Abstract
We recently demonstrated in a clinical trial the ability of a new protocol, IQ SPECT, to acquire myocardial perfusion imaging (MPI) studies in a quarter of the time (12 s/view) of the standard protocol, with preserved diagnostic accuracy. We now aim to establish the lower limit of radioactivity that can be administered to patients and the minimum acquisition time in SPECT MPI using an IQ SPECT protocol, while preserving diagnostic accuracy. Methods: An anthropomorphic cardiac phantom was used to acquire clinical rest scans with a simulated in vivo distribution of 99mTc-tetrofosmin at full dose (740 MBq) and at doses equal to 50%, 25%, and 18%. For each dose, 2 sets of images were acquired, with and without a transmural defect (TD). Variable acquisition times were also used for each dose. We analyzed raw data and reconstructed images, including no correction and correction for attenuation (AC), for scatter (SC), or for both (ACSC). Images were evaluated qualitatively and quantitatively in order to assess left ventricle (LV) wall thickness (full width at half maximum of the medial sections), TD, and cavity contrast in the LV wall. Data were compared across different acquisition times within the same dose and across doses with the same acquisition time. Results: Images were visually scored as very-good quality except those acquired with 4 s/view or less at 100% dose and 6 s/view or less with 50%, 25%, or 18% dose, due to false-positive defects. LV wall thickness was not significantly different among all acquisitions. Cavity contrast remained unchanged within the same dose for all images and tended to be higher in AC and ACSC images. TD contrast remained unchanged within the same dose for all images. In SC and no-correction images, contrast was constant for all doses. AC images had significantly higher TD contrast values, and ACSC images showed a drop in TD contrast for a 50% dose. Conclusion: IQ SPECT effectively preserved both image quality and quantitative measurements with reduced acquisition time or administered dose in a phantom study. These findings suggest that approximately one eighth of the time, compared with standard protocols with a full dose, or a lower dose at an acquisition time of 12 s/view can be applied in MPI without the loss of diagnostic accuracy.
- coronary artery disease
- 99mTc-tetrofosmin SPECT/CT
- IQ SPECT
- low counts acquisition
- myocardial perfusion imaging
SPECT myocardial perfusion imaging (MPI) has been extensively validated for the diagnosis and prognosis of cardiac disease and is currently largely recommended in national and international guidelines (1).
Growing interest in shortening scan time or in reducing administered dose has led to the development of new hardware and modern software packages with the aim of improving image quality and diagnostic accuracy comparable or even superior to standard protocol (2,3).
In a clinical trial, we have recently validated a new protocol, IQ SPECT, characterized by the use of multifocal collimators with dedicated reconstruction software (4). The new IQ SPECT with multifocal collimators, which can be applied as a plug-in on multipurpose cameras, has a favorable performance regarding sensitivity and contrast-to-noise ratio when compared with conventional cameras equipped with low-energy and high-resolution collimators (5). The unique geometry of the collimator, with holes focused at the center and near-parallel at the edge, facilitates enhanced sensitivity for the cardiac region while permitting acquisition of untruncated projection data. In conjunction with a cardiocentric scan orbit at 28 cm to maximize regional magnification, this configuration provides a 4-fold-higher sensitivity for the cardiac region than parallel-hole collimators (6). Because the collimator response is not only distance-dependent but also variable across its face, an accurate modeling of magnification and the system point-response function (PRF) is essential. As such, the 3-dimensional PRF is modeled from the autocorrelation of the hexagonal shapes of the collimator holes at the entry and exit points (6), and the collimator is programmed to automatically measure hole orientation, thus taking into account deviations from design specifications that are introduced in the casting process. This collimator setup allows the higher sensitivity to be taken advantage of without the poorer spatial resolution or inconsistent reconstructed data that occur when low doses or short acquisition times are used. Furthermore, the implementation of a proprietary conjugate-gradient iterative reconstruction algorithm incorporating measured values for gantry deflections, collimator-hole angles, and system PRF contributes to enhanced sensitivity and diagnostic accuracy (7). This algorithm also includes software for incorporating CT data into a patient-specific μ map and an energy window–based estimate to correct for patient-induced scatter to overcome poor count statistics. In fact, the addition of attenuation correction in the iterative algorithms improves the accuracy of the camera over resolution recovery alone and leads to greater consistency and more accurate reconstructed images (8). Taken together, these approaches maximize the image resolution and sensitivity under the constraint of shortened acquisition time. It remains unclear whether this maintained image quality also pertains to lower injected dose.
