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Journal of Nuclear Medicine Vol. 47 No. 5 807-814
© 2006 by Society of Nuclear Medicine


Basic Science Investigation

Electron- and Positron-Emitting Radiolanthanides for Therapy: Aspects of Dosimetry and Production

Helena Uusijärvi1, Peter Bernhardt1, Frank Rösch2, Helmut R. Maecke3 and Eva Forssell-Aronsson1

1 Department of Radiation Physics, Göteborg University, Sahlgrenska University Hospital, Göteborg, Sweden; 2 Institute for Nuclear Chemistry, Johannes Gutenberg-University Mainz, Mainz, Germany; and 3 Division of Radiological Chemistry, University Hospital Basel, Basel, Switzerland

Correspondence: For correspondence or reprints contact: Helena Uusijärvi, Department of Radiation Physics, Göteborg University, Sahlgrenska University Hospital, SE-413 45 Göteborg, Sweden. E-mail: helena.uusijarvi{at}radfys.gu.se

All lanthanides have similar chemical properties regarding labeling. Therefore, radiolanthanides that have been used for therapy, such as 153Sm and 177Lu, might easily be replaced with other radiolanthanides. The aim of this work was to investigate the suitability of electron- and positron-emitting radiolanthanides for radionuclide therapy with reference to dosimetry and production possibilities. Methods: Radiolanthanides with half-lives of 1 h to 15 d, stable or long-lived daughters, and limited photon emission were selected. The ratio of the absorbed dose rate to the tumors and the normal tissue (Formula) was calculated for different tumor sizes and compared with the Formula values for 90Y and 131I. The normal tissue and tumors were simulated as an ellipsoid and spheres, respectively. The Formula values depend on the physical parameters of the radionuclides, the tumor size, and the ratio between the activity concentrations in the tumor and normal tissue (TNC). Results: 153Sm, 161Tb, 169Er, 175Yb, and 177Lu had the highest Formula values for most of the tumor sizes studied. Among these radiolanthanides, 161Tb and 177Lu are the only ones that can be produced no-carrier-added (nca) and with high specific activities. The Auger-electron emitters 161Ho and 167Tm had high Formula values for tumors weighing less than 1 mg and can be produced nca and with high specific activities. 142Pr, 145Pr, and 166Ho showed Formula values similar to those of 90Y. 166Ho is generator produced and can be obtained nca and at high specific activities. 143Pr, 149Pm, 150Eu, 159Gd, 165Dy, 176mLu, and 179Lu had higher Formula values than did 90Y for all tumor sizes studied, but only 149Pm can be produced nca and at high specific activities. The other electron-emitting radiolanthanides and the positron-emitting radiolanthanides showed low Formula values for all tumor sizes because of the high photon contribution. Conclusion: The low-energy electron emitters 161Tb, 177Lu, and 167Tm might be suitable for radionuclide therapy. The Auger-electron emitter 161Ho might not be suitable for systemic radionuclide therapy (intravenous injection) because of its short half-life but might be suitable for local therapy (e.g., in body cavities). If higher electron energy is needed, 149Pm or 166Ho might be suitable for radionuclide therapy.

Key Words: radiolanthanides • radionuclide therapy • dosimetry • production







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Copyright © 2006 by the Society of Nuclear Medicine.