Rational evaluation of the therapeutic effect and dosimetry of auger electrons for radionuclide therapy in a cell culture model
Objective Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models...
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Published in | Annals of nuclear medicine Vol. 32; no. 2; pp. 114 - 122 |
---|---|
Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
Published |
Tokyo
Springer Japan
01.02.2018
Springer Nature B.V |
Subjects | |
Online Access | Get full text |
ISSN | 0914-7187 1864-6433 1864-6433 |
DOI | 10.1007/s12149-017-1225-9 |
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Abstract | Objective
Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models and conducted a dosimetry simulation using radioiodine-labeled metaiodobenzylguanidine (MIBG) as a model compound.
Methods
We evaluated the cellular uptake of
125
I-MIBG and the therapeutic effects of
125
I- and
131
I-MIBG in 2D and 3D PC-12 cell culture models. We used a Monte Carlo simulation code (PHITS) to calculate the absorbed radiation dose of
125
I or
131
I in computer simulation models for 2D and 3D cell cultures. In the dosimetry calculation for the 3D model, several distribution patterns of radionuclide were applied.
Results
A higher cumulative dose was observed in the 3D model due to the prolonged retention of MIBG compared to the 2D model. However,
125
I-MIBG showed a greater therapeutic effect in the 2D model compared to the 3D model (respective EC
50
values in the 2D and 3D models: 86.9 and 303.9 MBq/cell), whereas
131
I-MIBG showed the opposite result (respective EC
50
values in the 2D and 3D models: 49.4 and 30.2 MBq/cell). The therapeutic effect of
125
I-MIBG was lower than that of
131
I-MIBG in both models, but the radionuclide-derived difference was smaller in the 2D model. The dosimetry simulation with PHITS revealed the influence of the radiation quality, the crossfire effect, radionuclide distribution, and tumor shape on the absorbed dose. Application of the heterogeneous distribution series dramatically changed the radiation dose distribution of
125
I-MIBG, and mitigated the difference between the estimated and measured therapeutic effects of
125
I-MIBG.
Conclusions
The therapeutic effect of
125
I-MIBG was comparable to that of
131
I-MIBG in the 2D model, but the efficacy was inferior to that of
131
I-MIBG in the 3D model, since the crossfire effect is negligible and the homogeneous distribution of radionuclides was insufficient. Thus, auger electrons would be suitable for treating small-sized tumors. The design of radiopharmaceuticals with auger electron emitters requires particularly careful consideration of achieving a homogeneous distribution of the compound in the tumor. |
---|---|
AbstractList | Objective
Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models and conducted a dosimetry simulation using radioiodine-labeled metaiodobenzylguanidine (MIBG) as a model compound.
Methods
We evaluated the cellular uptake of
125
I-MIBG and the therapeutic effects of
125
I- and
131
I-MIBG in 2D and 3D PC-12 cell culture models. We used a Monte Carlo simulation code (PHITS) to calculate the absorbed radiation dose of
125
I or
131
I in computer simulation models for 2D and 3D cell cultures. In the dosimetry calculation for the 3D model, several distribution patterns of radionuclide were applied.
Results
A higher cumulative dose was observed in the 3D model due to the prolonged retention of MIBG compared to the 2D model. However,
125
I-MIBG showed a greater therapeutic effect in the 2D model compared to the 3D model (respective EC
50
values in the 2D and 3D models: 86.9 and 303.9 MBq/cell), whereas
131
I-MIBG showed the opposite result (respective EC
50
values in the 2D and 3D models: 49.4 and 30.2 MBq/cell). The therapeutic effect of
125
I-MIBG was lower than that of
131
I-MIBG in both models, but the radionuclide-derived difference was smaller in the 2D model. The dosimetry simulation with PHITS revealed the influence of the radiation quality, the crossfire effect, radionuclide distribution, and tumor shape on the absorbed dose. Application of the heterogeneous distribution series dramatically changed the radiation dose distribution of
125
I-MIBG, and mitigated the difference between the estimated and measured therapeutic effects of
125
I-MIBG.
