2019
DOI: 10.1002/mp.13563
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Efficient 169Yb high‐dose‐rate brachytherapy source production using reactivation

Abstract: Purpose: To present and quantify the effectiveness of a method for the efficient production of 169 Yb high-dose-rate brachytherapy sources with 27 Ci activity upon clinical delivery, which have about the same dose rate in water at 1 cm from the source center as 10 Ci 192 Ir sources. Materials: A theoretical framework for 169 Yb source activation and reactivation using thermal neutrons in a research reactor and 168 Yb-Yb 2 O 3 precursor is derived and benchmarked against published data. The model is dependent p… Show more

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Cited by 17 publications
(21 citation statements)
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“…The source can be adapted to handle more activity to lower treatment times, if needed, by increasing the length of the active core. For a highly enriched precursor, the 175 Yb impurities levels are sufficiently low after activation and additional cooling is not required . To modulate the intensity profile of the source, thin platinum shields are inserted within the catheters, using a similar approach as Adams et al Platinum was selected due to its high density (21.45 g cm −3 ), high atomic number (Z = 78), and ferromagnetic properties.…”
Section: Methodsmentioning
confidence: 99%
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“…The source can be adapted to handle more activity to lower treatment times, if needed, by increasing the length of the active core. For a highly enriched precursor, the 175 Yb impurities levels are sufficiently low after activation and additional cooling is not required . To modulate the intensity profile of the source, thin platinum shields are inserted within the catheters, using a similar approach as Adams et al Platinum was selected due to its high density (21.45 g cm −3 ), high atomic number (Z = 78), and ferromagnetic properties.…”
Section: Methodsmentioning
confidence: 99%
“…For a highly enriched precursor, the 175 Yb impurities levels are sufficiently low after activation and additional cooling is not required. 35,37 To modulate the intensity profile of the source, thin platinum shields are inserted within the catheters, using a similar approach as Adams et al 18 Platinum was selected due to its high density (21.45 g cm À3 ), high atomic number (Z = 78), and ferromagnetic properties. The shield partially fills the hollow portion of a six French (2 mm) plastic catheter with a wall thickness of 0.25 mm [Figs.…”
Section: A Source and Shield Designmentioning
confidence: 99%
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