• 文献检索
  • 文档翻译
  • 深度研究
  • 学术资讯
  • Suppr Zotero 插件Zotero 插件
  • 邀请有礼
  • 套餐&价格
  • 历史记录
应用&插件
Suppr Zotero 插件Zotero 插件浏览器插件Mac 客户端Windows 客户端微信小程序
定价
高级版会员购买积分包购买API积分包
服务
文献检索文档翻译深度研究API 文档MCP 服务
关于我们
关于 Suppr公司介绍联系我们用户协议隐私条款
关注我们

Suppr 超能文献

核心技术专利:CN118964589B侵权必究
粤ICP备2023148730 号-1Suppr @ 2026

文献检索

告别复杂PubMed语法,用中文像聊天一样搜索,搜遍4000万医学文献。AI智能推荐,让科研检索更轻松。

立即免费搜索

文件翻译

保留排版,准确专业,支持PDF/Word/PPT等文件格式,支持 12+语言互译。

免费翻译文档

深度研究

AI帮你快速写综述,25分钟生成高质量综述,智能提取关键信息,辅助科研写作。

立即免费体验

激光驱动离子源LION处次级辐射场的Geant4蒙特卡罗模拟研究

Geant4 Monte Carlo simulation study of the secondary radiation fields at the laser-driven ion source LION.

作者信息

Tisi M, Mares V, Schreiber J, Englbrecht F S, Rühm W

机构信息

Institute of Radiation Medicine, Helmholtz Zentrum München, Neuherberg, Germany.

Department of Medical Physics, Faculty of Physics, Ludwig-Maximilians-Universität, Garching bei München, Germany.

出版信息

Sci Rep. 2021 Dec 24;11(1):24418. doi: 10.1038/s41598-021-03897-2.

DOI:10.1038/s41598-021-03897-2
PMID:34952912
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8709851/
Abstract

At the Center for Advanced Laser Applications (CALA), Garching, Germany, the LION (Laser-driven ION Acceleration) experiment is being commissioned, aiming at the production of laser-driven bunches of protons and light ions with multi-MeV energies and repetition frequency up to 1 Hz. A Geant4 Monte Carlo-based study of the secondary neutron and photon fields expected during LION's different commissioning phases is presented. Goal of this study is the characterization of the secondary radiation environment present inside and outside the LION cave. Three different primary proton spectra, taken from experimental results reported in the literature and representative of three different future stages of the LION's commissioning path are used. Together with protons, also electrons are emitted through laser-target interaction and are also responsible for the production of secondary radiation. For the electron component of the three source terms, a simplified exponential model is used. Moreover, in order to reduce the simulation complexity, a two-components simplified geometrical model of proton and electron sources is proposed. It has been found that the radiation environment inside the experimental cave is either dominated by photons or neutrons depending on the position in the room and the source term used. The higher the intensity of the source, the higher the neutron contribution to the total dose for all scored positions. Maximum neutron and photon ambient dose equivalent values normalized to 10 simulated incident primaries were calculated at the exit of the vacuum chamber, where values of about 85 nSv (10 primaries) and 1.0 μSv (10 primaries) were found.

