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Field RA diff. DEC diff.<br />

["] ["]<br />

W1 +0.014 +0.010<br />

W2 −0.035 −0.025<br />

W3 +0.011 +0.010<br />

W4 −0.026 −0.023<br />

Table 13: Mean RA and DEC differences between the external errors in each field and the mean external errors,<br />

averaged over the four Wide fields.<br />

external reference catalogue. This astrometric accuracy of CFHTLS stacks measures the final<br />

absolute astrometric accuracy of each stack and their corresponding catalogues.<br />

The astrometric calibration of the Wide survey is described in Section 3.5.<br />

4.5.1 Astrometric calibration errors<br />

The mean internal astrometric calibration errors are derived using the cross-identifications of sources<br />

inside the overlapping regions of adjacent fields (see Fig. 21). All single input MegaCam Wide, Pre-<br />

Wide (see Fig. 21) and short photometric exposures images remaining after selection are included.<br />

The cross-identifications and the internal errors are obtained during the SCAMP calibration process. The<br />

calibrations outputs of the Wide fields W1, W2, W3 and W4 are available from the synoptic table.<br />

Over the whole survey, the mean internal rms error is<br />

σ RA = 0.0279” ± 0.0049” , and , σ DEC = 0.0256 ± 0.0057” , (16)<br />

where the reported errors are not the SCAMP internal errors, but the mean absolute difference of the<br />

internal errors between the four Wide fields and the mean error values. Since the four fields are calibrated<br />

independently, the errors quoted above are approximate; the internal errors for W1, W2, W3 and W4 are<br />

given in Table 6.<br />

For each field, the mean rms external RA and DEC errors of the astrometric solution are derived during<br />

the SCAMP calibration process, using the cross-identification of sources inside each single CFHTLS Wide<br />

image with the 2MASS catalogue. The mean external calibration errors over the whole survey are σ RA =<br />

0.239” and σ DEC = 0.232”. They roughly correspond to the internal errors of the 2MASS catalogue.<br />

The mean scatter from one Wide field to another is uncertain, because the CFHTLS is made of only four<br />

independent fields. It can be estimated from the offsets of the mean external errors of each field separately<br />

with respect to the mean value over the four fields. The offsets are listed in Table 13. The amplitudes<br />

are very close to the internal astrometric calibration errors of the Wide fields, hence we conclude that the<br />

internal astrometric accuracy for the CFHTLS Wide does not have significant field-to-field scatter.<br />

59

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