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Research ArticleImaging

Imaging of the Thyroid and Parathyroid Using a Cardiac Cadmium-Zinc-Telluride Camera: Phantom Studies

Yosuke Miyazaki, Yasuhiro Kato, Akira Imoto and Kazuki Fukuchi
Journal of Nuclear Medicine Technology March 2018, 46 (1) 39-44; DOI: https://doi.org/10.2967/jnmt.117.199042
Yosuke Miyazaki
1Division of Medical Technology and Science, Department of Medical Physics and Engineering, Course of Health Science, Osaka University Graduate School of Medicine, Suita, Osaka, Japan; and
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Yasuhiro Kato
1Division of Medical Technology and Science, Department of Medical Physics and Engineering, Course of Health Science, Osaka University Graduate School of Medicine, Suita, Osaka, Japan; and
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Akira Imoto
2Department of Radiology, National Cerebral and Cardiovascular Center, Suita, Osaka, Japan
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Kazuki Fukuchi
1Division of Medical Technology and Science, Department of Medical Physics and Engineering, Course of Health Science, Osaka University Graduate School of Medicine, Suita, Osaka, Japan; and
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Abstract

Cadmium-zinc-telluride (CZT) detectors have recently been introduced to the field of clinical nuclear cardiology. However, the feasibility of using them for organs other than the heart remains unclear. The aim of this study was to evaluate the potential of a cardiac CZT camera to acquire thyroid and parathyroid images. We used custom-made phantoms and the currently available standard protocols for a CZT camera, instead of a sodium-iodine scintillation (NaI) camera. Methods: Thyroid phantoms with or without parathyroid adenomas were made from agar using radiopharmaceuticals (99mTc or 123I) and imaged using CZT and NaI cameras. Using the CZT camera data, we prepared maximum-intensity-projection (MIP) images and planar-equivalent images. Image counts were compared with those from the NaI camera, and the radioactivity of the phantoms was measured. For parathyroid imaging, 3 different protocols with the NaI camera were tested using MIP images. Results: For thyroid imaging, MIP could provide images as clear as those obtained from the NaI camera. The radioactivity and image counts correlated better for the planar-equivalent images than for the MIP images, especially for 123I. We succeeded in obtaining clear parathyroid adenoma images from MIP images using all 3 protocols. Conclusion: A cardiac CZT camera can effectively perform qualitative and quantitative assessments of the thyroid and parathyroid organs.

  • cadmium zinc telluride (CZT)
  • thyroid imaging
  • parathyroid imaging
  • dual-isotope acquisition

Recently, semiconductor cadmium-zinc-telluride (CZT) detectors have been introduced to the field of cardiovascular nuclear medicine. These CZT-based cameras have better sensitivity and spatial resolution than a conventional γ-camera composed of sodium-iodine scintillation detectors (NaI camera) (1–6). Gambhir et al. reported that a CZT camera has 10-fold better sensitivity and approximately 2-fold better spatial resolution than a NaI camera (6). This marked increase in sensitivity results in a reduction of acquisition time and radiopharmaceutical dose (1–3,5–7).

In addition, a CZT camera has better energy resolution than a NaI camera. Takahashi et al. reported that the energy resolution of a CZT camera is 5% whereas that of a NaI camera is 10% (4). Therefore, CZT SPECT has the potential to separate the primary photons of 99mTc and 123I, which are very close, and provides better-quality dual-tracer simultaneous imaging (8,9).

Although CZT SPECT has the remarkable above-mentioned advantage for nuclear medicine imaging, it is currently applied clinically only for cardiovascular and breast imaging (2). If cardiac CZT SPECT were to be used for focused imaging of other organs, the same advantages are to be expected. To make this possible, however, there are some problems that need to be overcome. First, the current cardiac CZT camera can acquire only tomographic images and not planar images. Second, the field of view of the apparatus is limited (2,3). Even with these limitations, it should be possible to image small and superficial organs using a cardiac CZT camera; therefore, we assumed that the thyroid and parathyroid organs would be suitable for this imaging modality.

The aim of this study was to verify the ability to use cardiac CZT SPECT for imaging of the thyroid and parathyroid. Thyroid and parathyroid adenoma phantoms were fabricated to use in simulation studies, which were performed with current clinical thyroid and parathyroid scintigraphy protocols (10–18).

