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ACS Data Handbook v. 8.0
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ACS Data Handbook > Chapter 1: ACS Overview > 1.1 Instrument Design and Capabilities

1.1
ACS was designed for deep, visible to near-IR imaging and spectroscopic surveys using its Wide Field Channel (WFC), near-UV to near-IR imaging and coronagraphy with its now-defunct High Resolution Channel (HRC), and far-UV imaging and spectroscopy using its Solar Blind Channel (SBC). The WFC's discovery efficiency (i.e., the product of its field of view and throughput) is 10 times greater than that of WFPC2. The failure of ACS's CCD electronics in January 2007 halted its near-UV to near-IR science capabilities until Servicing Mission 4 in May 2009, during which the WFC's functionality was fully restored. Unfortunately, the HRC was not recovered.
ACS comprises three channels, each optimized for specific goals:
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The WFC’s high sensitivity and large field of view make it the preferred camera for deep imaging programs at red and near-infrared wavelengths. By oversampling the HST PSF at λ > 6000 , the HRC was especially useful for high precision photometry in stellar population studies before its failure in January 2007. The HRC's coronagraph was used for detection of circumstellar disks and QSO host galaxies.
1.1.1 Detectors
ACS employs different large-format detectors in each channel:
The WFC and HRC CCDs are thinned, backside-illuminated devices regulated by thermoelectric coolers and sealed in evacuated dewars with fused silica windows. The spectral response of the WFC CCDs is optimized for imaging at visible to near-IR wavelengths. The wavelength coverage of the HRC’s CCD was similar to that of the WFC, but its spectral response was optimized for near-UV wavelengths. As with all CCD detectors, there is read noise associated with clocking and sampling the collected charge in each pixel through the output amplifiers. The dynamic range of CCD images is determined by the read noise and the depth of the pixel well (~85,000 e− for WFC and ~155,000 e− for HRC), which determines the saturation limit of any one pixel. Hot pixels and cosmic rays affect all ACS CCD exposures.
All ACS CCDs produce a time-integrated image in the ACCUM data mode. The HRC also had a target-acquisition mode for coronagraphic observations. The minimum exposure time for WFC is 0.5 seconds and for HRC was 0.1 seconds. The minimum time between successive identical full frame exposures is ~135 seconds for WFC and was 45 seconds for HRC. These times can be reduced to ~36 seconds using WFC subarray readout modes. WFC and HRC observations should be split into multiple dithered exposures to allow removal of hot pixels and cosmic rays in post-observation data processing.
The SBC MAMA is a photon-counting detector that provides two-dimensional imaging optimized for far-UV wavelengths. The SBC is operated only in ACCUM mode. SBC observations are subject to both scientific and absolute brightness limits. At high local (>= 50 counts sec-1 pixel-1) and global (> 285,000 counts sec-1) illumination rates, counting becomes nonlinear in a way that is not correctable. At slightly higher illumination rates, MAMA detectors can be permanently damaged. Lower absolute local and global count rate limits have been imposed that define bright object screening limits for each SBC configuration. Targets that violate these screening limits cannot be observed in the proposed configuration.
1.1.2 Optical Design
ACS has two main optical channels, one dedicated to the WFC and one shared by the HRC and the SBC. These channels are shown in Figures 3.2 and 3.3 of the ACS Instrument Handbook. Each channel has independent corrective optics to compensate for HST’s spherical aberration. The WFC has three optical elements coated with silver to optimize visible light throughput. The silver coatings absorb wavelengths shortward of 3700 . WFC shared two filter wheels with the HRC, which enabled internal WFC/HRC parallel observing for some filter combinations.
The HRC/SBC optical chain comprises three aluminized mirrors overcoated with MgF2. The HRC was selected by inserting a plane fold mirror into the optical path so that the beam was imaged on the HRC’s detector through the WFC/HRC filter wheels. The SBC is selected by moving the fold mirror out of the beam and allowing light to pass through the SBC filter wheel onto the SBC detector. The aberrated beam coronagraph was deployed with a mechanism that inserted a window with two occulting spots at the aberrated telescope focal plane and an apodizer at the re-imaged exit pupil. For health and safety reasons, use of the coronagraph with SBC is forbidden.
