2.6 CTE Considerations
Observers should consider the effect of charge transfer efficiency (CTE) losses on their data. These issues and recommendations are discussed in some detail for ACS/WFC and WFC3/UVIS in the CTE White Paper and on the ACS CTE Information webpage. CTE losses can be mitigated using two different approaches: (1) post-processing with either a pixel-based correction algorithm to restore the values of the pixels, or correcting photometry to account for the losses, and/or (2) adjusting the observing strategy to maximize the CTE during the CCD readout process.
For option (1), the CALACS pipeline now employs a third generation pixel-based CTE correction algorithm described in ACS ISR 2018-04 and 2024-07. This routine works well when CTE losses are not severe. Extensive testing has shown that for typical ACS backgrounds (>30 e–), the parallel (y-direction) CTE correction algorithm has a 75% reconstruction accuracy. For very low backgrounds, 90% of the charge can be lost as the CCD is read out, and these large losses cannot be reconstructed. An alternative technique for point sources is to apply the formula provided in ACS ISR 2022-06 to correct the measured photometry for parallel CTE losses as a function of CCD position, background level, source flux, and observation date. This formula is similarly unable to estimate accurate fluxes for objects that have been CTE-trailed beyond detectability. The ACS Photometric CTE Calculator is available to apply this CTE correction formula to measured photometry.
For option (2), there are several strategies that can be employed. The simplest is to place the source near the WFC serial registers (located furthest from the gap between the WFC CCDs) to reduce the number of CCD parallel transfers. This can be accomplished by using the aperture WFC1-CTE
(Table 7.7) and/or a suitable Y POS TARG. If this is not possible (e.g., if the source subtends >5 arcsec), then the observer should estimate the sky background using the information given in ACS ISR 2022-01. Here empirical sky backgrounds are provided for all of the ACS filters as a function of exposure time and compared to Exposure Time Calculator (ETC) estimates. Observers should check that the sky background is above 30 e– for a given exposure time. If the background is lower than this value, observers should consider increasing their exposure times or using a LED post-flash to increase the background. For the latest details and recommendations on ACS/WFC post-flash capabilities, please refer to ACS ISRs 2024-02 and 2018-02.
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ACS Instrument Handbook
- • Acknowledgments
- • Change Log
- • Chapter 1: Introduction
- Chapter 2: Considerations and Changes After SM4
- Chapter 3: ACS Capabilities, Design and Operations
- Chapter 4: Detector Performance
- Chapter 5: Imaging
- Chapter 6: Polarimetry, Coronagraphy, Prism and Grism Spectroscopy
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Chapter 7: Observing Techniques
- • 7.1 Designing an ACS Observing Proposal
- • 7.2 SBC Bright Object Protection
- • 7.3 Operating Modes
- • 7.4 Patterns and Dithering
- • 7.5 A Road Map for Optimizing Observations
- • 7.6 CCD Gain Selection
- • 7.7 ACS Apertures
- • 7.8 Specifying Orientation on the Sky
- • 7.9 Parallel Observations
- • 7.10 Pointing Stability for Moving Targets
- Chapter 8: Overheads and Orbit-Time Determination
- Chapter 9: Exposure-Time Calculations
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Chapter 10: Imaging Reference Material
- • 10.1 Introduction
- • 10.2 Using the Information in this Chapter
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10.3 Throughputs and Correction Tables
- • WFC F435W
- • WFC F475W
- • WFC F502N
- • WFC F550M
- • WFC F555W
- • WFC F606W
- • WFC F625W
- • WFC F658N
- • WFC F660N
- • WFC F775W
- • WFC F814W
- • WFC F850LP
- • WFC G800L
- • WFC CLEAR
- • HRC F220W
- • HRC F250W
- • HRC F330W
- • HRC F344N
- • HRC F435W
- • HRC F475W
- • HRC F502N
- • HRC F550M
- • HRC F555W
- • HRC F606W
- • HRC F625W
- • HRC F658N
- • HRC F660N
- • HRC F775W
- • HRC F814W
- • HRC F850LP
- • HRC F892N
- • HRC G800L
- • HRC PR200L
- • HRC CLEAR
- • SBC F115LP
- • SBC F122M
- • SBC F125LP
- • SBC F140LP
- • SBC F150LP
- • SBC F165LP
- • SBC PR110L
- • SBC PR130L
- • 10.4 Geometric Distortion in ACS
- • Glossary