MATERIALS AND METHODS

Thyroid and Parathyroid Adenoma Phantoms

A thyroid phantom mold was made from potassium alginate and sodium alginate for modeling the normal-sized thyroid glands as a reference (19–21). The length, width, and depth of the thyroid phantom were 60, 20, and 15 mm, respectively. Agar solution and radiopharmaceuticals were then poured into the mold and stirred until the concentration of radioactivity was homogeneous. After 30 min, the agar solidified and was usable as a thyroid phantom. A parathyroid adenoma phantom was made using a similar method. We gave it a diameter of 8 mm and a cylindric height of 7 mm based on the size of parathyroid adenomas resected from patients (22,23). This phantom was fixed to the lower quadrant of the left lobe of the thyroid phantom using a needle. Thyroid phantoms with or without a parathyroid adenoma phantom were fixed in the center of a 1,500-mL cylindric plastic bottle (30-cm circumference) filled with tracer-containing water, which was used to simulate an adult neck with background activity.

Thyroid Imaging

We prepared several thyroid phantoms with various concentrations of 99mTc-pertechnetate or 123I-15-(p-iodophenyl)-3-methylpentadecanoic acid (123I-BMIPP). In Japan, Na123I is available only in the form of a powder contained in a capsule, which is not usable for a phantom study. Therefore, we used 123I-BMIPP, a liquid radiopharmaceutical, to mix homogeneously with agar. In the thyroid phantoms, 1.85–27.8 MBq of 99mTc-pertechnetate or 0.37–3.7 MBq of 123I-BMIPP were included. Plastic bottles were filled with a 0.03 MBq/mL solution of 99mTc-pertechnetate or a 0.006 MBq/mL solution of 123I-BMIPP for background. These background tracer concentrations were determined using a previous thyroid phantom experiment as a reference (24). The neck phantom was placed supine, and imaging was performed first with the CZT camera and then with the NaI camera for 10 min each. After these images had been acquired, the thyroid phantoms were divided into 2 pieces (right and left lobes). The radioactivity of each lobe was then measured using an automatic well counter, and their volumes were measured using a measuring cylinder.

Parathyroid Imaging

We simulated the following 3 acquisition protocols: a dual-phase 99mTc-sestamibi protocol, a dual-tracer 99mTc-sestamibi/99mTc-pertechnetate protocol, and a dual-tracer 99mTc-sestamibi/123I-iodine protocol.

The tracer dose of each phantom in these 3 protocols is shown in Table 1. 99mTc-pertechnetate was substituted for 99mTc-sestamibi in all our phantom studies since both tracers have the same photo energy of 99mTc. All scanning procedures were performed using the CZT camera for 10 min.

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TABLE 1

Tracer Dose of Each Phantom in 3 Parathyroid Imaging Protocols

Dual-Phase 99mTc-Sestamibi Protocol

99mTc-sestamibi accumulates in both parathyroid adenoma and thyroid tissue as a function of blood flow, gland size, and mitochondrial activity (15,17). However, 99mTc-sestamibi washes out more rapidly from thyroid tissue than from parathyroid adenoma (15,16). Because of the difference in washout rate from the 2 tissues, a parathyroid adenoma is detected more clearly in a delayed-phase image than in an early-phase image. Thus, we prepared 2 types of neck phantoms to mimic the early- and delayed-phase neck images.

We determined the radioactivity of the early-phase phantom on the basis of preliminary experiments, including prior thyroid imaging. The radioactivity of the thyroid gland in the delayed-phase phantom was determined using a previous study for reference (25). In that study, the washout rate of 99mTc-sestamibi from thyroid tissue was 0.013 at 180 min after administration. This value was approximately 13% of the radioactivity of the early-phase image (at 20 min after administration). Generally, no biologic washout of 99mTc-sestamibi was observed from the parathyroid adenoma; hence, we calculated the radioactivity of the parathyroid adenoma in the delayed phase on the basis of only physical decay of 99mTc, which was similar to the background. After calibration, these early and delayed neck phantoms were imaged.

Dual-Tracer 99mTc-Sestamibi/99mTc-Pertechnetate Protocol

Although 99mTc-sestamibi accumulates in both parathyroid adenomas and thyroid tissue, 99mTc-pertechnetate accumulates only in thyroid tissue, not in a parathyroid adenoma. Thus, by subtracting a 99mTc-pertechnetate image from a 99mTc-sestamibi image, we could obtain an image of a parathyroid adenoma (16,18).

