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最大动能在质子立体定向放射外科中的考虑。

Maximum kinetic energy considerations in proton stereotactic radiosurgery.

机构信息

Department of Medical Physics, University of Wisconsin School of Medicine and Public Health, Madison, WI 53705, USA.

出版信息

J Appl Clin Med Phys. 2011 Apr 12;12(3):3533. doi: 10.1120/jacmp.v12i3.3533.

DOI:10.1120/jacmp.v12i3.3533
PMID:21844866
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC4878444/
Abstract

The purpose of this study was to determine the maximum proton kinetic energy required to treat a given percentage of patients eligible for stereotactic radiosurgery (SRS) with coplanar arc-based proton therapy, contingent upon the number and location of gantry angles used. Treatment plans from 100 consecutive patients treated with SRS at the University of Wisconsin Carbone Cancer Center between June of 2007 and March of 2010 were analyzed. For each target volume within each patient, in-house software was used to place proton pencil beam spots over the distal surface of the target volume from 51 equally-spaced gantry angles of up to 360°. For each beam spot, the radiological path length from the surface of the patient to the distal boundary of the target was then calculated along a ray from the gantry location to the location of the beam spot. This data was used to generate a maximum proton energy requirement for each patient as a function of the arc length that would be spanned by the gantry angles used in a given treatment. If only a single treatment angle is required, 100% of the patients included in the study could be treated by a proton beam with a maximum kinetic energy of 118 MeV. As the length of the treatment arc is increased to 90°, 180°, 270°, and 360°, the maximum energy requirement increases to 127, 145, 156, and 179 MeV, respectively. A very high percentage of SRS patients could be treated at relatively low proton energies if the gantry angles used in the treatment plan do not span a large treatment arc. Maximum proton kinetic energy requirements increase linearly with size of the treatment arc.

摘要

本研究的目的是确定在使用共面弧形质子治疗为符合立体定向放射外科 (SRS) 条件的患者进行治疗时,所需的最大质子动能,这取决于所使用的龙门架角度的数量和位置。分析了 2007 年 6 月至 2010 年 3 月期间在威斯康星大学 Carbone 癌症中心接受 SRS 治疗的 100 名连续患者的治疗计划。对于每位患者的每个靶区,使用内部软件在多达 360°的 51 个等距龙门架角度上在靶区的远端表面放置质子铅笔束点。对于每个射束点,从患者表面到靶区远端边界的放射学路径长度通过从龙门架位置到射束点位置的射线进行计算。然后,将该数据用于为每位患者生成最大质子能量需求,该需求作为在特定治疗中使用的龙门架角度所跨越的弧形长度的函数。如果仅需要单个治疗角度,则可以用最大动能为 118 MeV 的质子束治疗研究中包含的 100%的患者。随着治疗弧的长度增加到 90°、180°、270°和 360°,最大能量需求分别增加到 127、145、156 和 179 MeV。如果治疗计划中使用的龙门架角度不跨越大的治疗弧,则可以用相对较低的质子能量治疗 SRS 患者的很大一部分。最大质子动能需求随治疗弧的大小呈线性增加。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/51a980ad14e3/ACM2-12-122-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/a0993575cc05/ACM2-12-122-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/c1cfa057ed86/ACM2-12-122-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/1db71942245e/ACM2-12-122-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/e4f232e666db/ACM2-12-122-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/99a21cc9e308/ACM2-12-122-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/51a980ad14e3/ACM2-12-122-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/a0993575cc05/ACM2-12-122-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/c1cfa057ed86/ACM2-12-122-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/1db71942245e/ACM2-12-122-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/e4f232e666db/ACM2-12-122-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/99a21cc9e308/ACM2-12-122-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2b54/5718640/51a980ad14e3/ACM2-12-122-g006.jpg

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本文引用的文献

1
Maximum proton kinetic energy and patient-generated neutron fluence considerations in proton beam arc delivery radiation therapy.质子束弧形放射治疗中质子最大动能及患者产生的中子注量考量
Med Phys. 2009 Feb;36(2):364-72. doi: 10.1118/1.3049787.
2
Monte Carlo calculations and measurements of absorbed dose per monitor unit for the treatment of uveal melanoma with proton therapy.质子治疗葡萄膜黑色素瘤时每监测单位吸收剂量的蒙特卡罗计算与测量。
Phys Med Biol. 2008 Mar 21;53(6):1581-94. doi: 10.1088/0031-9155/53/6/005. Epub 2008 Feb 25.
3
Comparison of intensity modulated x-ray therapy and intensity modulated proton therapy for selective subvolume boosting: a phantom study.
用于选择性子体积增敏的调强X线治疗与调强质子治疗的比较:一项模体研究
Phys Med Biol. 2007 Oct 21;52(20):6073-91. doi: 10.1088/0031-9155/52/20/001. Epub 2007 Oct 1.
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Monte Carlo simulations for configuring and testing an analytical proton dose-calculation algorithm.用于配置和测试分析质子剂量计算算法的蒙特卡罗模拟。
Phys Med Biol. 2007 Aug 7;52(15):4569-84. doi: 10.1088/0031-9155/52/15/014. Epub 2007 Jul 10.
5
Point/counterpoint. Proton therapy is too expensive for the minimal potential improvements in outcome claimed.正方/反方观点。质子治疗对于所宣称的微小潜在疗效改善来说过于昂贵。
Med Phys. 2007 Apr;34(4):1135-8. doi: 10.1118/1.2717380.
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Proton therapy - a systematic review of clinical effectiveness.质子治疗——临床疗效的系统评价
Radiother Oncol. 2007 May;83(2):123-32. doi: 10.1016/j.radonc.2007.03.001. Epub 2007 May 11.
7
Within the next decade conventional cyclotrons for proton radiotherapy will become obsolete and replaced by far less expensive machines using compact laser systems for the acceleration of the protons.在未来十年内,用于质子放射治疗的传统回旋加速器将过时,并被使用紧凑型激光系统加速质子的成本低得多的机器所取代。
Med Phys. 2006 Mar;33(3):571-3. doi: 10.1118/1.2150220.
8
Proton therapy.质子治疗
Phys Med Biol. 2006 Jul 7;51(13):R491-504. doi: 10.1088/0031-9155/51/13/R26. Epub 2006 Jun 20.
9
Design tools for proton therapy nozzles based on the double-scattering foil technique.基于双散射箔技术的质子治疗喷嘴设计工具。
Radiat Prot Dosimetry. 2005;116(1-4 Pt 2):211-5. doi: 10.1093/rpd/nci229.
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Virtual commissioning of a treatment planning system for proton therapy of ocular cancers.眼部癌症质子治疗计划系统的虚拟调试
Radiat Prot Dosimetry. 2005;115(1-4):159-63. doi: 10.1093/rpd/nci224.