摘要

在德国加兴的先进激光应用中心(CALA),正在对LION(激光驱动离子加速)实验进行调试,目标是产生能量高达数兆电子伏特且重复频率高达1赫兹的激光驱动质子束和轻离子束。本文介绍了一项基于Geant4蒙特卡罗方法的研究,该研究针对LION不同调试阶段预期产生的次级中子和光子场。这项研究的目的是对LION实验洞穴内外的次级辐射环境进行表征。使用了三种不同的初级质子能谱,这些能谱取自文献报道的实验结果,代表了LION调试路径的三个不同未来阶段。除了质子,电子也通过激光与靶的相互作用发射出来,并且也会产生次级辐射。对于三个源项中的电子部分,使用了一个简化的指数模型。此外,为了降低模拟复杂度,提出了一个质子和电子源的双组分简化几何模型。研究发现,实验洞穴内的辐射环境由光子或中子主导,这取决于房间内的位置和所使用的源项。源的强度越高,对于所有计分位置,中子对总剂量的贡献就越高。在真空腔出口处计算了归一化为10个模拟入射初级粒子的最大中子和光子环境剂量当量值,发现约为85纳希沃特(10个初级粒子)和1.0微希沃特(10个初级粒子)。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/5df061c4297b/41598_2021_3897_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/ec2c062ae47d/41598_2021_3897_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/a82f09cd7ad1/41598_2021_3897_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/77ad093ce0a8/41598_2021_3897_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/7d7de05dd11c/41598_2021_3897_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/a51c1e5948bf/41598_2021_3897_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/b3ec6fc6a55e/41598_2021_3897_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/395c29000d77/41598_2021_3897_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/34b4c61e970b/41598_2021_3897_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/6dc7d1245bbe/41598_2021_3897_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/ac1d43ffa660/41598_2021_3897_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/92773680d3bb/41598_2021_3897_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/5df061c4297b/41598_2021_3897_Fig12_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/ec2c062ae47d/41598_2021_3897_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/a82f09cd7ad1/41598_2021_3897_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/77ad093ce0a8/41598_2021_3897_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/7d7de05dd11c/41598_2021_3897_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/a51c1e5948bf/41598_2021_3897_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/b3ec6fc6a55e/41598_2021_3897_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/395c29000d77/41598_2021_3897_Fig7_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/34b4c61e970b/41598_2021_3897_Fig8_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/6dc7d1245bbe/41598_2021_3897_Fig9_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/ac1d43ffa660/41598_2021_3897_Fig10_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/92773680d3bb/41598_2021_3897_Fig11_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b490/8709851/5df061c4297b/41598_2021_3897_Fig12_HTML.jpg

相似文献

1
Geant4 Monte Carlo simulation study of the secondary radiation fields at the laser-driven ion source LION.激光驱动离子源LION处次级辐射场的Geant4蒙特卡罗模拟研究
Sci Rep. 2021 Dec 24;11(1):24418. doi: 10.1038/s41598-021-03897-2.
2
Radiation protection modelling for 2.5 Petawatt-laser production of ultrashort x-ray, proton and ion bunches: Monte Carlo model of the Munich CALA facility.2.5 拍瓦激光产生超短 X 射线、质子和离子束的辐射防护建模:慕尼黑 CALA 设施的蒙特卡罗模型。
J Radiol Prot. 2020 Sep 18;40(4). doi: 10.1088/1361-6498/aba8e4.
3
A comprehensive Monte Carlo study of out-of-field secondary neutron spectra in a scanned-beam proton therapy gantry room.扫描束质子治疗机架室中外照射野次级中子能谱的综合蒙特卡罗研究。
Z Med Phys. 2021 May;31(2):215-228. doi: 10.1016/j.zemedi.2021.01.001. Epub 2021 Feb 20.
4
Shielding implications for secondary neutrons and photons produced within the patient during IMPT.在 IMPT 中,患者体内产生的次级中子和光子的屏蔽影响。
Med Phys. 2013 Jul;40(7):071701. doi: 10.1118/1.4807089.
5
Neutron and Photon Dose Rates in a D-T Neutron Generator Facility: MCNP Simulations and Experiments.D-T 中子发生器设施中的中子和光子剂量率:MCNP 模拟与实验。
Health Phys. 2020 Jun;118(6):600-608. doi: 10.1097/HP.0000000000001175.
6
Systematic out-of-field secondary neutron spectrometry and dosimetry in pencil beam scanning proton therapy.笔形束扫描质子治疗中的系统外野次级中子谱测量与剂量学研究。
Med Phys. 2017 May;44(5):1912-1920. doi: 10.1002/mp.12206. Epub 2017 Apr 20.
7
Validation of a Monte Carlo Framework for Out-of-Field Dose Calculations in Proton Therapy.用于质子治疗中射野外剂量计算的蒙特卡罗框架的验证
Front Oncol. 2022 Jun 8;12:882489. doi: 10.3389/fonc.2022.882489. eCollection 2022.
8
A Monte Carlo study on the secondary neutron generation by oxygen ion beams for radiotherapy and its comparison to lighter ions.蒙特卡罗研究氧离子束在放射治疗中的次级中子产生及其与轻离子的比较。
Phys Med Biol. 2024 Jan 2;69(1). doi: 10.1088/1361-6560/ad0f45.
9
Photonuclear dose calculations for high-energy photon beams from Siemens and Varian linacs.西门子和瓦里安直线加速器高能光子束的光核剂量计算。
Med Phys. 2003 Aug;30(8):1990-2000. doi: 10.1118/1.1590436.
10
Measurement of stray radiation within a scanning proton therapy facility: EURADOS WG9 intercomparison exercise of active dosimetry systems.扫描质子治疗设施内杂散辐射的测量:EURADOS WG9有源剂量测定系统的比对试验
Med Phys. 2015 May;42(5):2572-84. doi: 10.1118/1.4916667.

