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296      DIGITAL IMAGE PROCESSING

                                called histogram equalization or histogram leveling, yields a histogram that contains no
                                peaks and has a flat, horizontal profile. In leveling, pixel values are reassigned so that
                                each gray level is given the same number of pixels, while the rank order of the pixel val-
                                ues in the original picture is preserved as much as possible. This operation is used to
                                enhance contrast in very-low-contrast (flat) images where most of the pixels have close
                                to the same value, and where conventional methods of histogram stretching are ineffec-
                                tive. Equalization is an extreme measure to rescue images with low-amplitude gradients,
                                but works well as a way to examine bias, dark, and flat-field frames, which can look
                                nearly featureless. The effect of histogram equalization is often dramatic.


                                Unsharp Masking


                                This image-processing procedure does an excellent job of enhancing fine details in an
                                image. Unsharp masking is well known to photographers and astronomers who used the
                                method as a darkroom technique to enhance faint details in photographic prints. As
                                designed by photographers, a blurred, reverse-contrast negative (or unsharp mask) is
                                made of the original negative. The two negatives are sandwiched together in perfect reg-
                                istration in the enlarger and a print is made. To perform this operation on a computer, an
                                unsharp mask is produced by blurring and reducing the amplitude of the original image;
                                the unsharp mask is then subtracted from the original to produce a sharpened image.
                                Extended, uniform regions are rendered a medium gray, whereas regions with sharp gra-
                                dients in amplitude appear as brighter or darker intensities. The principle of unsharp
                                masking is shown in Figure 15-9, and an example of a microscope image processed by
                                this method is shown in Figure 15-10. If the program you are using does not perform
                                unsharp masking, you can perform this operation manually using the following steps:

                                 • Prepare a copy of the original and blur it with a conservative blurring filter. Images
                                    with fine details (high spatial frequencies) require more conservative blurring than
                                    images containing big blocky objects (low spatial frequencies).
                                 • Subtract 50–95% of the amplitude of the blurred image from 100% of the original
                                    using an image math function in the program. The higher the percentage that is sub-
                                    tracted, the greater the sharpening effect.
                                 • Using histogram stretching, adjust the brightness and contrast in the difference
                                    image.



                                Fast Fourier Transform (FFT)

                                This filtering operation selectively diminishes or enhances low or high spatial frequen-
                                cies (extended vs. fine detailed structures) in the object image. This is a valuable opera-
                                tion to consider, because it reinforces concepts given in previous chapters on the
                                location of high- and low-spatial-frequency information in the diffraction plane, which
                                is located in the objective back aperture in the microscope. The effect is similar to that
                                of the blurring and sharpening filters already described, but can be made to be much
                                more specific due to an operation called spatial frequency filtering (Fig. 15-11). When
                                an image is transformed into the so-called frequency domain through an FFT command,
                                the information is represented in two plots (images): one containing a distribution of
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