We constructed 2 types of neck phantoms. A single-tracer phantom to imitate a 99mTc-pertechnetate image contained 99mTc-pertechnetate in the thyroid gland but not in the parathyroid adenoma. A dual-tracer phantom that simulated 99mTc-sestamibi and 99mTc-pertechnetate images contained 99mTc-pertechnetate in both the thyroid gland and the parathyroid adenoma. We set reference markers on the neck phantom and scan bed to reproduce the position of phantoms consistently. First the single-tracer phantom was scanned. We then changed the single-tracer phantom to a dual-tracer phantom using the reference markers as a guide to maintain their scan positions. The dual-tracer phantom was then imaged.

Dual-Tracer 99mTc-Sestamibi/123I-Iodine Protocol

Sodium 123I-iodide accumulates only in thyroid tissue, and 99mTc-sestamibi accumulates in both parathyroid adenoma and thyroid tissue. By subtracting a 123I-iodine image from a 99mTc-sestamibi image, one can isolate the uptake in the parathyroid adenoma (16).

We prepared the thyroid phantom to include both 99mTc-pertechnetate and 123I-BMIPP, whereas the parathyroid adenoma phantom included only 99mTc-pertechnetate. The background included both 99mTc-pertechnetate and 123I-BMIPP. Dual-energy simultaneous acquisition of 99mTc and 123I was performed. After acquisition, we generated 99mTc and 123I window images separately, and subtracted the 123I window image from the 99mTc window image.

Image Acquisition and Processing

In this study, we used D-SPECT (Spectrum Dynamics Medical) for CZT SPECT imaging. D-SPECT is equipped with tungsten parallel-hole collimators and uses list-mode acquisition, with 120 projections per detector. The matrix size of CZT SPECT images was 16 × 64, and the pixel size was 2.26 mm/pixel. CZT SPECT data were reconstructed using ordered-subset expectation maximization, with 7 iterations and 32 subsets. When we performed dual-tracer acquisition with the 99mTc and 123I windows, 2 different energy windows were used simultaneously without scatter correction. The NaI camera (BrightView; Philips) was equipped with a low-energy, high-resolution collimator. The matrix size of the planar image from the NaI camera (NaI planar image) was 256 × 256, and the pixel size was 6.4 mm/pixel. The details of the energy windows used for the CZT and NaI cameras are shown in Table 2.

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TABLE 2

Energy Windows Used with CZT and NaI Cameras

All images were analyzed using freely downloadable software for nuclear medicine (Prominence Processor, version 3.1; Japanese Society of Radiologic Technology) (26). Using this software, we made maximum-intensity-projection (MIP) images from the CZT SPECT data by the same method as that used to make MIP images from the NaI data (27). The maximum intensity along the viewing path was projected. We also used the “planar H/M” application program, which was installed on the D-SPECT workstation (3). This application was programmed to evaluate the heart-to-mediastinum ratio in cardiac 123I-metaiodobenzylguanidine scintigraphy. Each detector of D-SPECT provides a small 2-dimensional (2D) image per angular position. Taken together, all the small 2D images that share the same angle yield wide 2D planar-equivalent (PE) images, which look similar to planar images from a NaI camera.

In thyroid imaging, we set a region of interest on both lobes of the thyroid gland and on the background and measured the mean count per pixel. Image count for the region of interest was calculated by subtracting the background mean count from the region-of-interest mean count. In parathyroid imaging, image subtraction was performed using dual-tracer protocols on the MIP image. We adjusted the phantom position and uptake intensity between different photopeak images for subtraction using the software, and subjectively satisfactory images for diagnosis were thus obtained.

Statistical Analysis

The data were analyzed using a website for statistical computation (VassarStats; http://vassarstats.net/). Correlations between the radioactivity and image counts were assessed using the Pearson correlation coefficient (r). Differences in correlation coefficients between images were assessed using the Fisher transformation test. A 2-tailed P value of less than 0.05 was considered statistically significant.

RESULTS

Thyroid Imaging

Typical images obtained using 3 different methods are shown in Figure 1. MIP images could depict the thyroid gland with good image quality; however, PE images were inferior to MIP and NaI planar images in both the 99mTc and the 123I windows.

FIGURE 1.
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FIGURE 1.

Typical thyroid images using 99mTc (top) and 123I (bottom) tracers. Shown are MIP images (left), PE images (middle), and NaI planar images (right).

The relationship between radioactivity and image counts is shown in Figures 2 and 3. MIP images and PE images showed statistically significant correlations between the radioactivity and image counts for both 99mTc (r = 0.93 and 0.97, respectively; P < 0.05) and 123I images (r = 0.89 and 0.99, respectively; P < 0.05). Similar results were obtained using the NaI planar images for the 99mTc and 123I windows (r = 0.98 and 0.99, respectively; P < 0.05). The correlations between radioactivity and image counts of 99mTc tracer did not significantly differ between MIP and PE images (P = 0.54). However, with the 123I tracer, PE images had significantly stronger correlations than the MIP images (P < 0.05).