We therefore aimed to establish the lower limit of administered radioactivity and minimum acquisition time in SPECT MPI using the IQ SPECT system, while preserving diagnostic accuracy.
MATERIALS AND METHODS
Phantom Preparation
An anthropomorphic phantom featuring inserts to simulate lungs, liver, left ventricle (LV) wall, LV chamber, and a removable transmural perfusion defect (TD) (Torso Phantom and Cardiac Insert; Data Spectrum Corp.) was used in this study. The TD insert (45 × 2 cm) was filled with nonradioactive water to simulate a TD and located in the mid to basal lateral position in the LV wall. The lung inserts were filled with Styrofoam (The Dow Chemical Co.) beads and nonradioactive water to simulate lung tissue attenuation density. The remaining chambers were filled with variable-activity concentrations of 99mTc: 159 ± 8 kBq × mL−1 for the LV wall, 94 ± 2 kBq × mL−1 for the liver, and 7.6 ± 0.2 kBq × mL−1 for the chest and LV chamber. Concentrations were selected to reflect the in vivo distribution pattern of 740 MBq of 99mTc-tetrofosmin (9,10).
Image Protocol and Acquisition
IQ SPECT System
Images were acquired on a hybrid dual-head SPECT/CT system (Symbia T; Siemens Medical Solutions AG) equipped with multifocal collimators (Smartzoom) of 128 × 128 matrix size and a zoom factor of 1. Each collimator consists of 48,000 hexagonal holes (diameter, 1.9 mm; length, 40 mm). Spatial resolution is progressively increased from the camera surface to the cardiac sweet-spot at 28 cm, which was set as the center of rotation for this study, thereby keeping the LV phantom at the highest magnification throughout the acquisition. A scanning arc of 104° with 6° angular steps was used for each of the camera heads. For each detector, 17 views were acquired. Acquired data were then reconstructed using a proprietary iterative reconstruction algorithm (3 iterations, 10 subsets) accounting for gantry deflections, collimator-hole angles, and system PRF (4). Attenuation correction was applied using a patient-dedicated low-dose CT-derived μ map. An energy window–based estimate was used to correct for scatter, identifying dual-energy windows (127–155 keV, primary; 99–126 keV, scatter).
Imaging Protocol
Phantom images with and without the TD insert were acquired serially at the time of loading (0 h) and after 6, 12, and 15 h to simulate a dose reduction to 50%, 25%, and 18%, respectively. This approach minimized variability in activity loading among different phantom cavities.
For each dose, different acquisition times were also used (for the 100% dose, 1, 2, 3, 4, 6, 8, and 12 s/view; for the 50% dose, 6 and 12 s/view; for the 25% dose, 6 and 12 s/view; and for the 18% dose, 6, 12, and 24 s/view). Acquisitions were performed sequentially from shortest to longest time.
Images were analyzed with and without attenuation or scatter correction, generating 4 datasets: with no corrections (NC), attenuation-corrected (AC), scatter-corrected (SC), and attenuation- and scatter-corrected (ACSC). The software for SC and AC was provided by the manufacturer using default settings. Alignment between CT and SPECT images was visually verified. Images have been qualitatively and quantitatively evaluated.
Visual Analysis
The quantitative perfusion SPECT–quantitative gated SPECT software and the dedicated IQ SPECT protocol generated left ventricular polar maps of perfusion, which were divided into 17 segments. Three experienced readers, masked to acquisition modality, reviewed the images and evaluated the map uniformity, the extent of TD, and the presence of unexpected artifacts. Uptake in each segment was scored using a 5-point score according to guidelines of the American Society of Nuclear Medicine (11) (normal perfusion, 0; mild reduction in counts not definitively abnormal, 1; moderate reduction in counts—definitively abnormal, 2; severe reduction in uptake, 3; and absent uptake, 4). Interobserver discrepancies were resolved by consensus.