Conclusions
The therapeutic effect of
125
I-MIBG was comparable to that of
131
I-MIBG in the 2D model, but the efficacy was inferior to that of
131
I-MIBG in the 3D model, since the crossfire effect is negligible and the homogeneous distribution of radionuclides was insufficient. Thus, auger electrons would be suitable for treating small-sized tumors. The design of radiopharmaceuticals with auger electron emitters requires particularly careful consideration of achieving a homogeneous distribution of the compound in the tumor. Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models and conducted a dosimetry simulation using radioiodine-labeled metaiodobenzylguanidine (MIBG) as a model compound. We evaluated the cellular uptake of I-MIBG and the therapeutic effects of I- and I-MIBG in 2D and 3D PC-12 cell culture models. We used a Monte Carlo simulation code (PHITS) to calculate the absorbed radiation dose of I or I in computer simulation models for 2D and 3D cell cultures. In the dosimetry calculation for the 3D model, several distribution patterns of radionuclide were applied. A higher cumulative dose was observed in the 3D model due to the prolonged retention of MIBG compared to the 2D model. However, I-MIBG showed a greater therapeutic effect in the 2D model compared to the 3D model (respective EC values in the 2D and 3D models: 86.9 and 303.9 MBq/cell), whereas I-MIBG showed the opposite result (respective EC values in the 2D and 3D models: 49.4 and 30.2 MBq/cell). The therapeutic effect of I-MIBG was lower than that of I-MIBG in both models, but the radionuclide-derived difference was smaller in the 2D model. The dosimetry simulation with PHITS revealed the influence of the radiation quality, the crossfire effect, radionuclide distribution, and tumor shape on the absorbed dose. Application of the heterogeneous distribution series dramatically changed the radiation dose distribution of I-MIBG, and mitigated the difference between the estimated and measured therapeutic effects of I-MIBG. The therapeutic effect of I-MIBG was comparable to that of I-MIBG in the 2D model, but the efficacy was inferior to that of I-MIBG in the 3D model, since the crossfire effect is negligible and the homogeneous distribution of radionuclides was insufficient. Thus, auger electrons would be suitable for treating small-sized tumors. The design of radiopharmaceuticals with auger electron emitters requires particularly careful consideration of achieving a homogeneous distribution of the compound in the tumor. ObjectiveRadionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models and conducted a dosimetry simulation using radioiodine-labeled metaiodobenzylguanidine (MIBG) as a model compound.MethodsWe evaluated the cellular uptake of 125I-MIBG and the therapeutic effects of 125I- and 131I-MIBG in 2D and 3D PC-12 cell culture models. We used a Monte Carlo simulation code (PHITS) to calculate the absorbed radiation dose of 125I or 131I in computer simulation models for 2D and 3D cell cultures. In the dosimetry calculation for the 3D model, several distribution patterns of radionuclide were applied.ResultsA higher cumulative dose was observed in the 3D model due to the prolonged retention of MIBG compared to the 2D model. However, 125I-MIBG showed a greater therapeutic effect in the 2D model compared to the 3D model (respective EC50 values in the 2D and 3D models: 86.9 and 303.9 MBq/cell), whereas 131I-MIBG showed the opposite result (respective EC50 values in the 2D and 3D models: 49.4 and 30.2 MBq/cell). The therapeutic effect of 125I-MIBG was lower than that of 131I-MIBG in both models, but the radionuclide-derived difference was smaller in the 2D model. The dosimetry simulation with PHITS revealed the influence of the radiation quality, the crossfire effect, radionuclide distribution, and tumor shape on the absorbed dose. Application of the heterogeneous distribution series dramatically changed the radiation dose distribution of 125I-MIBG, and mitigated the difference between the estimated and measured therapeutic effects of 125I-MIBG.ConclusionsThe therapeutic effect of 125I-MIBG was comparable to that of 131I-MIBG in the 2D model, but the efficacy was inferior to that of 131I-MIBG in the 3D model, since the crossfire effect is negligible and the homogeneous distribution of radionuclides was insufficient. Thus, auger electrons would be suitable for treating small-sized tumors. The design of radiopharmaceuticals with auger electron emitters requires particularly careful consideration of achieving a homogeneous distribution of the compound in the tumor. Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models and conducted a dosimetry simulation using radioiodine-labeled metaiodobenzylguanidine (MIBG) as a model compound.OBJECTIVERadionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we evaluated the usefulness of an auger electron emitter and compared it with that of a beta emitter for tumor treatment in in vitro models and conducted a dosimetry simulation using radioiodine-labeled metaiodobenzylguanidine (MIBG) as a model compound.We evaluated the cellular uptake of 125I-MIBG and the therapeutic effects of 125I- and 131I-MIBG in 2D and 3D PC-12 cell culture models. We used a Monte Carlo simulation code (PHITS) to calculate the absorbed radiation dose of 125I or 131I in computer simulation models for 2D and 3D cell cultures. In the dosimetry calculation for the 3D model, several distribution patterns of radionuclide were applied.METHODSWe evaluated the cellular uptake of 125I-MIBG and the therapeutic effects of 125I- and 131I-MIBG in 2D and 3D PC-12 cell culture models. We used a Monte Carlo simulation code (PHITS) to calculate the absorbed radiation dose of 125I or 131I in computer simulation models for 2D and 3D cell cultures. In the dosimetry calculation for the 3D model, several distribution patterns of radionuclide were applied.A higher cumulative dose was observed in the 3D model due to the prolonged retention of MIBG compared to the 2D model. However, 125I-MIBG showed a greater therapeutic effect in the 2D model compared to the 3D model (respective EC50 values in the 2D and 3D models: 86.9 and 303.9 MBq/cell), whereas 131I-MIBG showed the opposite result (respective EC50 values in the 2D and 3D models: 49.4 and 30.2 MBq/cell). The therapeutic effect of 125I-MIBG was lower than that of 131I-MIBG in both models, but the radionuclide-derived difference was smaller in the 2D model. The dosimetry simulation with PHITS revealed the influence of the radiation quality, the crossfire effect, radionuclide distribution, and tumor shape on the absorbed dose. Application of the heterogeneous distribution series dramatically changed the radiation dose distribution of 125I-MIBG, and mitigated the difference between the estimated and measured therapeutic effects of 125I-MIBG.RESULTSA higher cumulative dose was observed in the 3D model due to the prolonged retention of MIBG compared to the 2D model. However, 125I-MIBG showed a greater therapeutic effect in the 2D model compared to the 3D model (respective EC50 values in the 2D and 3D models: 86.9 and 303.9 MBq/cell), whereas 131I-MIBG showed the opposite result (respective EC50 values in the 2D and 3D models: 49.4 and 30.2 MBq/cell). The therapeutic effect of 125I-MIBG was lower than that of 131I-MIBG in both models, but the radionuclide-derived difference was smaller in the 2D model. The dosimetry simulation with PHITS revealed the influence of the radiation quality, the crossfire effect, radionuclide distribution, and tumor shape on the absorbed dose. Application of the heterogeneous distribution series dramatically changed the radiation dose distribution of 125I-MIBG, and mitigated the difference between the estimated and measured therapeutic effects of 125I-MIBG.The therapeutic effect of 125I-MIBG was comparable to that of 131I-MIBG in the 2D model, but the efficacy was inferior to that of 131I-MIBG in the 3D model, since the crossfire effect is negligible and the homogeneous distribution of radionuclides was insufficient. Thus, auger electrons would be suitable for treating small-sized tumors. The design of radiopharmaceuticals with auger electron emitters requires particularly careful consideration of achieving a homogeneous distribution of the compound in the tumor.CONCLUSIONSThe therapeutic effect of 125I-MIBG was comparable to that of 131I-MIBG in the 2D model, but the efficacy was inferior to that of 131I-MIBG in the 3D model, since the crossfire effect is negligible and the homogeneous distribution of radionuclides was insufficient. Thus, auger electrons would be suitable for treating small-sized tumors. The design of radiopharmaceuticals with auger electron emitters requires particularly careful consideration of achieving a homogeneous distribution of the compound in the tumor. |
