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IMAGING PERFORMANCE OF A CCD DETECTOR        273

                                      Selected           Radius of Airy disk produced
                                      pixel sizes           by various objectives

                                             6.8  m
                                                           100×, 1.30 NA = 26  m
                                             9  m            63×, 1.25 NA = 16  m
                                                             40×, 1.30 NA = 10  m
                                                             32×, 0.40 NA = 27  m
                                             12  m
                                                             10×, 0.25 NA = 13  m
                                             17  m


                                             23  m

                       Figure 14-11
                       Comparison of pixel dimensions to diffraction spot size. Left: The pixel sizes of various CCD
                       imagers are indicated in micrometers. Right: The diameter of the diffraction spot (Airy disk)
                       produced by various objective lenses as it would appear on a the surface of a CCD.
                       According to the Nyquist sampling theorm, preservation of the spatial resolution of the optics
                       requires that a diffraction disk radius be covered by a minimum of 2 adjacent pixels on the
                       CCD. For a 40 , 1.3 NA lens the diffraction spot radius   40(0.61   0.546)/1.3   10  m,
                       so the coverage provided by a CCD with 6.8  m pixels is just barely adequate. However, the
                       same CCD provides excellent sampling for a 100 , 1.3 NA lens with spot radius   100
                       (0.61   0.546)/1.3   26  m, even under conditions of 2   2 binning (6.8   2   13.6  m).



                       front-illuminated CCDs are efficient, sensitive detectors with a peak quantum efficiency
                       of 40–50% (80% for the newest designs) at visible wavelengths ranging from 400 to
                       1100 nm with peak sensitivity at 550–800 nm (Fig. 14-12). With special coatings on the
                       CCD, it is possible to extend the spectral range from 120 to  1100 nm. With special
                       thinned, back-illuminated designs (very expensive!), quantum efficiency can be greater
                       than 90%. However, the most recent interline CCD designs include high-transparency
                       materials for defining pixel boundaries on the CCD surface that allow front illumination
                       with 80% QE. Sometimes it is important to increase the sensitivity of signal detection
                       and improve the S/N ratio in other ways, such as by decreasing the background signal,
                       increasing the object signal, or selecting more efficient fluorescent dyes.


                       Noise


                       System noise refers to electrons in the CCD signal that have their origins in sources
                       other than the object photons. Most noises are associated with the camera electronics
                       (bias noise and read noise), and to a lesser extent, the thermal noise from the CCD. Bias
                       signal (also called offset) and bias noise are components of the CCD signal that arise
                       from the application of a positive bias voltage as required for proper digitization by the
                       ADC. As already described, thermal noise refers to the generation of electrons from the
                       kinetic vibrations of silicon atoms in the CCD substrate. It is common to refer to the bias
                       noise and thermal noise together as the dark noise. As we will see later on, the photo-
                       electron signal itself is also associated with a level of uncertainty called the photon or
                       shot noise that always accompanies measurement of discrete quanta such as photons
                       within a finite time or space. The amplitudes of the principal noises present in a CCD
                       image are summarized in Table 14-1. Noise plays a major role in the determination of
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