After the preliminary screening to eliminate spurious data, 1446 observation records were retained. The general statistics of the FWHM measurements is:
Average: 0.79 arcsecBecause tracking and guiding errors are not corrected by a fast tilting mirror as it was the case with HRCam, the FOCam image sizes are larger than the ones obtained by HRCam and also show a higher dependency on wind speed:Median: 0.75 arcsec
Rms: 0.205 arcsec
Minimum: 0.32 arcsec
Median for U < 3 m/s: 0.74 arcsecFig. shows a scatter plot of FWHM values with respect to . Only observations with and U < 6 m/s are plotted.Median for 3 < U < 6 m/s: 0.75 arcsec
Median for 6 < U < 10 m/s: 0.78 arcsec
Median for U > 10 m/s: 0.91 arcsec
For K, seeing even appears to decrease but the scarcity of data does not allow us to attribute a statistical significance to the trend.
Fig. shows the scatter of FWHM values with respect to the temperature difference between the dome interior and the outside air. The FOCam data also cover the range of positive up to 4K and, although here also the data points are very unevenly scattered, no trends are apparent.
[IMAGE ]
Figure: FWHM from the FOCam data
as a function temperature difference
between the mirror surface and the surrounding air.
The full line represents a best fit of binned median values: for
the mirror seeing contribution is evaluated
0.3 .
The dashed line corresponds to a factor of 0.38, as obtained from
the HRCam data.
Figure: FWHM from the FOCam data
as a function of the temperature
difference between dome interior and outside.
The airmass effect is then evaluated by analyzing a subset with
0.3K and U < 6 m/s (fig. ).
Noting that the median FWHM for is 0.71 arcsec,
a least square fit on the binned median values
gives a fixed error due to the instrument
arcsec
while the airmass dependent variable is evaluated as
arcsec
While we had expected the value of from FOCam to be larger that in HRCam, we find that also the apparent natural seeing is larger. Barring the possibility that HRCam can correct seeing image motion to such an extent, this suggests the presence of mechanical effects from the telescope which cause the tracking performance to depend on orientation. As the data set does not allow the discrimination of this particular effect, we will proceed in the analysis on the basis of the values evaluated above, since the effect of an inaccuracy in the relative weighting on other seeing effects is anyway minor (see equation ()).
Inserting the computed values of and in equation (), a least square fit on the mirror seeing data (fig. ) gives for :
One should remind that the value of this coefficient is determined to a large extent by only three data sequences and therefore carries less confidence than the value found in the HRCam case (which was 0.38 arcsec/). Both trend lines are drawn for illustration on fig. .
[IMAGE ]
Figure: FOCam FWHM versus in absence of wind and mirror
seeing effects.
Fig. shows a scatter plot of FWHM with respect to wind speed.
This subset only includes data for which
and K (562 records).
This plot shows the overall effect of wind on the FOCam
performance, averaging out the influence of relative azimuth of
observation with respect to wind direction.
Assuming that the median of the wind induced errors are
proportional to the square of wind speed
a best fit of equation
gives then
[IMAGE ]
Figure: FOCam FWHM versus wind speed.