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Wide Field Camera 3 Instrument Handbook for Cycle 19 - Space ...

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36 Chapter 5: WFC3 Detector Characteristics and Per<strong>for</strong>mance<br />

associated with the normal Poisson distribution of incoming photons. The correction is<br />

theoretically about 1.7 e – /photon at 200 nm, decreasing linearly to 1.0 at 340 nm.<br />

Measurements of ground-based data, however, have indicated that the effect in the<br />

WFC3 chips is much less, 1.07 e – /photon at 218 nm and 1.03 e – /photon at 275 nm in<br />

broadband data (WFC3 ISR 2008-47) as well as monochromatic narrowband data<br />

(WFC3 ISR 2010-11). The cause <strong>for</strong> this is unclear, but may be due to charge sharing<br />

(Janesick, J.R., 2007, “Photon Transfer DM-->λ“, SPIE, Bellingham, Washington, p<br />

45-48).<br />

Given the low level of quantum yield measured in the WFC3 data, neither the QE<br />

curves presented in Figure 5.2 nor the WFC3 Exposure Time Calculator (ETC)<br />

include the effects of quantum yield. The noise distortion from multiple electrons is<br />

not large compared to other contributions to the signal-to-noise ratio in the ultraviolet<br />

(see Section 9.2).<br />

5.4.3 Flat <strong>Field</strong>s<br />

Be<strong>for</strong>e launch, ground-based flats were obtained <strong>for</strong> all UVIS filters at a S/N of<br />

~200 per pixel using an external optical stimulus (WFC3 ISR 2008-12). Because the<br />

overall illumination pattern of the ground-based flats did not precisely match the<br />

illumination attained on-orbit from the OTA, there are errors in these ground-based<br />

flats on large spatial scales. These errors are being measured by per<strong>for</strong>ming stellar<br />

photometry on rich stellar fields that have been observed using large-scale dither<br />

patterns during SMOV and cycle 17. In the SMOV exposures, the rms difference<br />

between the average magnitude of a star and its magnitude in the first pointing varied<br />

from 1.5% to 4.5%, from the long to the short wavelengths (WFC ISR 2009-<strong>19</strong>).<br />

Reference files resulting from the completed analysis of all of the data are expected to<br />

support photometry to ~1% accuracy over the full WFC3 UVIS field of view at<br />

wavelengths longer than 350 nm, and to 2-3% accuracy at UV wavelengths. A<br />

detailed description of the production of UVIS flat field reference files is given in<br />

Section 5.4 of the WFC3 Data <strong>Handbook</strong>.<br />

The latest in<strong>for</strong>mation about UVIS flats can be found on the WFC3<br />

Web site: http://www.stsci.edu/hst/wfc3/analysis/uvis_flats<br />

Figure 5.3 shows examples of bias-corrected ground-based flats <strong>for</strong> two wide-band<br />

filters. Both are displayed with an inverse greyscale stretch chosen to highlight<br />

features; the vignetting in the upper-right corner is not instrument-related but an<br />

artifact of the optical stimulus. The crosshatch features in the UV flat field (F336W)<br />

are normal, due to the detection-layer structure in the CCDs; the level is typically

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