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利用均匀扫描质子束测量质子治疗中心的中子剂量当量。

Measurements of neutron dose equivalent for a proton therapy center using uniform scanning proton beams.

机构信息

ProCure Proton Therapy Center, 5901 West Memorial Road, Oklahoma City, OK 73142, USA.

出版信息

Med Phys. 2012 Jun;39(6):3484-92. doi: 10.1118/1.4718685.

Abstract

PURPOSE

Neutron exposure is of concern in proton therapy, and varies with beam delivery technique, nozzle design, and treatment conditions. Uniform scanning is an emerging treatment technique in proton therapy, but neutron exposure for this technique has not been fully studied. The purpose of this study is to investigate the neutron dose equivalent per therapeutic dose, H/D, under various treatment conditions for uniform scanning beams employed at our proton therapy center.

METHODS

Using a wide energy neutron dose equivalent detector (SWENDI-II, ThermoScientific, MA), the authors measured H/D at 50 cm lateral to the isocenter as a function of proton range, modulation width, beam scanning area, collimated field size, and snout position. They also studied the influence of other factors on neutron dose equivalent, such as aperture material, the presence of a compensator, and measurement locations. They measured H/D for various treatment sites using patient-specific treatment parameters. Finally, they compared H/D values for various beam delivery techniques at various facilities under similar conditions.

RESULTS

H/D increased rapidly with proton range and modulation width, varying from about 0.2 mSv/Gy for a 5 cm range and 2 cm modulation width beam to 2.7 mSv/Gy for a 30 cm range and 30 cm modulation width beam when 18 × 18 cm(2) uniform scanning beams were used. H/D increased linearly with the beam scanning area, and decreased slowly with aperture size and snout retraction. The presence of a compensator reduced the H/D slightly compared with that without a compensator present. Aperture material and compensator material also have an influence on neutron dose equivalent, but the influence is relatively small. H/D varied from about 0.5 mSv/Gy for a brain tumor treatment to about 3.5 mSv/Gy for a pelvic case.

CONCLUSIONS

This study presents H/D as a function of various treatment parameters for uniform scanning proton beams. For similar treatment conditions, the H/D value per uncollimated beam size for uniform scanning beams was slightly lower than that from a passive scattering beam and higher than that from a pencil beam scanning beam, within a factor of 2. Minimizing beam scanning area could effectively reduce neutron dose equivalent for uniform scanning beams, down to the level close to pencil beam scanning.

摘要

目的

在质子治疗中,中子照射是一个关注点,其取决于束流输送技术、喷嘴设计和治疗条件。均匀扫描是质子治疗中的一种新兴治疗技术,但该技术的中子照射尚未得到充分研究。本研究的目的是在我们质子治疗中心使用的均匀扫描束的各种治疗条件下,研究每治疗剂量的中子剂量当量,H/D。

方法

使用宽能中子剂量当量探测器(SWENDI-II,ThermoScientific,MA),作者测量了离轴 50cm 处的 H/D 与质子射程、调制宽度、束扫描面积、准直野大小和探头位置的关系。他们还研究了其他因素对中子剂量当量的影响,如孔径材料、补偿器的存在以及测量位置。他们使用患者特定的治疗参数测量了不同治疗部位的 H/D。最后,他们比较了在相似条件下不同设施的各种束流输送技术的 H/D 值。

结果

H/D 随质子射程和调制宽度的增加而迅速增加,当使用 18×18cm²均匀扫描束时,从射程为 5cm、调制宽度为 2cm 的束的约 0.2mSv/Gy 变化到射程为 30cm、调制宽度为 30cm 的束的 2.7mSv/Gy。H/D 与束扫描面积呈线性关系,随孔径尺寸和探头缩回缓慢减小。与不使用补偿器相比,使用补偿器略微降低了 H/D。孔径材料和补偿器材料也对中子剂量当量有影响,但影响相对较小。H/D 从脑肿瘤治疗的约 0.5mSv/Gy 变化到骨盆病例的约 3.5mSv/Gy。

结论

本研究提出了均匀扫描质子束的各种治疗参数与 H/D 的关系。对于相似的治疗条件,均匀扫描束的未经准直的束尺寸每单位 H/D 值稍低于被动散射束,高于铅笔束扫描束,在 2 倍以内。最小化束扫描面积可以有效地降低均匀扫描束的中子剂量当量,使其降低到接近铅笔束扫描的水平。

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