• Acta Physica Sinica
  • Vol. 68, Issue 23, 238502-1 (2019)
Zhi-Liang Hu1、2、3, Wei-Tao Yang1, Yong-Hong Li1、*, Yang Li1, Chao-Hui He1, Song-Lin Wang2、3, Bin Zhou2、3, Quan-Zhi Yu2、4, Huan He1, Fei Xie1, Yu-Rong Bai1, and Tian-Jiao Liang2、3、*
Author Affiliations
  • 1School of Nuclear Science and Technology, Xi’an Jiaotong University, Xi’an 710049, China
  • 2Spallation Neutron Source Science Center, Dongguan 523803, China
  • 3Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
  • 4Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
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    DOI: 10.7498/aps.68.20191196 Cite this Article
    Zhi-Liang Hu, Wei-Tao Yang, Yong-Hong Li, Yang Li, Chao-Hui He, Song-Lin Wang, Bin Zhou, Quan-Zhi Yu, Huan He, Fei Xie, Yu-Rong Bai, Tian-Jiao Liang. Atmospheric neutron single event effect in 65 nm microcontroller units by using CSNS-BL09[J]. Acta Physica Sinica, 2019, 68(23): 238502-1 Copy Citation Text show less
    Cross sections of different energy neutrons interacting with various nuclear atoms in semiconductor: (a) Cross sections of B and Si isotopes, the neutron energy interval is 10–11−1 MeV; (b) cross sections of14N, 16O, 27Al, 28Si and 184W, the neutron energy interval is 1−150 MeV.半导体中各核素的中子反应截面 (a)与B, Si的同位素的反应截面, 对应中子能量范围10–11−1 MeV; (b)与14N, 16O, 27Al, 28Si, 184W的反应截面, 对应中子能量范围1−150 MeV
    Fig. 1. Cross sections of different energy neutrons interacting with various nuclear atoms in semiconductor: (a) Cross sections of B and Si isotopes, the neutron energy interval is 10–11−1 MeV; (b) cross sections of14N, 16O, 27Al, 28Si and 184W, the neutron energy interval is 1−150 MeV. 半导体中各核素的中子反应截面 (a)与B, Si的同位素的反应截面, 对应中子能量范围10–11−1 MeV; (b)与14N, 16O, 27Al, 28Si, 184W的反应截面, 对应中子能量范围1−150 MeV
    Neutron spectrum of the experiments.实验束线中子能谱
    Fig. 2. Neutron spectrum of the experiments.实验束线中子能谱
    65 nm MCU neutron test site: (a) The device under test and the 2 cm ejection hole; (b) with 2 mm cadmium shielding; (c) without cadmium shielding.65 nm MCU散裂中子辐照测试现场图 (a) DUT与出射孔相对位置图; (b)含2 mm厚镉屏蔽体测试现场图; (c)无镉屏蔽测试现场图
    Fig. 3. 65 nm MCU neutron test site: (a) The device under test and the 2 cm ejection hole; (b) with 2 mm cadmium shielding; (c) without cadmium shielding.65 nm MCU散裂中子辐照测试现场图 (a) DUT与出射孔相对位置图; (b)含2 mm厚镉屏蔽体测试现场图; (c)无镉屏蔽测试现场图
    The LET values and ranges of secondary particles from thermal neutrons interacting with 10B.热中子与10B反应产生次级粒子在不同能量下的LET与硅中射程
    Fig. 4. The LET values and ranges of secondary particles from thermal neutrons interacting with 10B. 热中子与10B反应产生次级粒子在不同能量下的LET与硅中射程
    The sketch of thermal neutron interacting with 10B in 65 nm MCU.65 nm MCU内部热中子与10B反应次级粒子沉积能量示意图
    Fig. 5. The sketch of thermal neutron interacting with 10B in 65 nm MCU. 65 nm MCU内部热中子与10B反应次级粒子沉积能量示意图
    物理量测试组对照组
    实验值实验值推导值
    SBU次数166346
    总质子数/p5.3363 × 10177.2131 × 10175.3363 × 1017
    中子注量/n·cm–2镉上中子7.6997 × 10101.0703 × 10117.9182 × 1010
    热中子1.2585 × 1081.0062 × 10107.4440 × 109
    Table 1.

    The experiment data in two irradiations.

    两组辐照下的实验数据

    Zhi-Liang Hu, Wei-Tao Yang, Yong-Hong Li, Yang Li, Chao-Hui He, Song-Lin Wang, Bin Zhou, Quan-Zhi Yu, Huan He, Fei Xie, Yu-Rong Bai, Tian-Jiao Liang. Atmospheric neutron single event effect in 65 nm microcontroller units by using CSNS-BL09[J]. Acta Physica Sinica, 2019, 68(23): 238502-1
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