Scintigraphic myocardial uptake of 123 I-metaiodobenzylguanidine ( 123 I-mIBG) is usually semiquantified by calculating a heart-to-mediastinum (H/M) ratio, after drawing region of interest (ROI) over the heart (including or not including the cavity) and the upper mediastinum (avoiding the thyroid gland) in the planar anterior view. Then, average counts per pixel in the myocardium are divided by average counts per pixel in the mediastinum. Despite efforts to standardize myocardial 123 I-mIBG scintigraphy, 2 difference in collimator use is one of the most important causes of discrepancy in H/M ratio values among institutions. The widespread availability of low-energy (LE) parallel hole collimators determines their common use for 123 I studies; however mediumenergy (ME) collimators have been shown to provide superior semiquantitative accuracy in these type of studies.3,4 In addition to the major emission of 159-keV photons, 123 I emits high-energy photons of more than 400 keV (approximately 2.87%, main contributor 529 keV, 1.28%), which lead to penetration of the LE collimator septa and cause scatter detected in the 159-keV energy window, resulting in image quality degradation and H/M ratio modification. The H/M ratio is lower when a LE collimator is used because of the increased proportion of mediastinum counts from scattered higher-energy photons.5 ME collimators minimize the effects of septal penetration (Figure 1). [3][4][5] To further complicate the standardization of the technique, the classification of collimators in two major groups of LE and ME is rather simplistic. Camera vendors offer several types of collimators in order to optimize balance among resolution, sensitivity, and applicable energy range, and collimators with equal designation from different vendors are not exactly the same. In addition, vendors can even change the specifications of the collimators without reclassifying them to a different category, which may further increase the variability in H/M ratio among institutions and published studies. It should also be taken into account that other technical gamma camera characteristics such as uniformity may influence the H/M ratio measurement.To overcome differences in the choice of collimator for H/M ratio quantification, methods of multiple window acquisition and phantom cross-calibration have been reported. Multi-window methods can be easily performed by institutions attending to the capability of current camera-computer systems, but they lack deep validation and clinical experience. Furthermore, dualenergy window methods increase the H/M ratio at expense of reducing heart count density and, consequently, defect contrast.
6Three years ago, Nakajima et al. published the results of a large multicenter study of cross-institution phantom calibrations for the quantification of the H/M ratio by various gamma camera and collimator combinations from common vendors. 7 The authors had previously reported the phantom design to easily produce predefined H/M ratios.6 They had also previously reported the i...