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

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20 Chapter 3: Choosing the Optimum HST <strong>Instrument</strong><br />

samplings offered by the NICMOS/NIC1 and NIC2 channels. Further, the WFC3/IR<br />

channel covers 45 times the area of the NICMOS/NIC2 channel with slightly coarser<br />

sampling, but arguable better photometric precision.<br />

Table 3.1 presents a comparison of the wavelength coverage, pixel scale, and field<br />

of view of WFC3 and of the other HST imaging instruments that are currently<br />

available.<br />

3.3.3 Detector Per<strong>for</strong>mance<br />

Table 3.2 summarizes the on-orbit measurements of read-out noise and dark<br />

current <strong>for</strong> the WFC3 detectors, and compares them with the parameters <strong>for</strong> the other<br />

currently available HST imaging detectors. Chapter 5 gives more detailed in<strong>for</strong>mation<br />

about the detectors in both channels. Chapter 9 discusses sensitivities, limiting<br />

magnitudes, and exposure times.<br />

Table 3.2: Characteristics of HST CCD and HgCdTe imaging detectors currently available. The<br />

WFC3/IR dark current includes the instrument thermal background.<br />

Detector<br />

Read-out noise<br />

(e – rms)<br />

Dark current<br />

(e – /pix/s)<br />

Mean well Depth<br />

(e – )<br />

WFC3/UVIS 3.1–3.2 0.0008 75,000-80,000<br />

ACS/WFC 4.8 0.0062 84,700<br />

STIS/CCD<br />

5.4 (gain=1),<br />

7.7 (gain=4)<br />

0.009 114,000<br />

WFC3/IR ~12.0 1<br />

0.05 77,900<br />

NICMOS/NIC1 26 0.3 145,000<br />

NICMOS/NIC2 26 0.3 152,000<br />

NICMOS/NIC3 29 0.3 213,000<br />

1. WFC3/IR read noise is <strong>for</strong> a 16-read linear fit; NICMOS read noise is<br />

<strong>for</strong> a pair of reads (double sampling). WFC3/IR double sampling read<br />

noise is 20.2–21.4 e – .<br />

3.3.4 System Throughputs and Discovery Efficiencies<br />

Figure 3.2 plots the measured on-orbit system throughputs of the two WFC3<br />

channels as functions of wavelength, compared to those of ACS, NICMOS, and<br />

WFPC2. These curves include the throughput of the OTA, all of the optical elements<br />

of the instruments themselves, and the sensitivities of the detectors. Throughputs were<br />

calculated at the central wavelength (the “pivot wavelength”; see Footnote 3 to Table<br />

6.2) of each wide-band filter of each instrument.<br />

As Figure 3.2 shows, WFC3 offers a unique combination of high sensitivity and<br />

wide spectral coverage ranging from the UV to the near-IR. WFC3 extends and<br />

complements, over a large field of view, the optical per<strong>for</strong>mance of ACS/WFC at<br />

wavelengths shorter than ~400 nm and longer than 1000 nm. The good degree of

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