REMOVING NOISE
Noise means many different things in different circumstances. Generally, it refers
to some part of the image signal that does not represent the actual subject but has
been introduced by the imaging system. In film photography, the grains of halide
particles or the dye molecules may be described as “noise superimposed on the real
image.” So, too, may dust or scratches on the film. There are rough equivalents to
these with digital photography, and some other problems as well.
A digital picture of a perfectly uniform and uniformly illuminated test card does
not consist of identical pixel values. The histogram of such an image typically shows
a peak with a generally Gaussian shape. The width of the peak is a measure of the
random variation or speckle in the pixels, which although much coarser than the
grain in film, has the same underlying statistical characteristics. All of the processes
of generating charge in the detectors, transferring that charge out of the chip,
amplifying the analog voltage that results, and digitizing that voltage, are statistical
in nature. Some, such as the efficiency of each transistor, also vary because of the
finite tolerances of manufacture. For scanning microscopes, there are also both
statistical variations such as the production of X-rays or secondary electrons and
stability concerns such as the electron gun emission or creep in piezo drivers.
The statistical variations are sensitive to the magnitude of the signal. In the SEM,
increasing the beam current or slowing the scan rate down so that more electrons
are collected at each point, reduces the amount of the speckle as a percentage of the
value, and so reduces the width of the peak in the histogram as shown in Figure 2.24.
Instrumentation variations do not reduce in magnitude as the signal increases. Some,
such as transistor variations on the camera chip, do not vary with time, and are
described as “fixed pattern noise.” The two types of noise are multiplicative noise
(proportional to signal) and additive noise (independent of signal), respectively.
Consider a test image consisting of greyscale steps (a similar image will be used
in Chapter 5 to calibrate measurements based on brightness). If an image contains
only additive noise, and if the detector is linear (output proportional to intensity)
the width of each peak corresponding to one of the grey scale steps would be the
same. If the image contains only multiplicative noise, the peak widths would be
proportional to the intensity value. Figure 2.24 illustrates both situations. This
changes if the final output is logarithmic, in which case multiplicative noise produces
equal width peaks. In practice, most devices are subject to both types of noise and
the peak widths will vary with brightness but not in strict proportion. One of the
important characteristics of random noise is that the amount of noise in an image
varies from bright to dark areas, and some noise reduction schemes take this into
account.
Although the absolute amount of random noise may increase with signal, it
usually drops as a percentage of the signal. Collecting more signal by averaging
over time adds to the signal while the random variations may be either positive or
negative, and tend to cancel out. For purely multiplicative noise, the signal-to-noise
ratio increases as the square root of the averaging time. Of course, in many real
situations the strategy of temporal averaging (collecting more signal) to reduce noise
is not practical or even possible.
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