Author | Shinohara, Ayaka Sakashita, Tetsuya Sato, Tatsuhiko Ishioka, Noriko S. Tsushima, Yoshito Yamaguchi, Aiko Hanaoka, Hirofumi |
Author_xml | – sequence: 1 givenname: Ayaka surname: Shinohara fullname: Shinohara, Ayaka organization: Department of Heavy Ion Beam Medical Physics and Biology, Gunma University Graduate School of Medicine – sequence: 2 givenname: Hirofumi orcidid: 0000-0003-2421-7397 surname: Hanaoka fullname: Hanaoka, Hirofumi email: hanaokah@gunma-u.ac.jp organization: Department of Bioimaging Information Analysis, Gunma University Graduate School of Medicine – sequence: 3 givenname: Tetsuya surname: Sakashita fullname: Sakashita, Tetsuya organization: Quantum Beam Science Research Directorate, National Institutes for Quantum and Radiological Science and Technology – sequence: 4 givenname: Tatsuhiko surname: Sato fullname: Sato, Tatsuhiko organization: Nuclear Science and Engineering Center, Japan Atomic Energy Agency – sequence: 5 givenname: Aiko surname: Yamaguchi fullname: Yamaguchi, Aiko organization: Department of Bioimaging Information Analysis, Gunma University Graduate School of Medicine – sequence: 6 givenname: Noriko S. surname: Ishioka fullname: Ishioka, Noriko S. organization: Quantum Beam Science Research Directorate, National Institutes for Quantum and Radiological Science and Technology – sequence: 7 givenname: Yoshito surname: Tsushima fullname: Tsushima, Yoshito organization: Department of Diagnostic Radiology and Nuclear Medicine, Gunma University Graduate School of Medicine, Research Program for Diagnostic and Molecular Imaging, Division of Integrated Oncology Research, Gunma University Initiative for Advanced Research (GIAR), Gunma University Graduate School of Medicine |
BackLink | https://www.ncbi.nlm.nih.gov/pubmed/29238922$$D View this record in MEDLINE/PubMed |
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CitedBy_id | crossref_primary_10_1038_s41598_021_85635_2 crossref_primary_10_3390_onco1020011 crossref_primary_10_1007_s12194_021_00628_0 crossref_primary_10_1051_radiopro_2023020 crossref_primary_10_1080_09553002_2020_1831706 crossref_primary_10_1007_s12149_020_01548_6 crossref_primary_10_3389_fphar_2018_00952 |
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Keywords | Radionuclide therapy Computer simulation 3D cell culture model I-Metaiodobenzylguanidine I-MIBG Auger electron emitter 125/131I-Metaiodobenzylguanidine (125/131I-MIBG) |
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Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low.... Radionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here we... ObjectiveRadionuclide therapy with low-energy auger electron emitters may provide high antitumor efficacy while keeping the toxicity to normal organs low. Here... |
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SubjectTerms | Anticancer properties Antitumor activity Augers Cell culture Cell Survival - radiation effects Cells, Cultured Computer simulation Dosimeters Dosimetry Electrons Emitters (electron) Imaging Iodine 131 Iodine Radioisotopes - therapeutic use Mathematical models Medicine Medicine & Public Health Monte Carlo Method Monte Carlo simulation Nuclear Medicine Organs Original Article Personal computers Radiation dosage Radiation therapy Radioisotopes Radiology Radiometry Radiotherapy Therapy Three dimensional models Toxicity Treatment Outcome Tumors Two dimensional models |
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Title | Rational evaluation of the therapeutic effect and dosimetry of auger electrons for radionuclide therapy in a cell culture model |
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