A Monte Carlo study on 223Ra imaging for unsealed radionuclide therapy

Research output: Contribution to journalArticle

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Abstract

Purpose: Radium-223 (223Ra), an α-emitting radionuclide, is used in unsealed radionuclide therapy for metastatic bone tumors. The demand for qualitative 223Ra imaging is growing to optimize dosimetry. The authors simulated 223Ra imaging using an in-house Monte Carlo simulation code and investigated the feasibility and utility of 223Ra imaging. Methods: The Monte Carlo code comprises two modules, HEXAGON and NAI. The HEXAGON code simulates the photon and electron interactions in the tissues and collimator, and the NAI code simulates the response of the NaI detector system. A 3D numeric phantom created using computed tomography images of a chest phantom was installed in the HEXAGON code. 223Ra accumulated in a part of the spine, and three x-rays and 19 γ rays between 80 and 450 keV were selected as the emitted photons. To evaluate the quality of the 223Ra imaging, the authors also simulated technetium-99m (99mTc) imaging under the same conditions and compared the results. Results: The sensitivities of the three photopeaks were 147 counts per unit of source activity (cps MBq-1; photopeak: 84 keV, full width of energy window: 20%), 166 cps MBq-1 (154 keV, 15%), and 158 cps MBq-1 (270 keV, 10%) for a low-energy general-purpose (LEGP) collimator, and those for the medium-energy general-purpose (MEGP) collimator were 33, 13, and 8.0 cps MBq-1, respectively. In the case of 99mTc, the sensitivity was 55 cps MBq-1 (141 keV, 20%) for LEGP and 52 cps MBq-1 for MEGP. The fractions of unscattered photons of the total photons reflecting the image quality were 0.09 (84 keV), 0.03 (154 keV), and 0.02 (270 keV) for the LEGP collimator and 0.41, 0.25, and 0.50 for the MEGP collimator, respectively. Conversely, this fraction was approximately 0.65 for the simulated 99mTc imaging. The sensitivity with the LEGP collimator appeared very high. However, almost all of the counts were because of photons that penetrated or were scattered in the collimator; therefore, the proportions of unscattered photons were small. Conclusions: Their simulation study revealed that the most promising scheme for 223Ra imaging is an 84-keV window using an MEGP collimator. The sensitivity of the photopeaks above 100 keV is too low for 223Ra imaging. A comparison of the fractions of unscattered photons reveals that the sensitivity and image quality are approximately two-thirds of those for 99mTc imaging.

Original languageEnglish
Pages (from-to)2965-2974
Number of pages10
JournalMedical physics
Volume43
Issue number6
DOIs
Publication statusPublished - Jun 1 2016

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Photons
Radionuclide Imaging
Radioisotopes
Therapeutics
Monte Carlo Method
Radium
Technetium
Spine
Thorax
Tomography
X-Rays
Electrons
Bone and Bones
Neoplasms

All Science Journal Classification (ASJC) codes

  • Biophysics
  • Radiology Nuclear Medicine and imaging

Cite this

A Monte Carlo study on 223Ra imaging for unsealed radionuclide therapy. / Takahashi, Akihiko; Miwa, Kenta; Sasaki, Masayuki; Baba, Shingo.

In: Medical physics, Vol. 43, No. 6, 01.06.2016, p. 2965-2974.

Research output: Contribution to journalArticle

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title = "A Monte Carlo study on 223Ra imaging for unsealed radionuclide therapy",
abstract = "Purpose: Radium-223 (223Ra), an α-emitting radionuclide, is used in unsealed radionuclide therapy for metastatic bone tumors. The demand for qualitative 223Ra imaging is growing to optimize dosimetry. The authors simulated 223Ra imaging using an in-house Monte Carlo simulation code and investigated the feasibility and utility of 223Ra imaging. Methods: The Monte Carlo code comprises two modules, HEXAGON and NAI. The HEXAGON code simulates the photon and electron interactions in the tissues and collimator, and the NAI code simulates the response of the NaI detector system. A 3D numeric phantom created using computed tomography images of a chest phantom was installed in the HEXAGON code. 223Ra accumulated in a part of the spine, and three x-rays and 19 γ rays between 80 and 450 keV were selected as the emitted photons. To evaluate the quality of the 223Ra imaging, the authors also simulated technetium-99m (99mTc) imaging under the same conditions and compared the results. Results: The sensitivities of the three photopeaks were 147 counts per unit of source activity (cps MBq-1; photopeak: 84 keV, full width of energy window: 20{\%}), 166 cps MBq-1 (154 keV, 15{\%}), and 158 cps MBq-1 (270 keV, 10{\%}) for a low-energy general-purpose (LEGP) collimator, and those for the medium-energy general-purpose (MEGP) collimator were 33, 13, and 8.0 cps MBq-1, respectively. In the case of 99mTc, the sensitivity was 55 cps MBq-1 (141 keV, 20{\%}) for LEGP and 52 cps MBq-1 for MEGP. The fractions of unscattered photons of the total photons reflecting the image quality were 0.09 (84 keV), 0.03 (154 keV), and 0.02 (270 keV) for the LEGP collimator and 0.41, 0.25, and 0.50 for the MEGP collimator, respectively. Conversely, this fraction was approximately 0.65 for the simulated 99mTc imaging. The sensitivity with the LEGP collimator appeared very high. However, almost all of the counts were because of photons that penetrated or were scattered in the collimator; therefore, the proportions of unscattered photons were small. Conclusions: Their simulation study revealed that the most promising scheme for 223Ra imaging is an 84-keV window using an MEGP collimator. The sensitivity of the photopeaks above 100 keV is too low for 223Ra imaging. A comparison of the fractions of unscattered photons reveals that the sensitivity and image quality are approximately two-thirds of those for 99mTc imaging.",
author = "Akihiko Takahashi and Kenta Miwa and Masayuki Sasaki and Shingo Baba",
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AU - Takahashi, Akihiko

