Page 346 - Biomedical Engineering and Design Handbook Volume 2, Applications
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324  DIAGNOSTIC EQUIPMENT DESIGN

                                   Spatial Linearity Correction
                                                                             New location
                                Event location is                            x = x′ + Δx′
                                estimated as x′, y′                          y = y′ + Δy′

























                                    Before correction             After correction

                             FIGURE 11.6 Spatial linearity correction. Residual positioning errors are corrected by creating a
                             correction map from the image of a precision hole phantom. A lookup table of the position-dependent
                             correction factors allows on the fly repositioning of the detected events that dramatically improves
                             image uniformity.




                         Displacements for regions in between holes that are not directly sampled are interpolated at a
                       very-high sampling frequency and stored as a lookup table. When a valid event is detected, the ini-
                       tial x and y coordinates are modified by the appropriated displacements read from the lookup table.
                       Using this approach, events can be accurately positioned to better than 0.5 mm. The improvement in
                       spatial linearity has a profound effect on field uniformity. Both images show the response of the scin-
                       tillation camera to a uniform flux of gamma rays. With spatial linearity correction, the field becomes
                       uniform to within ±10 percent of the mean image counts. Although this level of uniformity may be
                       adequate for conventional planar imaging, tomographic imaging requires better uniformity.
                         There are still some residual nonuniformities that exist in the scintillation camera even after
                       energy and spatial linearity correction have been applied. These are further reduced by applying uni-
                       formity correction. Typically, a high count flood is acquired and a map of the nonuniformities is
                       stored in a memory buffer. During acquisition, the number of valid events that are acquired is mod-
                       ulated by this reference uniformity map to ensure uniformity. With this additional correction, the
                       field uniformity can be reduced to within ±3 percent of the mean image counts.
                         Photomultiplier tubes are relatively unstable components. Their performance drifts as they age
                       and the tubes are also sensitive to variations in temperature and humidity. In order for the energy,
                       spatial linearity, and uniformity corrections to remain valid, there must be some way of maintaining
                       the PMTs at a constant operating point. Most scintillation camera systems have PMT stabilization
                       firmware that dynamically adjusts the PMTs in response to a known reference signal. Some vendors
                       use a constant output light-emitting diode inside the detector housing that flashes at a rate of 10 times
                       per second. The individual PMT signals from these calibration flashes are monitored to compare the
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