Quantitative Analysis
After reconstruction, all image sets were processed to evaluate the following 3 parameters, associated with image quality for MPI: LV wall thickness, contrast between LV wall and LV cavity, and contrast between LV wall and TD. Wall thickness and wall-to-cavity contrast were evaluated only without the TD insert in the LV wall. Measurements were obtained using ImageJ software (12) and repeated at least 3 times by an experienced operator to minimize measurement errors. Quantitative data were compared for variable shortened image acquisition times at a constant dose (i.e., 100%) and for variable lower doses at a constant image acquisition time (i.e., 12 s/view).
LV Wall Thickness
LV wall thickness was calculated as full width at half maximum (FWHM) of the myocardial signal in the midventricular section of the LV short-axis by fitting the central count profile with a theoretic gaussian one. The image was summed over 3 consecutive slices in the midventricular section, and LV wall thickness was estimated as a mean of 3 different measurements taken from 3 different profiles—that is, anterior, septal, and inferior wall.
Cavity Contrast
To calculate the contrast between cavity and LV wall, 2 regions of interest (ROIs) were drawn on the midventricular short-axis images, to estimate the mean counts per voxel for the LV wall (ηLV) and ventricular chamber (ηIC), respectively. Figure 1A shows in detail how the measurements were performed. The dimensions of the circular ROI drawn on the ventricular cavity were kept identical among all acquired images (diameter, 9.6 mm).
Cavity contrast was defined as:where CLV and CIC are the true tracer concentrations in the inserts simulating LV wall and LV cavity, respectively.
TD Contrast
The contrast between TD and LV wall was evaluated in the LV short-axis by drawing ROIs on the central short-axis images of the phantom acquisitions with TD defect, to estimate the ηLV and TD (ηTD), respectively. The dimension of the circular ROI drawn on TD was kept identical among all acquired images (diameter, 7.6 mm) (Fig. 1B).
TD contrast was defined as:
Statistical Analysis
Statistical analysis was performed using SPSS software (version 16.00 [SPSS Inc.] for Windows [Microsoft]). All numeric values are given as mean ± SD. Differences among the acquisitions concerning LV thickness, background variability, cavity contrast, and TD contrast were assessed by paired t test and a 3-way factorial ANOVA. Reconstruction protocols, positioning combinations, and count statistics were considered as independent variables (factors) and image quality indices as dependent variables. All P values less than 0.05 were considered to be statistically significant.
RESULTS
Qualitative Evaluation
Images were qualitatively reviewed in random sequence, with operators masked to acquisition time and dose. Images acquired with 100% dose with very low counts (i.e., those acquired with an acquisition time of 1 s/view) showed severe inhomogeneity, with false defects in the anteroseptal and inferolateral walls. Images with an intermediate acquisition time (2–4 s/view) were more homogeneous but still exhibited discernible false defects. The interobserver concordance was excellent (100%) both for images with very low count statistics and for images with longer acquisition times (i.e., 1, 2, 6, 8, and 12 s/view). Those images acquired with 3 and 4 s generated disagreements in 1 of the 3 operators, only concerning the evaluation of the small false-positive defects. Disagreement within the idealized confines of the phantom study would likely be amplified in clinical application. Therefore, we considered as adequate only images with very-good quality (i.e., those acquired with at least an acquisition time of 6 s/view, which did not show any false-positive defects) (Figs. 2–3).
The same approach was followed when evaluating images acquired with different doses. Very-good-quality images were acquired with at least 12 s/view for the 50%, 25%, and 18% doses. No interobserver discrepancy was found for lower doses.
Quantitative Evaluation
To determine the effect of acquisition time on image quantification, analysis was performed at 100% dose over all acquisition times. Because qualitative evaluation for the less-than-100% dose showed that only images acquired with at least 12 s/view were of sufficient quality, we performed quantitative analysis only with this acquisition time for the 50%, 25%, and 18% doses.
LV Wall Thickness
Table 1 shows FWHM values for all images, acquired with different doses and at different times. No statistically significant differences were evidenced among all acquisitions with different doses and different reconstruction corrections.