FIGURE 2.
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FIGURE 2.

Relationship between image counts and radioactivity of 99mTc-containing thyroid phantoms: NaI planar image (A), MIP image (B), and PE image (C).

FIGURE 3.
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FIGURE 3.

Relationship between image counts and radioactivity of 123I thyroid phantoms: NaI planar image (A), MIP image (B), and PE image (C).

Parathyroid Imaging

Figure 4 shows the dual-phase 99mTc-sestamibi protocol. The early-phase image depicted tracer uptake in the thyroid gland, with regional emphasis on the parathyroid adenoma in the lower quadrant of the left thyroid lobe. A clear accumulation in the parathyroid adenoma was visible in the simulated delayed-phase image.

FIGURE 4.
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FIGURE 4.

Typical early (A) and delayed (B) images from dual-phase 99mTc-sestamibi protocol using MIP. Clear accumulation of tracer is visible in lower quadrant of left thyroid lobe in delayed image.

Figure 5 shows the dual-tracer 99mTc-sestamibi/99mTc-pertechnetate protocol. Dual-tracer images showed tracer uptake in the thyroid gland and parathyroid adenoma, whereas single-tracer images showed tracer uptake in the thyroid gland only. Subtraction of the single-tracer image from the dual-tracer image showed the parathyroid adenoma unmistakably.

FIGURE 5.
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FIGURE 5.

Typical single-tracer (A), dual-tracer (B), and subtracted (C) images from 99mTc-sestamibi/99mTc-pertechnetate protocol using MIP. After single-tracer image was subtracted from dual-tracer image, solitary parathyroid adenoma was clearly visible.

Figure 6 shows the dual-tracer 99mTc-sestamibi/123I-iodine protocol. The 123I photopeak image showed tracer uptake in the thyroid gland. In contrast, the 99mTc photopeak image showed tracer uptake in the thyroid gland and parathyroid adenoma; however, identifying the parathyroid adenoma was difficult. After subtraction of the 123I photopeak image from the 99mTc photopeak image, the parathyroid adenoma was discernable.

FIGURE 6.
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FIGURE 6.

Representative 99mTc photopeak (A), 123I photopeak (B), and subtracted (C) parathyroid images from 99mTc-sestamibi/123I-iodine protocol using MIP. 99mTc tracer is seen in thyroid and parathyroid glands, and 123I is distributed in thyroid tissue. Parathyroid adenoma was then clearly visualized by subtracting 123I image from 99mTc image.

DISCUSSION

Thyroid Imaging and Quantitative Analysis

Cardiac CZT SPECT does not directly generate planar images, and most thyroid imaging is performed using a 2D approach. Thus, we needed to convert tomographic data to 2D data for a corresponding thyroid assessment. After an MIP image was generated, it could depict the thyroid gland as effectively as images from a NaI camera. In contrast, PE images were not adequate for visual assessment of the thyroid gland. The reason for this phenomenon is unclear, because this technique is theoretically similar to that performed with a NaI camera (3). At the least it can be concluded that an MIP image needs to be generated for visual assessment of the thyroid gland using cardiac CZT SPECT.

Image counts measured by setting a region of interest on the CZT SPECT and NaI scans were significantly correlated in both the 99mTc and the 123I images. However, a detailed inspection revealed that in the MIP images, the regression line of the correlation did not cross the origin of the coordinates. In an MIP-image–visualized plane, because the voxels with maximum intensity that fall in the way of parallel rays trace from the viewpoint to the plane of projection, the count data might be overestimated. Thus, the approximate lines of the MIP image shifted to the higher-count area. In addition, the PE images produced stronger correlations of radioactivity with image counts for the 123I tracer than for the 99mTc tracer. PE images were developed especially for calculation of the mean pixel counts of 123I tracer (3). This property may be the reason for better quantification for the 123I tracer than for the 99mTc tracer.

Parathyroid Imaging

In this study, we obtained clear parathyroid adenoma images in our phantom experiments that faithfully reproduced 3 different acquisition protocols using a CZT camera (16).