AU - Miwa, Kenta

AU - Sasaki, Masayuki

AU - Baba, Shingo

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N2 - Purpose: Radium-223 (223Ra), an α-emitting radionuclide, is used in unsealed radionuclide therapy for metastatic bone tumors. The demand for qualitative 223Ra imaging is growing to optimize dosimetry. The authors simulated 223Ra imaging using an in-house Monte Carlo simulation code and investigated the feasibility and utility of 223Ra imaging. Methods: The Monte Carlo code comprises two modules, HEXAGON and NAI. The HEXAGON code simulates the photon and electron interactions in the tissues and collimator, and the NAI code simulates the response of the NaI detector system. A 3D numeric phantom created using computed tomography images of a chest phantom was installed in the HEXAGON code. 223Ra accumulated in a part of the spine, and three x-rays and 19 γ rays between 80 and 450 keV were selected as the emitted photons. To evaluate the quality of the 223Ra imaging, the authors also simulated technetium-99m (99mTc) imaging under the same conditions and compared the results. Results: The sensitivities of the three photopeaks were 147 counts per unit of source activity (cps MBq-1; photopeak: 84 keV, full width of energy window: 20%), 166 cps MBq-1 (154 keV, 15%), and 158 cps MBq-1 (270 keV, 10%) for a low-energy general-purpose (LEGP) collimator, and those for the medium-energy general-purpose (MEGP) collimator were 33, 13, and 8.0 cps MBq-1, respectively. In the case of 99mTc, the sensitivity was 55 cps MBq-1 (141 keV, 20%) for LEGP and 52 cps MBq-1 for MEGP. The fractions of unscattered photons of the total photons reflecting the image quality were 0.09 (84 keV), 0.03 (154 keV), and 0.02 (270 keV) for the LEGP collimator and 0.41, 0.25, and 0.50 for the MEGP collimator, respectively. Conversely, this fraction was approximately 0.65 for the simulated 99mTc imaging. The sensitivity with the LEGP collimator appeared very high. However, almost all of the counts were because of photons that penetrated or were scattered in the collimator; therefore, the proportions of unscattered photons were small. Conclusions: Their simulation study revealed that the most promising scheme for 223Ra imaging is an 84-keV window using an MEGP collimator. The sensitivity of the photopeaks above 100 keV is too low for 223Ra imaging. A comparison of the fractions of unscattered photons reveals that the sensitivity and image quality are approximately two-thirds of those for 99mTc imaging.

AB - Purpose: Radium-223 (223Ra), an α-emitting radionuclide, is used in unsealed radionuclide therapy for metastatic bone tumors. The demand for qualitative 223Ra imaging is growing to optimize dosimetry. The authors simulated 223Ra imaging using an in-house Monte Carlo simulation code and investigated the feasibility and utility of 223Ra imaging. Methods: The Monte Carlo code comprises two modules, HEXAGON and NAI. The HEXAGON code simulates the photon and electron interactions in the tissues and collimator, and the NAI code simulates the response of the NaI detector system. A 3D numeric phantom created using computed tomography images of a chest phantom was installed in the HEXAGON code. 223Ra accumulated in a part of the spine, and three x-rays and 19 γ rays between 80 and 450 keV were selected as the emitted photons. To evaluate the quality of the 223Ra imaging, the authors also simulated technetium-99m (99mTc) imaging under the same conditions and compared the results. Results: The sensitivities of the three photopeaks were 147 counts per unit of source activity (cps MBq-1; photopeak: 84 keV, full width of energy window: 20%), 166 cps MBq-1 (154 keV, 15%), and 158 cps MBq-1 (270 keV, 10%) for a low-energy general-purpose (LEGP) collimator, and those for the medium-energy general-purpose (MEGP) collimator were 33, 13, and 8.0 cps MBq-1, respectively. In the case of 99mTc, the sensitivity was 55 cps MBq-1 (141 keV, 20%) for LEGP and 52 cps MBq-1 for MEGP. The fractions of unscattered photons of the total photons reflecting the image quality were 0.09 (84 keV), 0.03 (154 keV), and 0.02 (270 keV) for the LEGP collimator and 0.41, 0.25, and 0.50 for the MEGP collimator, respectively. Conversely, this fraction was approximately 0.65 for the simulated 99mTc imaging. The sensitivity with the LEGP collimator appeared very high. However, almost all of the counts were because of photons that penetrated or were scattered in the collimator; therefore, the proportions of unscattered photons were small. Conclusions: Their simulation study revealed that the most promising scheme for 223Ra imaging is an 84-keV window using an MEGP collimator. The sensitivity of the photopeaks above 100 keV is too low for 223Ra imaging. A comparison of the fractions of unscattered photons reveals that the sensitivity and image quality are approximately two-thirds of those for 99mTc imaging.

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