Cavity Contrast
Table 2 shows cavity contrast measurements for all images, acquired with different doses and at different times. Reducing acquisition time at a 100% dose did not significantly alter the cavity contrast measurements. Cavity contrast tended to be higher in images corrected for attenuation (AC and ACSC), though a statistical significance was not reached (P = 0.20) (Fig. 4).
Reducing the administered dose with a constant acquisition time also did not significantly alter cavity contrast. The nonsignificant tendency for higher contrast after AC and ACSC remained (P = 0.21) (Fig. 5).
At a 18% dose, cavity contrast did not differ between images acquired with either 12 or 24 s/view.
TD Contrast
Table 3 shows TD contrast measurements for all images, acquired with different doses and at different times. When acquisition time was reduced with a standard 100% dose, TD contrast was unchanged. AC and ACSC images showed a modest increase in TD contrast, compared with uncorrected images (P = 0.14) (Fig. 6). By contrast, lower administered dose affected the TD contrast, partially dependent on the corrections applied. Although in uncorrected and SC-alone images TD contrast was constant across doses, AC images exhibited significantly higher TD contrast (P = 0.04) at all doses. When both AC and SC were applied, TD contrast values were not statistically different, compared with AC, SC, and NC images (P = 0.16), but were inconsistent at variable doses. As shown in Figure 7, TD contrast was decreased at a 50% dose, restored somewhat at a 25% dose, and decreased again at a 18% dose. TD contrast values in ACSC images acquired with a 50% dose were significantly different from values in ACSC images obtained with other doses (P = 0.02). At a 18% dose, the reduction of ACSC image TD contrast approached statistical significance, compared with both 100% and 25% doses (P = 0.11).
DISCUSSION
This is the first study, to our knowledge, investigating the feasibility of a substantial dose reduction in MPI using the IQ SPECT protocol. We previously demonstrated an equivalence between quarter-time IQ SPECT and full-time standard SPECT with an ordered-subset expectation maximization reconstruction algorithm (4), but the impact of dose reduction has not been elucidated.
Images obtained using a full standard dose showed no statistical difference in wall thickness or contrast ratio with lower acquisition times. The relative image quality was somewhat reduced on acquisitions shorter than 6 s/view, suggesting that, for a 740-MBq standard dose, a minimum acquisition time of 6 s/view is required.
When evaluating the performance of a package with a dedicated iterative reconstruction algorithm, reconstruction parameters (number of iterations, number of subsets, and postfilters) can have a significant impact on image quality (13). Moreover, integrated software to correct for attenuation and scatter can also lead to differences in the results (9). Therefore, while looking at the lowest possible dose, we also evaluated the impact of different corrections when performing MPI.
Wall thickness and contrast remained constant for NC, SC, and AC images across different doses, though AC appeared to improve contrast. Conversely, TD contrast in ACSC images was distinctly reduced with a 50% dose. Higher TD contrast with attenuation correction is a logical result and is consistent with more accurate estimation of TD extent as reported in the literature. Johansen et al. demonstrated a significant diagnostic modification in approximately 20% of abnormal studies when AC was applied, predominantly within the right coronary artery territory (14). Similar findings were reported by Giubbini et al. (15), in which AC significantly reduced both summed stress score and summed rest score; they reasoned that without AC the scar size was systematically overestimated.
These MPI studies, using parallel-hole collimators, report inferior and posterobasal wall artifacts due to diaphragmatic attenuation and the presence of typical apex thinning. When IQ SPECT is used, these same territories are affected, but the apparent size of such artifacts appears increased because of the different collimator shape (4,7). Regional counts in these high-attenuation territories dramatically affected the TD contrast calculation in the absence of AC.
The unexpected drop in TD contrast with a 50% dose and relative recovery of the correction with further dose reductions requires further examination.
We may speculate that the particular collimation shape can influence the estimation of scatter and generation of attenuation maps, particularly with lower count statistics. The simultaneous application of 2 correction parameters would amplify such an error and contribute to a degradation of image quality (16). The recovery of TD contrast with further reduced administered doses may relate to the manufacturer default reconstruction algorithm settings, which may be more optimal for a quarter-dose protocol, compared with a 50% dose. As such, the algorithm may compensate more effectively for the count reduction in a specific dose range, manifesting as an improvement of image quality. With further dose reduction, the compensation tends to be less effective, as evidenced by reloss of TD contrast values at an 18% dose.
