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PGAI瞬发伽玛射线活化成像技术理想化模型的模拟

耿书群 贾文宝 黑大千 程璨

耿书群, 贾文宝, 黑大千, 等. PGAI瞬发伽玛射线活化成像技术理想化模型的模拟[J]. 强激光与粒子束, 2018, 30: 016005. doi: 10.11884/HPLPB201830.170246
引用本文: 耿书群, 贾文宝, 黑大千, 等. PGAI瞬发伽玛射线活化成像技术理想化模型的模拟[J]. 强激光与粒子束, 2018, 30: 016005. doi: 10.11884/HPLPB201830.170246
Geng Shuqun, Jia Wenbao, Hei Daqian, et al. Prompt gamma activation imaging technology under idealized model[J]. High Power Laser and Particle Beams, 2018, 30: 016005. doi: 10.11884/HPLPB201830.170246
Citation: Geng Shuqun, Jia Wenbao, Hei Daqian, et al. Prompt gamma activation imaging technology under idealized model[J]. High Power Laser and Particle Beams, 2018, 30: 016005. doi: 10.11884/HPLPB201830.170246

PGAI瞬发伽玛射线活化成像技术理想化模型的模拟

doi: 10.11884/HPLPB201830.170246
基金项目: 

国家自然科学基金项目 GBA1501401

详细信息
    作者简介:

    耿书群(1992-), 男,硕士,主要从事核技术及应用;54745591@qq.com

    通讯作者:

    贾文宝(1968-), 男,教授,主要从事核技术及应用;jiawenbao@163.com

  • 中图分类号: TL99

Prompt gamma activation imaging technology under idealized model

  • 摘要: 为了讨论PGAI技术分析的准确性,并验证冷中子和热中子应用于PGAI技术的可行性,通过蒙特卡罗模拟计算软件对PGAI技术理想化模型进行了研究,采用高准直的冷中子及热中子束和高纯锗探测器,对一块5 cm× 5 cm×1 cm均匀铁单质样品进行了模拟计算及图像重建,选取的等效体积大小为1 cm×1 cm×1 cm。结果显示:两种能量中子可以用于PGAI技术实现元素分布测量,但无论使用何种能量中子,由于物料体效应带来的中子自屏效应、中子散射效应以及伽马射线自吸收作用,即便在对均匀单质样品进行测量时,图像重建结果也无法保证各位置元素响应的一致性。因此,在后续工作中,需理清PGAI物理机制,建立相应的修正模型。
  • 图  1  PGAI理想化模型示意图

    Figure  1.  Sketch of PGAI under idealized model

    图  2  伽马射线强度随铅块的厚度变化

    Figure  2.  Relationship between intensity of gamma ray and thickness of lead

    图  3  样品及PGAI测量平台结构示意图

    Figure  3.  Diagrammatic sketch of sample and PGAI setup

    图  4  每列的特征伽马射线计数随中子穿透距离的变化

    Figure  4.  Relationship between characteristic counts of gamma ray and penetration of neutron in each column

    图  5  模拟得到的样品内部目标元素的归一化计数的图像

    Figure  5.  Monte Carlo simulated target-element-normalized counts maps of sample

    图  6  样品内部目标元素修正后的归一化计数的图像

    Figure  6.  Target-element-corrected normalized counts maps of sample

    表  1  高纯锗探测器结构尺寸和材料

    Table  1.   Structure size and material of the high-purity Ge detector

    structure of the detector parameter dimension/mm material
    crystal diameter 54 Ge
    crystal length 72.6 Ge
    Mount Cup base thickness 3 Al
    Mount Cup wall thickness 0.8 Al
    End Up incident window 0.5 Be
    dead layer outside thickness 1 Ge/B
    dead layer inside thickness 0.007 Ge/Li
    下载: 导出CSV
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出版历程
  • 收稿日期:  2017-06-21
  • 修回日期:  2017-08-27
  • 刊出日期:  2018-01-15

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