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技术说明:用于放射治疗应用的 Al O :C 光激励发光剂量计纳米点和 LiF:Mg,Ti 热释光剂量计的高剂量和超高剂量率(UHDR)评估。

Technical note: High-dose and ultra-high dose rate (UHDR) evaluation of Al O :C optically stimulated luminescent dosimeter nanoDots and powdered LiF:Mg,Ti thermoluminescent dosimeters for radiation therapy applications.

机构信息

Division of Radiation Oncology, Department of Radiation Physics, The University of Texas MD Anderson Cancer Center, Houston, Texas, USA.

The University of Texas MD Anderson Cancer Center UTHealth Houston Graduate School of Biomedical Sciences, Houston, Texas, USA.

出版信息

Med Phys. 2024 Mar;51(3):2311-2319. doi: 10.1002/mp.16832. Epub 2023 Nov 22.

Abstract

BACKGROUND

Dosimetry in ultra-high dose rate (UHDR) electron beamlines poses a significant challenge owing to the limited usability of standard dosimeters in high dose and high dose-per-pulse (DPP) applications.

PURPOSE

In this study, Al O :C nanoDot optically stimulated luminescent dosimeters (OSLDs), single-use powder-based LiF:Mg,Ti thermoluminescent dosimeters (TLDs), and Gafchromic EBT3 film were evaluated at extended dose ranges (up to 40 Gy) in conventional dose rate (CONV) and UHDR beamlines to determine their usability for calibration and dose verification in the setting of FLASH radiation therapy.

METHODS

OSLDs and TLDs were evaluated against established dose-rate-independent Gafchromic EBT3 film with regard to the potential influence of mean dose rate, instantaneous dose rate, and DPP on signal response. The dosimeters were irradiated at CONV or UHDR conditions on a 9-MeV electron beam. Under UHDR conditions, different settings of pulse repetition frequency (PRF), pulse width (PW), and pulse amplitude were used to characterize the individual dosimeters' response in order to isolate their potential dependencies on dose, dose rate, and DPP.

RESULTS

The OSLDs, TLDs, and Gafchromic EBT3 film were found to be suitable at a dose range of up to 40 Gy without any indication of saturation in signal. The response of OSLDs and TLDs in UHDR conditions were found to be independent of mean dose rate (up to 1440 Gy/s), instantaneous dose rate (up to 2 MGy/s), and DPP (up to 7 Gy), with uncertainties on par with nominal values established in CONV beamlines (± 4%). In cross-comparing the response of OSLDs, TLDs and Gafchromic film at dose rates of 0.18-245 Gy/s, the coefficient of variation or relative standard deviation in the measured dose between the three dosimeters (inter-dosimeter comparison) was found to be within 2%.

CONCLUSIONS

We demonstrated the dynamic range of OSLDs, TLDs, and Gafchromic film to be suitable up to 40 Gy, and we developed a protocol that can be used to accurately translate the measured signal in each respective dosimeter to dose. OSLDs and powdered TLDs were shown to be viable for dosimetric measurement in UHDR beamlines, providing dose measurements with accuracies on par with Gafchromic EBT3 film and their concurrent use demonstrating a means for redundant dosimetry in UHDR conditions.

摘要

背景

超高剂量率(UHDR)电子束线中的剂量学具有挑战性,这是因为在高剂量和高剂量脉冲(DPP)应用中,标准剂量计的可用性有限。

目的

在这项研究中,我们评估了 Al O :C 纳米点光激励发光剂量计(OSLD)、一次性粉末状 LiF:Mg,Ti 热释光剂量计(TLD)和 Gafchromic EBT3 薄膜在常规剂量率(CONV)和 UHDR 束线中的扩展剂量范围内(高达 40Gy)的适用性,以确定它们在 FLASH 放射治疗中的校准和剂量验证中的可用性。

方法

针对既定的剂量率独立的 Gafchromic EBT3 薄膜,我们评估了 OSLD 和 TLD 对平均剂量率、瞬时剂量率和 DPP 对信号响应的潜在影响。在 9 MeV 电子束下,在 CONV 或 UHDR 条件下辐照剂量计。在 UHDR 条件下,使用不同的脉冲重复频率(PRF)、脉冲宽度(PW)和脉冲幅度设置来表征各个剂量计的响应,以分离它们对剂量、剂量率和 DPP 的潜在依赖性。

结果

发现 OSLD、TLD 和 Gafchromic EBT3 薄膜在高达 40Gy 的剂量范围内没有信号饱和的迹象,因此是合适的。在 UHDR 条件下,OSLD 和 TLD 的响应被发现与平均剂量率(高达 1440Gy/s)、瞬时剂量率(高达 2MGy/s)和 DPP(高达 7Gy)无关,其不确定度与 CONV 束线中建立的标称值相当(±4%)。在比较 OSLD、TLD 和 Gafchromic 薄膜在 0.18-245Gy/s 的剂量率下的响应时,发现三个剂量计之间(剂量计之间的比较)测量剂量的变异系数或相对标准偏差在 2%以内。

结论

我们证明了 OSLD、TLD 和 Gafchromic 薄膜的动态范围在高达 40Gy 的范围内是合适的,并且我们开发了一种可以用来准确地将每个相应剂量计的测量信号转换为剂量的协议。OSLD 和粉末状 TLD 被证明可用于 UHDR 束线中的剂量测量,其剂量测量精度与 Gafchromic EBT3 薄膜相当,并且它们的同时使用提供了在 UHDR 条件下冗余剂量测量的手段。

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