With the dual-phase 99mTc-sestamibi protocol, a parathyroid adenoma can be visualized in a delayed-phase image. Because a dual-phase 99mTc-sestamibi protocol is the most popular imaging protocol for parathyroid adenomas, our result indicates that this protocol may be one of the most feasible methods for the imaging of other organs using a CZT camera instead of an NaI camera. To clarify this issue, further studies that include various sizes and radioactivities of a parathyroid adenoma are needed.

In the dual-tracer 99mTc-sestamibi/99mTc-pertechnetate protocol, we also obtained a good image of a parathyroid adenoma. Although several position gaps appeared between 2 different neck phantoms, software-based registration can permit high-quality subtraction to clearly emphasize a parathyroid adenoma. Thus, this protocol also seems to be acceptable for parathyroid imaging by CZT SPECT. In the clinical setting, these 2 images are obtained without changing a patient’s neck position, unlike in our study; thus, a much clearer and motionless parathyroid image would be expected in human imaging.

Because both images were acquired simultaneously, in the dual-tracer 99mTc-sestamibi/123I-iodine protocol a parathyroid adenoma was clearly visualized by subtracting the 123I photopeak image from the 99mTc photopeak image. Although the emission energies of these tracers are close and crosstalk has an influence on image quality, currently this protocol is often performed in routine practice using a NaI camera. Energy resolution is better for a CZT camera than for a NaI camera; thus, CZT SPECT is theoretically more suitable for the dual-tracer protocol using 99mTc and 123I. Tunninen et al. reported that the 99mTc-sestamibi/123I-iodine dual-tracer protocol is superior to the 99mTc-sestamibi single-tracer protocol (14). Taieb et al. also reported a high sensitivity using 99mTc-sestamibi/123I-iodine subtraction scintigraphy (28). Therefore, the dual-tracer 99mTc-sestamibi/123I-iodine acquisition using CZT SPECT seems to be the best protocol for nuclear medicine imaging of the parathyroid. Further clinical studies are needed to clarify the clinical impact of this technology.

Limitations

In this study, we used the same tracer dose and acquisition time for both the CZT and the NaI cameras because this preliminary study needed to compare these 2 modalities under the same conditions. Theoretically, a protocol with a lower dose or shorter acquisition time can be used with CZT SPECT. Therefore, in future studies the tracer dose and acquisition time should be reduced to take advantage of CZT SPECT. Because the dual-tracer protocol increases the radiation exposure, we should attempt to reduce this with CZT SPECT technology.

It is well known that a certain proportion of patients with hyperparathyroidism have an ectopic parathyroid adenoma (29). If an ectopic parathyroid adenoma were in the mediastinum, CZT SPECT with a limited field of view would not cover both the neck and the mediastinum using one-time scanning. Typically, CZT SPECT is used for cardiac imaging; thus, it would be acceptable to perform additional mediastinal imaging as is done in a cardiac study. However, further research is required.

CONCLUSION

To our knowledge, this is the first study that attempted imaging of the neck region using cardiac CZT SPECT. A combination of MIP and PE images appears to be useful for visual and quantitative assessment of thyroid disease. MIP images can be applied for the detection of parathyroid adenomas using several different protocols, including the dual-tracer method.

DISCLOSURE

No potential conflict of interest relevant to this article was reported.

Acknowledgments

We thank Shoji Nono of the Department of Radiology, National Cerebral and Cardiovascular Center, for his technical assistance.

Footnotes

  • Published online Nov. 10, 2017.

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  • Received for publication July 10, 2017.
  • Accepted for publication September 23, 2017.
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Journal of Nuclear Medicine Technology: 46 (1)
Journal of Nuclear Medicine Technology
Vol. 46, Issue 1
March 1, 2018
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Imaging of the Thyroid and Parathyroid Using a Cardiac Cadmium-Zinc-Telluride Camera: Phantom Studies
Yosuke Miyazaki, Yasuhiro Kato, Akira Imoto, Kazuki Fukuchi
Journal of Nuclear Medicine Technology Mar 2018, 46 (1) 39-44; DOI: 10.2967/jnmt.117.199042

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Imaging of the Thyroid and Parathyroid Using a Cardiac Cadmium-Zinc-Telluride Camera: Phantom Studies
Yosuke Miyazaki, Yasuhiro Kato, Akira Imoto, Kazuki Fukuchi
Journal of Nuclear Medicine Technology Mar 2018, 46 (1) 39-44; DOI: 10.2967/jnmt.117.199042
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Keywords

  • cadmium zinc telluride (CZT)
  • thyroid imaging
  • parathyroid imaging
  • dual-isotope acquisition
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