Tanguay J, Hou X, Buckley K, Schaffer P, Bénard F, Ruth T J, Celler A
Department of Radiology, University of British Columbia, 2329 West Mall, Vancouver, BC V6T 1Z4, Canada.
Phys Med Biol. 2015 May 21;60(10):3883-903. doi: 10.1088/0031-9155/60/10/3883. Epub 2015 Apr 24.
Cyclotron production of (99m)Tc through the (100)Mo(p,2n) (99m)Tc reaction channel is actively being investigated as an alternative to reactor-based (99)Mo generation by nuclear fission of (235)U. An exciting aspect of this approach is that it can be implemented using currently-existing cyclotron infrastructure to supplement, or potentially replace, conventional (99m)Tc production methods that are based on aging and increasingly unreliable nuclear reactors. Successful implementation will require consistent production of large quantities of high-radionuclidic-purity (99m)Tc. However, variations in proton beam currents and the thickness and isotopic composition of enriched (100)Mo targets, in addition to other irradiation parameters, may degrade reproducibility of both radionuclidic purity and absolute (99m)Tc yields. The purpose of this article is to present a method for quantifying relationships between random variations in production parameters, including (100)Mo target thicknesses and proton beam currents, and reproducibility of absolute (99m)Tc yields (defined as the end of bombardment (EOB) (99m)Tc activity). Using the concepts of linear error propagation and the theory of stochastic point processes, we derive a mathematical expression that quantifies the influence of variations in various irradiation parameters on yield reproducibility, quantified in terms of the coefficient of variation of the EOB (99m)Tc activity. The utility of the developed formalism is demonstrated with an example. We show that achieving less than 20% variability in (99m)Tc yields will require highly-reproducible target thicknesses and proton currents. These results are related to the service rate which is defined as the percentage of (99m)Tc production runs that meet the minimum daily requirement of one (or many) nuclear medicine departments. For example, we show that achieving service rates of 84.0%, 97.5% and 99.9% with 20% variations in target thicknesses requires producing on average 1.2, 1.5 and 1.9 times the minimum daily activity requirement. The irradiation parameters that would be required to achieve these service rates are described. We believe the developed formalism will aid in the development of quality-control criteria required to ensure consistent supply of large quantities of high-radionuclidic-purity cyclotron-produced (99m)Tc.
通过(100)Mo(p,2n)(99m)Tc反应通道利用回旋加速器生产(99m)Tc,作为通过(235)U核裂变基于反应堆生产(99)Mo的替代方法正在积极研究中。这种方法令人兴奋的一个方面是,它可以利用现有的回旋加速器基础设施来补充或潜在替代基于老化且越来越不可靠的核反应堆的传统(99m)Tc生产方法。成功实施将需要持续生产大量高放射性核素纯度的(99m)Tc。然而,除其他辐照参数外,质子束流以及富集(100)Mo靶的厚度和同位素组成的变化,可能会降低放射性核素纯度和绝对(99m)Tc产率的可重复性。本文的目的是提出一种方法,用于量化生产参数的随机变化之间的关系,包括(100)Mo靶厚度和质子束流,以及绝对(99m)Tc产率的可重复性(定义为轰击结束(EOB)时的(99m)Tc活度)。利用线性误差传播的概念和随机点过程理论,我们推导了一个数学表达式,该表达式量化了各种辐照参数变化对产率可重复性的影响,产率可重复性以EOB(99m)Tc活度的变异系数来量化。通过一个例子展示了所开发形式主义的实用性。我们表明,要使(99m)Tc产率的变异性小于20%,将需要高度可重复的靶厚度和质子电流。这些结果与服务率相关,服务率定义为满足一个(或多个)核医学科室每日最低需求的(99m)Tc生产运行的百分比。例如,我们表明,在靶厚度有20%变化的情况下,要达到84.0%、97.5%和99.9%的服务率,平均需要生产每日最低活度需求的1.2倍、1.5倍和1.9倍。描述了实现这些服务率所需的辐照参数。我们相信所开发的形式主义将有助于制定确保持续供应大量高放射性核素纯度的回旋加速器生产的(99m)Tc所需的质量控制标准。