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射波刀参考剂量测定法:对不断演变的关于校正因子和测量剂量的建议所产生影响的评估

CyberKnife reference dosimetry: An assessment of the impact of evolving recommendations on correction factors and measured dose.

作者信息

Buchegger Nicole, Grogan Garry, Hug Ben, Oliver Chris, Ebert Martin

机构信息

Department of Radiation Oncology, Sir Charles Gairdner Hospital, Nedlands, WA, 6009, Australia.

5D Clinics, Claremont, WA, 6010, Australia.

出版信息

Med Phys. 2020 Aug;47(8):3573-3585. doi: 10.1002/mp.14190. Epub 2020 May 25.

Abstract

PURPOSE

Specialized treatment machines such as the CyberKnife, TomoTherapy, or the GammaKnife, utilize flattening filter free (FFF) photon beams and may not be able to generate a 10 cm x 10 cm reference field. A new Code of Practice has recently been published (IAEA TRS483) to give recommendations for these machines. Additionally, some standard laboratories provide measured beam quality correction factors for the user's reference chamber, which can be used instead of the published tabulated beam quality correction factors. The purpose of this study was first to assess how different recommendations, as outlined below, affect the reference dosimetry at the CyberKnife, and second, to assess the impact of using measured rather than tabulated beam quality correction factors on measured dose.

METHODS

Following recommendations in TRS398, three field chambers (IBA CC04, Exradin A19, and Exradin A12S) were cross-calibrated with a user's reference chamber (IBA FC65-G), which was calibrated in a Cobalt-60 (Co-60) beam by a primary standards laboratory. The chamber response was corrected for influence quantities such as temperature, pressure, ion recombination, polarity, and beam quality. Additionally, correction factors for volume averaging and differences due the FFF beam spectrum were determined for the CyberKnife beam. Three different methods were utilized - TRS398; Intermediate (i.e. TRS398 with additional published recommendations); and TRS483. The measurements were undertaken in a 10 cm × 10 cm field defined by jaws for a uniform flattened (WFF) 6 MV photon beam of a Varian TrueBeam linear accelerator (linac) with a source to detector distance (SDD) of 100 cm, and in a 60 mm diameter circular field for a 6 MV flattening filter free (FFF) Accuray CyberKnife beam with SDD of 80 cm. All measurement was performed at 10 cm deep in a full scatter phantom as defined in TRS398.

RESULTS

Differences between the three methods in volume averaging correction factors ranged from 0.01% to 0.45% depending on the chamber assessed. As expected, an increased chamber length leads to a larger correction factor. The differences in beam spectrum correction factors range from 0.09% to 0.3%. Negligible differences in beam quality correction factors were observed; however, differences up to 1% were found between measured and tabulated values. Differences in cross-calibrated chamber calibration coefficients range from 0.05% to 0.51% depending on the chamber assessed. Differences in measured dose are up to 0.87% between Method TRS398 and Intermediate, again chamber dependent, and 0.28% between Method Intermediate and TRS483.

CONCLUSION

Using chambers cross-calibrated in the linac beam can lead to differences in measured dose per Monitor Unit (MU) in the CyberKnife beam of approximately 0.5% between chambers. Using Method Intermediate vs using recommendations given in TRS483 led to a difference of 0.28% in measured dose per MU, which is due to differences in volume averaging and beam spectrum correction factors. Using TRS483 is recommended as the cross-calibration is done in the CyberKnife beam and accounts for its specific reference conditions. It will also ensure consistency between different centers. The measured beam quality correction factors agree within the uncertainties with the tabulated values.

摘要

目的

射波刀、螺旋断层放疗或伽玛刀等专用治疗设备使用无均整器(FFF)光子束,可能无法产生10厘米×10厘米的参考射野。最近发布了一项新的操作规范(国际原子能机构TRS483),为这些设备提供建议。此外,一些标准实验室为用户的参考电离室提供测量得到的射束质量校正因子,可用于替代已公布的表格形式的射束质量校正因子。本研究的目的,一是评估如下所述的不同建议如何影响射波刀的参考剂量测定,二是评估使用测量得到的而非表格形式的射束质量校正因子对测量剂量的影响。

方法

按照TRS398中的建议,将三个射野电离室(IBA CC04、Exradin A19和Exradin A12S)与用户的参考电离室(IBA FC65-G)进行交叉校准,该参考电离室由一个基准标准实验室在钴-60(Co-60)射束中进行校准。对电离室响应进行了诸如温度、压力、离子复合、极性和射束质量等影响量的校正。此外,还确定了射波刀射束的体积平均校正因子以及因FFF射束光谱导致的差异的校正因子。采用了三种不同方法——TRS398;中间方法(即采用TRS398并结合其他已公布的建议);以及TRS483。测量在瓦里安TrueBeam直线加速器(直线加速器)的均匀均整(WFF)6兆伏光子束的10厘米×10厘米射野中进行,源到探测器距离(SDD)为100厘米,该射野由准直器界定,并且在射波刀Accuray 6兆伏无均整器(FFF)射束的60毫米直径圆形射野中进行,SDD为80厘米。所有测量均在TRS398中定义的全散射体模中10厘米深处进行。

结果

三种方法在体积平均校正因子方面的差异,根据所评估的电离室不同,在0.01%至0.45%之间。正如预期的那样,电离室长度增加会导致校正因子更大。射束光谱校正因子的差异在0.09%至0.3%之间。观察到射束质量校正因子的差异可忽略不计;然而,测量值与表格值之间发现了高达1%的差异。交叉校准的电离室校准系数的差异,根据所评估的电离室不同,在0.05%至0.51%之间。TRS398方法与中间方法之间测量剂量的差异高达0.87%,同样取决于电离室,中间方法与TRS483方法之间的差异为0.28%。

结论

使用在直线加速器射束中交叉校准的电离室,可能导致射波刀射束中每个监测单位(MU)的测量剂量在不同电离室之间相差约0.5%。采用中间方法与采用TRS483中给出的建议相比,每个MU的测量剂量相差0.28%,这是由于体积平均和射束光谱校正因子的差异所致。建议采用TRS483,因为交叉校准是在射波刀射束中进行的,并考虑了其特定的参考条件。这也将确保不同中心之间的一致性。测量得到的射束质量校正因子在不确定度范围内与表格值一致。

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