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ACS Instrument Handbook Cycle 19
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Advanced Camera for Surveys Instrument Handbook for Cycle 19 > Chapter 5: Imaging > 5.6 ACS Point Spread Functions

5.6 ACS Point Spread Functions
The ACS point spread function has been studied in ground test measurements, and by using on-orbit data and models generated by the Tiny TIM software (http://www.stsci.edu/software/tinytim/) developed by J. Krist and R. Hook. As with other HST instruments, the ACS point spread function is affected by both optical aberrations and geometric distortions. Point sources imaged with WFC and HRC experience blurring due to charge diffusion into adjacent pixels because of CCD subpixel variations, which reduces the limiting magnitudes that can be reached by WFC/HRC. The SBC PSF and the long-wavelength HRC PSF are also affected by a halo produced by the detectors themselves.
5.6.1
The sharpness of the CCD PSF is somewhat degraded by charge diffusion into adjacent pixels. The effect is usually described in terms of the pixel response function (PRF), which gives the distribution of flux from within the pixel into adjacent pixels. Charge diffusion results in ~0.5 magnitude loss in the WFC limiting magnitude at short wavelengths (the worst case). At longer wavelengths and at all wavelengths for the HRC the reduction in the limiting magnitude is ~0.2 magnitudes or less. Due to variations in the CCD thickness, charge diffusion is not constant over the field of view. At different wavelengths, the CCD pixel response functions can be represented by the following kernels (for the center of the field):
Figure 5.10: Kernels representing CCD pixel functions for HRC and WFC.
at λ = 4000 ,
at λ = 5500 , and
at λ = 8000 .
 
