In-target production of [11C]CH4 from a nitrogen/hydrogen gas target as a function of beam current, irradiation time, and target temperature

IF 4.4 Q1 CHEMISTRY, INORGANIC & NUCLEAR EJNMMI Radiopharmacy and Chemistry Pub Date : 2024-03-25 DOI:10.1186/s41181-024-00255-1
Semi Helin, Johan Rajander, Jussi Aromaa, Eveliina Arponen, Jatta S. Helin, Olof Solin
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Abstract

Background

Production of [11C]CH4 from gas targets is notorious for weak performance with respect to yield, especially when using high beam currents. Post-target conversion of [11C]CO2 to [11C]CH4 is a widely used roundabout method in 11C-radiochemistry, but the added complexity increase the challenge to control carrier carbon. Thus in-target-produced [11C]CH4 is superior with respect to molar activity. We studied the in-target production of [11C]CO2 and [11C]CH4 from nitrogen gas targets as a function of beam current, irradiation time, and target temperature.

Results

[11C]CO2 production was practically unchanged across the range of varied parameters, but the [11C]CH4 yield, presented in terms of saturation yield YSAT(11CH4), had a negative correlation with beam current and a positive correlation with target chamber temperature. A formulated model equation indicates behavior where the [11C]CH4 formation follows a parabolic graph as a function of beam current. The negative square term, i.e., the yield loss, is postulated to arise from Haber–Bosch-like NH3 formation: N2 + 3H2 → 2NH3. The studied conditions suggest that the NH3 (liq.) would be condensed on the target chamber walls, thus depleting the hydrogen reserve needed for the conversion of nascent 11C to [11C]CH4.

Conclusions

[11C]CH4 production can be improved by increasing the target chamber temperature, which is presented in a mathematical formula. Our observations have implications for targetry design (geometry, gas volume and composition, pressure) and irradiation conditions, providing specific knowledge to enhance [11C]CH4 production at high beam currents. Increased [11C]CH4 radioactivity is an obvious benefit in radiosynthesis in terms of product yield and molar radioactivity.

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氮氢气靶靶内产生的[11C]CH4与束流、辐照时间和靶温的函数关系
背景从气体靶材中制备[11C]CH4因其产率低而臭名昭著,尤其是在使用高束流时。目标后将 [11C]CO2 转化为[11C]CH4 是 11C 放射化学中广泛使用的迂回方法,但增加的复杂性增加了控制载碳的挑战。因此,靶内产生的[11C]CH4 在摩尔活性方面更具优势。我们研究了氮气靶的靶内产[11C]CO2 和[11C]CH4 与束流、辐照时间和靶温度的函数关系。结果[11C]CO2 的产量在不同参数范围内几乎没有变化,但以饱和产量 YSAT(11CH4) 表示的[11C]CH4 产量与束流呈负相关,与靶室温度呈正相关。所建立的模型方程表明,[11C]CH4 的形成与束流的函数关系呈抛物线形。据推测,负平方项(即产量损失)是由类似哈伯-博什的 NH3 形成引起的:N2 + 3H2 → 2NH3。研究条件表明,NH3(液态)会凝结在靶室壁上,从而耗尽新生 11C 转化为[11C]CH4 所需的氢储备。我们的观察结果对靶室设计(几何形状、气体体积和成分、压力)和辐照条件都有影响,为在高束流条件下提高[11C]CH4产量提供了具体的知识。提高[11C]CH4的放射性在放射合成中对产品产量和摩尔放射性都有明显的好处。
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来源期刊
CiteScore
7.20
自引率
8.70%
发文量
30
审稿时长
5 weeks
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