引用本文的文献

1
Secondary neutron dose measurements at the DRACO laser-driven ion source.在DRACO激光驱动离子源处进行的次级中子剂量测量。
Sci Rep. 2025 Jun 20;15(1):20161. doi: 10.1038/s41598-025-05442-x.

本文引用的文献

1
Radiation protection modelling for 2.5 Petawatt-laser production of ultrashort x-ray, proton and ion bunches: Monte Carlo model of the Munich CALA facility.2.5 拍瓦激光产生超短 X 射线、质子和离子束的辐射防护建模:慕尼黑 CALA 设施的蒙特卡罗模型。
J Radiol Prot. 2020 Sep 18;40(4). doi: 10.1088/1361-6498/aba8e4.
2
Spectral and spatial shaping of laser-driven proton beams using a pulsed high-field magnet beamline.利用脉冲强磁场束线对激光驱动质子束进行能谱和空间整形。
Sci Rep. 2020 Jun 4;10(1):9118. doi: 10.1038/s41598-020-65775-7.
3
Laser Acceleration of Highly Energetic Carbon Ions Using a Double-Layer Target Composed of Slightly Underdense Plasma and Ultrathin Foil.
利用由略欠稠密等离子体和超薄箔组成的双层靶对高能碳离子进行激光加速。
Phys Rev Lett. 2019 Jan 11;122(1):014803. doi: 10.1103/PhysRevLett.122.014803.
4
A novel approach to electron data background treatment in an online wide-angle spectrometer for laser-accelerated ion and electron bunches.一种用于激光加速离子束和电子束的在线广角光谱仪中电子数据背景处理的新方法。
Rev Sci Instrum. 2018 Jan;89(1):013301. doi: 10.1063/1.5001990.
5
Systematic out-of-field secondary neutron spectrometry and dosimetry in pencil beam scanning proton therapy.笔形束扫描质子治疗中的系统外野次级中子谱测量与剂量学研究。
Med Phys. 2017 May;44(5):1912-1920. doi: 10.1002/mp.12206. Epub 2017 Apr 20.
6
International Commission on Radiation Units and Measurements.国际辐射单位与测量委员会
J ICRU. 2014 Apr;14(1):NP. doi: 10.1093/jicru/ndw040.
7
RADIOLOGICAL SAFETY ASSESSMENT FOR THE EXPERIMENTAL AREA OF A HYPER-INTENSE LASER WITH PEAK-POWER OF 1PW-CETAL.
Radiat Prot Dosimetry. 2017 Jun 1;175(1):104-109. doi: 10.1093/rpd/ncw274.
8
Ionisation Chamber for Measurement of Pulsed Photon Radiation Fields.用于测量脉冲光子辐射场的电离室。
Radiat Prot Dosimetry. 2017 Apr 28;174(3):297-301. doi: 10.1093/rpd/ncw145.
9
Maximum Proton Energy above 85 MeV from the Relativistic Interaction of Laser Pulses with Micrometer Thick CH_{2} Targets.激光脉冲与微米厚CH₂靶相对论相互作用产生的85 MeV以上的最大质子能量
Phys Rev Lett. 2016 May 20;116(20):205002. doi: 10.1103/PhysRevLett.116.205002. Epub 2016 May 19.
10
Secondary neutron spectrum from 250-MeV passively scattered proton therapy: measurement with an extended-range Bonner sphere system.250兆电子伏特被动散射质子治疗产生的次级中子能谱:使用扩展量程邦纳球系统进行测量
Med Phys. 2014 Sep;41(9):092104. doi: 10.1118/1.4892929.