More details on ACS CCD charge diffusion are given in ACS ISR 2006-01. For details on CTE-induced photometric losses for ACS/WFC and techniques to correct for them, see ACS ISR 2006-01.
5.6.2
Table 5.9 and Table 5.10 give ACS model PSFs in the central 5  5 pixel region in two wavelength bands (filters). Numbers listed are the fraction of the total energy received in each pixel. The models have been generated using Tiny TIM, taking into account the HST optical aberrations and obscurations as well as the CCD pixel response function. Field dependent geometrical distortions are included. The real PSF will also differ from the model because of the jitter in the HST pointing, HST focus variation (focus breathing), and other instrumental effects, some of which are briefly discussed below. For further details on the PSF variations and an effective procedure to model them, see ACS ISR 2006-01.
Table 5.9: Model ACS CCD PSFs.
Table 5.10: Model ACS SBC PSFs.
5.6.3
In general, the ACS channels encircled energy distribution has been found to be within the original instrument specifications. Figure 5.11 and Figure 5.12 show the ACS encircled energy curves derived from on-orbit images. Tabulated values of the encircled energy for most filters are available in Sirianni et al. 2005 (PASP 117, 1049).
Due to telescope breathing over short time scales and focus drifts over long time scales, uses are encouraged to measure the encircled energy directly from their science images, rather than depending on the tabulated values, where deviations at small radii may be significant.
5.6.4
Geometric distortions produce a significant impact on the shape of the PSF in all three of the ACS channels, as can readily be seen in Figure 5.13 and Figure 5.14, which display WFC and HRC PSF images. The log stretch enhances the spider diffraction patterns, which the distortion renders non-perpendicular, and the outer Airy rings, which appear elliptical. The distortion owes primarily to the tilt of the focal surface to the chief ray at the large OTA field angles of the ACS apertures. The linear, field-independent approximation for the WFC produces a difference in plate scale of about 8% between the two diagonals of the field and, in the HRC and SBC, about a 16.5% difference in scale between orthogonal directions rotated about 20 from the aperture edges. Field-dependent distortions, measured as actual vs. predicted distances from field center, amount to about 2% peak in the WFC and about 1% in the HRC and SBC. The distortion solutions are stable following the WFC repair.
The distortions render the pixels, as projected on the sky, trapezoidal in shape and their area varies over the field by about 19% and 3.5% in the WFC and HRC/SBC, respectively. These variations have significant ramifications concerning appropriate techniques for flat-fielding and photometric calibration, especially when complicated by resampling in order to combine dithered image sets. Related issues are the manner in which the halation effects of the HRC and SBC detectors are removed and the treatment of spectra from the prisms and grism, which are not subject to the same distortion effects.
More details concerning geometric distortions in ACS can be found in ACS ISR 2002-02, ACS ISR 2004-15, ACS ISR 2007-08 and ACS ISR 2008-02. An introduction to calacs, is available in the ACS Data Handbook which is posted on the STScI ACS Web page. Information about multidrizzle, which applies corrections for geometric distortion, is available on-line at:
http://drizzlepac.stsci.edu
Figure 5.11: Encircled energy for the CCD channels.
Figure 5.12: Encircled energy for the SBC.
Figure 5.13: ACS WFC PSF - F625W.
Figure 5.14: ACS HRC PSF - F625W.
5.6.5
The CCDs used in the HRC and WFC suffer from a halo that is caused by very red photons passing through the device and being scattered back into the detector by the mounting substrate. This creates a large halo in HRC images beyond 7000  and WFC images past 9000 . At 8000  in the HRC, the halo contains about 10% of the light. At 10,000 , it contains about 30% and increases the surface brightness of the PSF wings by over an order of magnitude, overwhelming the PSF diffraction rings and spikes. A discussion of this may be found in Gilliland & Riess 2002 (HST Calibration Workshop) at:
http://www.stsci.edu/hst/HST_overview/documents/calworkshop/workshop2002/CW2002_Papers/gilliland.pdf
In the F850LP filter, in particular, extremely red stars show a progressive loss of flux in small to moderate sized apertures as a function of color. Additional information can be found in Sirianni et al. 2005, PASP, 117, 1049 and ACS ISR 2007-06. These papers provide a detailed recipe to correct for this effect. This halo effect is only partially treated by the Exposure Time Calculator. Observers can use synphot1 (see Section 9.3.2) to accurately calculate the photometry of red sources in the SDSS z-filter.
Long wavelength photons that pass through the CCD can also be scattered by the electrode structure on the back side of the device and will create two spikes that extend roughly parallel to the x-axis. These spikes are seen at wavelengths longer than 9500  in both the HRC and WFC (see Figure 5.15 and Figure 5.16).
Figure 5.15: ACS WFC PSFs (10" x 10"). FR914M images are saturated.
Figure 5.16: ACS HRC PSFs (3.25" x 3.25").
In the UV the core of the PSF becomes rather asymmetrical due to midfrequency optical surface errors. In the SBC, a halo is created by charge migration at the microchannel plate surface. This effect, seen previously in STIS MAMA images, broadens the PSF core and redistributes a small portion of flux into a broad halo that can be approximated by a Gaussian with FWHM ~20 pixels. The peak flux for a point source centered on a pixel is reduced by 30% to 40% depending on wavelength.
The encircled energy curves presented in this handbook and incorporated into the ETC include all of the scattering effects discussed here.
5.6.6
Residual aberration levels at the center of the field in each camera are 1/30 wave (HRC) and 1/20 wave (WFC) rms at 5500  (excluding defocus). Coma and astigmatism are minimized at the field center of each camera. The ACS PSF varies far less over the field of view than those of WFPC2 and STIS. WFPC2 especially suffered from a variable obscuration pattern that significantly altered the PSF structure depending on field position. Lacking the additional obscurations present in WFPC2, ACS PSF variations are instead due to changes in aberrations and charge diffusion.
At the extreme corners of the WFC field, increased astigmatism slightly elongates the PSF core. The axis of elongation rotates by 90 if the system passes through focus due to breathing. This may affect ellipticity measurements of small galaxies with bright cores at the field edges. Focus variations in the WFC, which alter the amount of light in the peak, are largely due to detector surface height irregularities and amount to the equivalent of 5 microns of breathing (1/18 wave rms). The largest focus offset is along the gap between the two CCDs. Variations in the width of the PSF core are dominated by changes in CCD charge diffusion, which is dependent on the thickness of the detector (12 to 17 microns for the WFC). The PSF FWHM in F550M, for example, can vary by 20% (0.10 to 0.13 arcseconds) over the field. More information about the dependence of the WFC PSF on OTA temperature and breathing is provided in ACS ISR 2007-12 and ACS ISR 2008-03.
The PSFs in the HRC and SBC are reasonably constant over their fields. The HRC FWHM is 0.060 to 0.073 arcseconds in F550M. More details on ACS PSF field variations are provided in ACS ISR 2003-06. The Tiny Tim PSF simulator includes field dependent aberrations and charge diffusion and may be used to estimate the impact of these variations. Information about the dependence of the WFC PSF on OTA temperature and breathing is provided in ACS ISR 2007-12 and ACS ISR 2008-03.

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