Abstract

Objective: Computed tomography (CT)-based attenuation correction (CTAC) offers the clear benefit of reliable reconstruction of single-photon emission computed tomography (SPECT) images through its ability to achieve object-specific attenuation maps, but artifacts from dense materials often deteriorate CTAC performance. Therefore, we investigate the feasibility of CTAC in the presence of dense materials using dual-energy virtual monochromatic CT data. Methods: A sodium pertechnetate-filled cylindrical uniform phantom, with a pair of undiluted iodine syringes attached, is scanned with a dual-source CT scanner to obtain both single-energy (120 kVp) polychromatic and dual-energy (80 kVp/140 kVp with tin filtering) virtual monochromatic CT images. The single-energy and the dual-energy CT images are then converted to attenuation maps at 141 keV. SPECT images are reconstructed from 99mTc emission data of the phantom using each single-energy and dual-energy attenuation map and incorporating CTAC procedure. A region-of-in- terest analysis is performed to quantitatively compare the attenuation maps between the single-energy and the dual-energy techniques, each at an iodine-free position and a position adjacent to the iodine solutions. Results: At the iodine-free position, the phantom provides a uniform distribution of attenuation maps in both the single-energy and the dual-energy techniques. In the presence of adjacent iodine solutions, however, severe artifacts appeare in the single-energy CT images. These artifacts make attenuation values fluctuate, resulting in erroneous pixel values in the CTAC SPECT images. In contrast, dual-energy CT strongly suppresses the artifacts and hence improves the uniformity of the attenuation maps and the resultant SPECT images. Conclusions: Dual-energy CT with virtual monochromatic reconstruction has the potential to substantially reduce artifacts arising from dense materials. It has the potential to improve the accuracy of attenuation maps and the resultant CTAC SPECT images.

Highlights

  • Reliable quantification of tracer distributions in single-photon emission computed tomography (SPECT) requires accurate attenuation correction (AC) of emission data, which entails an accurate determination of the attenuation map of the object [1]-[3]

  • Severe artifacts arising from the iodine solutions appeared in the single-energy Computed tomography (CT) image, resulting in an erroneous attenuation map

  • Some of these artifacts, which had positive error values propagated into the computed tomography-based attenuation correction (CTAC) SPECT image

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Summary

Introduction

Reliable quantification of tracer distributions in single-photon emission computed tomography (SPECT) requires accurate attenuation correction (AC) of emission data, which entails an accurate determination of the attenuation map of the object [1]-[3]. Compared to the conventional Chang attenuation correction method [4], x-ray computed tomography-based attenuation correction (CTAC) offers a clear benefit through its ability to correct non-uniform attenuation of photons inside the object [5] [6]. The advantage of the low-noise and high-throughput performance of CTAC over traditional transmission scans has been well recognized in clinical PET [14]-[16]. These features have attracted increasing interest in SPECT in recent years, with the introduction of hybrid SPECT/CT scanners [6] [17] [18]

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