1.1.3 Geometric Distortion
ACS’s focal planes exhibit significantly more geometric distortion than those of previous HST instruments. This distortion is principally caused by ACS's optical design, which has a minimal number of components for correcting the spherical aberration induced by the Optical Telescope Assembly (OTA) without introducing coma. The optics allow high throughput, but their focal surfaces are far from normal to the principal rays. The WFC detector is tilted by 22, so its projected diagonals differ by 8%. The HRC and SBC detectors are tilted by 25, so their projected diagonals differ by 12%. Consequently, the projected footprints of the detectors on the sky are rhomboidal rather than square, and the pixel scales are smaller along the radial direction of the OTA field of view than along the tangential direction. The angles between the projected x- and y-axis of the detectors are 84.9 for WFC1, 86.1 for WFC2, and 84.2 for HRC.
Figure 1.1 shows the locations of the WFC and HRC apertures in HST’s V2/V3 reference frame, the rhomboidal projections of each detector, and the locations of the four readout amplifiers (A, B, C, and D) for each channel. A telescope roll angle of zero degrees corresponds to an on-sky view with the V3 and V2 axes aligned north and east, respectively. The orientations of the physical edges of the detectors are approximately parallel with the V2 and V3 coordinate axes of the telescope, but the eigenaxes of the pixel scale transformation of the WFC are along the projected diagonals of the detectors. The situation is even more irregular for the HRC and SBC because the aperture diagonals do not lie along a radius of the OTA field of view. Moreover, the scale and area of WFC pixels vary by ~10% and ~18%, respectively, from corner to corner. For HRC and SBC, the pixels scale by only ~1% from corner to corner because these detectors have smaller fields of view.
The distorted pixel scales and areas must be made corrected before and photometry or astrometry of ACS images is performed. For detailed information about the correction of geometric distortion, please refer to the DrizzlePac Web site.
Figure 1.1: WFC and HRC Apertures Compared with the V2/V3 Reference Frame
The readout amplifiers (A,B,C,D) are indicated on the figure. When ACS images are processed through AstroDrizzle in the OPUS1 data pipeline, the resulting drizzled images are oriented with their x,y axes corresponding approximately to the x,y axes shown in this diagram. Thus, the WFC data products are oriented so that WFC1 (which uses amplifiers A and B) is on top in the positive y-direction (also see Section 2.3), and the HRC images are oriented such that amplifiers A and B are at the top in this diagram.
1.1.4 ACS Performance after Servicing Mission 4
ACS suffered component failures in its Side 1 and Side 2 electronics in June 2006 and January 2007, respectively. Although the latter failure halted operations of the WFC and HRC cameras, the SBC was unaffected by either failure and remained operational throughout this problematic period. The WFC was recovered after the successful installation of a replacement CCD electronics box (CEB-R) and power supply during Servicing Mission 4 (SM4) in May 2009. Unfortunately, further damage to the HRC power harness in January 2007 prevented recovery of the HRC during SM4, so it remains unavailable for scientific use.
Tests conducted shortly after SM4 showed that:
Table 1.1: Comparison of WFC Performance Before the Side 2 Failure and After SM4
Read Noise (e ; gain = 2)
Dark Current (e /pix/hr)
Cross-talk (50Ke source)
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The Operations Pipeline Unified System (OPUS) is the name of the pipeline software that controls the processing and archiving of data at STScI, converting telemetry into FITS data products, populating the Archive catalog, and performing housekeeping on the pipelines. See Section 3.1 for more details.
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stsci_python is a library of Python routines and C extensions that is being developed to provide a general astronomical data analysis infrastructure.


ACS Data Handbook > Chapter 1: ACS Overview > 1.1 Instrument Design and Capabilities

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