... pixels1
In imaging mode n pix of a point source is calculated within a 2 FWHM diameter aperture: n pix  = $ \pi$$ \left(\vphantom{\frac{\mathrm{seeing}}{\mathrm{scale}} }\right.$$ {\frac{{\mathrm{seeing}}}{{\mathrm{scale}}}}$$ \left.\vphantom{\frac{\mathrm{seeing}}{\mathrm{scale}} }\right)^{2}_{}$. In spectroscopic mode the program uses n pix = 2 . $ {\frac{{\mathrm{seeing}}}{{\mathrm{scale}}}}$. For an extended source n pix is set to 1 for both dimensions of the source.
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