel box surrounding the target (as computed by the COS Imaging Acquisition ETC) represents an equivalent safe upper limit.