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在超高剂量脉冲条件下,通风电离室的电荷收集效率、潜在的复合机制以及电极距离的作用。

Charge collection efficiency, underlying recombination mechanisms, and the role of electrode distance of vented ionization chambers under ultra-high dose-per-pulse conditions.

机构信息

PTW-Freiburg (R&D), Freiburg 79115, Germany; University Clinic for Medical Radiation Physics, Medical Campus Pius Hospital, Carl von Ossietzky University Oldenburg, 26121, Germany.

Physikalisch-Technische Bundesanstalt, Braunschweig 38116, Germany.

出版信息

Phys Med. 2022 Dec;104:10-17. doi: 10.1016/j.ejmp.2022.10.021. Epub 2022 Nov 7.

DOI:10.1016/j.ejmp.2022.10.021
PMID:36356499
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9719440/
Abstract

PURPOSE

Investigating and understanding of the underlying mechanisms affecting the charge collection efficiency (CCE) of vented ionization chambers under ultra-high dose rate pulsed electron radiation. This is an important step towards real-time dosimetry with ionization chambers in FLASH radiotherapy.

METHODS

Parallel-plate ionization chambers (PPIC) with three different electrode distances were build and investigated with electron beams with ultra-high dose-per-pulse (DPP) up to 5.4 Gy. The measurements were compared with simulations. The experimental determination of the CCE was done by comparison against the reference dose based on alanine dosimetry. The numerical solution of a system of partial differential equations taking into account charge creations by the radiation, their transport and reaction in an applied electric field was used for the simulations of the CCE and the underlying effects.

RESULTS

A good agreement between the experimental results and the simulated CCE could be achieved. The recombination losses found under ultra-high DPP could be attributed to a temporal and spatial charge carrier imbalance and the associated electric field distortion. With ultra-thin electrode distances down to 0.25 mm and a suitable chamber voltage, a CCE greater than 99 % could be achieved under the ultra-high DPP conditions investigated.

CONCLUSIONS

Well-guarded ultra-thin PPIC are suited for real-time dosimetry under ultra-high DPP conditions. This allows dosimetry also for FLASH RT according to common codes of practice, traceable to primary standards. The numerical approach used allows the determination of appropriate correction factors beyond the DPP ranges where established theories are applicable to account for remaining recombination losses.

摘要

目的

研究和了解影响超高剂量率脉冲电子辐射下通风电离室电荷收集效率 (CCE) 的潜在机制。这是在 FLASH 放射治疗中使用电离室进行实时剂量测量的重要一步。

方法

使用具有三个不同电极距离的平行板电离室 (PPIC) 并通过超高剂量脉冲 (DPP) 高达 5.4 Gy 的电子束进行了研究。将测量结果与模拟结果进行了比较。通过与基于丙氨酸剂量测量的参考剂量进行比较来确定 CCE 的实验测定。考虑到辐射产生的电荷、它们在施加电场中的传输和反应的偏微分方程组的数值解用于模拟 CCE 和潜在效应。

结果

实验结果和模拟 CCE 之间可以很好地达成一致。在超高 DPP 下发现的复合损失可归因于电荷载流子的时间和空间不平衡以及相关的电场变形。通过使用非常薄的电极距离(低至 0.25 毫米)和适当的腔室电压,可以在研究的超高 DPP 条件下实现大于 99%的 CCE。

结论

精心保护的超薄 PPIC 适合在超高 DPP 条件下进行实时剂量测量。这允许根据常见的实践规范进行 FLASH RT 剂量测量,可追溯到主要标准。所使用的数值方法允许确定适当的校正因子,以弥补现有理论适用的 DPP 范围之外的剩余复合损失。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/d580801bad3c/gr12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/f15dcbc4d563/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/1143a66355fa/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/8baf2687a9b4/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/c194091195fa/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/fa55e8506fb8/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/b5a7a465f2eb/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/dbc5783a810a/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/3d016785b21b/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/5c279e096e43/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/98ff0a41cea7/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/dcaa957a5e77/gr11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/d580801bad3c/gr12.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/f15dcbc4d563/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/1143a66355fa/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/8baf2687a9b4/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/c194091195fa/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/fa55e8506fb8/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/b5a7a465f2eb/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/dbc5783a810a/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/3d016785b21b/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/5c279e096e43/gr9.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/98ff0a41cea7/gr10.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/dcaa957a5e77/gr11.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/69ae/9719440/d580801bad3c/gr12.jpg

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