Spatial scale on IDS
Spatial profile degradation at the CCD edges   
   
The 235mm camera with RED+2 CCD provides a spatial scale of 0.44 arcsec/pixel. 
The maximum unvignetted slit-length usable with IDS is 3.3 arcmin, corresponding 
to some 450 detector pixels for RED+2.
Note that the spatial profile degrades toward the upper
and bottom parts of the CCD, giving the impression that in these regions
the star image is out-of-focus (most evident in the vignetted regions where
a stellar profiles becomes double-peaked). This is a feature due to the IDS
optics, in particular the CCD corrector lens, that was not designed for large
format detectors like the RED+2 CCD.
   
   
 Fringing and Cosmetic defects   
   
 RED+2 chip suffers from mild fringing. 
 Here there is an 
 image of a flat field spectra  showing fringing in the redmost part (from around 9000 Å) and here there is an 
 example showing the fringing modulation along the whole RED+2 CCD  with R300V grating covering up to 10000 Å. In this image, for comparison the fringing modulation of the EEV10 detector was included. The level of fringing for the RED+2 detector is less than 2% in all interval, with an average of about 1%. 
There are a few cosmetic defects on the surface of the chip, but 
 nothing particularly severe.  
   
 Charge spreading variations
Effects on spectral resolutions   
 
   
 The diffusion of charges between pixels during integrations causes a degrading 
 of the spatial and spectral resolution. For a long-slit spectrograph like 
 IDS, with the INT mean seeing around 1".0-1".5, spatial degradation is not significant with the pixel size of the RED+2, but should be considered in the spectral direction. For a back illuminated CCD this
 charge diffusion (often referred to as the Modulation Transfer Function;
 MTF) becomes progressively worse for shorter wavelength incident light. For
 example, using a slit-width projecting 2 pixels on the detector results
 in a FWHM measured of 2.4 pixels (measured at ~4000 Å) when the spectrograph
 is at best focus. Similarly, a slit-width projecting 4 detector pixels
 will produce a FWHM of ~4.4 pixels (at ~4000 Å). This effect becomes
 less severe towards redder wavelengths and is negligible at around 6000 Å.
   
   
 Measured throughput