A previous study (9), using iterative reconstruction algorithms applied to standard systems with parallel-hole collimators, suggested that ACSC images were more robust than with AC alone. The difference from the present study may be explained by the difference in collimation and reconstruction software.
There is an apparent discrepancy in that reducing relative imaging time appears to have a more dramatic effect on image quality than a comparable reduction of injected dose. Dose reduction was always evaluated at 25% of standard acquisition time. At one eighth of the standard acquisition time (i.e., 6 s/view, one eighth of the standard scan), image quality begins to deteriorate, whereas a dose reduction to 18% of the standard dose at one-quarter the standard acquisition time (i.e.,12 s/view, one twenty-fourth of the standard scan) has a lesser effect on image quality. Part of this difference may derive from lost time due to camera movement and settling, as evidenced by more pronounced count reduction with lower time acquisition versus lower administered dose (i.e., 540 kcounts at 6 s/view vs. 650 kcounts at 50% dose, 12 s/view). With longer acquisitions, this dead time is likely negligible but is accentuated with shorter times per view. However, the resultant 17%–20% difference in total counts is insufficient to fully explain the discrepant effect on visual image quality. One may speculate that the uniformity of image reconstruction is more finely attuned to reduced global counts, but a complete explanation of this aberration requires further investigation.
Our study has some limitations. First, acquisitions with different times per view were sequentially performed; therefore, results could be theoretically influenced by 99mTc decay. However, time interval between the first and the last examination within the same established dose was limited (maximum, 20 min). Second, we did not evaluate the influence of other iterative reconstruction parameters (i.e., number of subsets, iterations, and resolution recovery) on the results. Third, these results were obtained in an ideal standard situation and might not be completely applicable in clinical practice; therefore, further clinical studies on patients are necessary to validate the clinical relevance of the findings. All acquisitions and data points derive from a single phantom source and activity loading. Finally, the phantom used in this study only allows the evaluation of ungated SPECT images; therefore, the results could be different when higher count statistics are required, as in the case of electrocardiography-gated studies, and the impact of motion cannot be evaluated.
In summary, an accurate evaluation was provided by acquiring a phantom MPI study with a standard dose and an acquisition time of 6 s/view (i.e., approximately one eighth, compared with the standard protocol). With regard to the administered dose, although as low as an 18% dose provided sufficient image quality, such a dramatic dose reduction may be excessive. For clinical application, many additional factors such as gated acquisitions, motion, and patient-induced scatter may complicate corrections and degrade image quality, and in vivo studies are warranted. Regarding reconstruction corrections, we would also suggest the use of noncorrected and AC images in clinical practice, because of less variability under different conditions.
Acquiring data of good quality with lower radioactivity would reduce patients’ effective dose to approximately 2.5–3 mSv for a stress–rest study with 99mTc-labeled tracers, much lower than current protocols with general-purpose low-energy and high-resolution collimator cameras (∼9–10 mSv) and similar to those obtained with the new cadmium-zinc-telluride cameras (17). Moreover, the possibility to perform SPECT studies with reduced tracer activities may be helpful to overcome limitations due to 99mTc shortages and could also address the requirement for population dose containment.
CONCLUSION
We demonstrated that IQ SPECT in a phantom study effectively preserved both image quality and quantitative contrast with reduced acquisition time or administered dose. If translated to clinical application, these protocols may improve patient comfort and reduce radioexposure without compromising diagnostic accuracy, which could be of particular interest for those centers in which a new dedicated heart camera system is not available.
DISCLOSURE
The costs of publication of this article were defrayed in part by payment of page charges. Therefore, and solely to indicate this fact, this article is hereby marked “advertisement” in accordance with 18 USC section 1734. No potential conflicts of interest relevant to this article are reported.
Footnotes
Published online Nov. 20, 2014.
- © 2014 by the Society of Nuclear Medicine and Molecular Imaging, Inc.
REFERENCES
- Received for publication May 23, 2014.
- Accepted for publication October 27, 2014.