• Laser & Optoelectronics Progress
  • Vol. 58, Issue 17, 1732001 (2021)
Haolin Liu1、*, Qing Liu1, Xiaohui Zhang1, Jing Sun2, Song Gu2, and Zhengyu Zhong3
Author Affiliations
  • 1School of Automation and Information Engineering, Xi'an University of Technology, Xi'an , Shaanxi 710048, China
  • 2China Academy of Space Technology (Xi'an), Xi'an , Shaanxi 710100, China
  • 3Beijing San-talking Testing Engineering Academy, Beijing100089, China
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    DOI: 10.3788/LOP202158.1732001 Cite this Article Set citation alerts
    Haolin Liu, Qing Liu, Xiaohui Zhang, Jing Sun, Song Gu, Zhengyu Zhong. Heavy Ion Single Event Effect Test Calibration System[J]. Laser & Optoelectronics Progress, 2021, 58(17): 1732001 Copy Citation Text show less
    Structure of single event effect test calibration system
    Fig. 1. Structure of single event effect test calibration system
    4-chip storage structure of AT68166F chip
    Fig. 2. 4-chip storage structure of AT68166F chip
    8-region storage structure of AT60142F chip
    Fig. 3. 8-region storage structure of AT60142F chip
    Overall structure of heavy ion single particle calibration system
    Fig. 4. Overall structure of heavy ion single particle calibration system
    Heavy ion single particle calibration system plate
    Fig. 5. Heavy ion single particle calibration system plate
    Flip distribution of C ion irradiation at different incident angles (test data is 00). (a) Incident angle is 0; (b) incident angle is 45°; (c) incident angle is 60°
    Fig. 6. Flip distribution of C ion irradiation at different incident angles (test data is 00). (a) Incident angle is 0; (b) incident angle is 45°; (c) incident angle is 60°
    Flip distribution of C ion irradiation at different incident angles (test datas is FF). (a) Incident angle is 0; (b) incident angle is 45°; (c) incident angle is 60°
    Fig. 7. Flip distribution of C ion irradiation at different incident angles (test datas is FF). (a) Incident angle is 0; (b) incident angle is 45°; (c) incident angle is 60°
    Single particle flip distribution of Kr ion irradiation. (a) Incident angle is 0, and test data is 00; (b) incident angle is 0, and test data is FF
    Fig. 8. Single particle flip distribution of Kr ion irradiation. (a) Incident angle is 0, and test data is 00; (b) incident angle is 0, and test data is FF
    ModuleDescription
    Serial controlSet serial port parameters
    Serial receiving and sendingSend and receive data by serial port
    Reading and writingWrite data to the disk and data stream mode read
    Chart drawingDraw curve graphs and scatter plots under XY coordinates
    Error statisticsCompare with the initial vector and count the number of errors
    Section calculationCalculate the cross section
    Write to vectorSend commands to the calibration system to achieve write operations to the target device
    Read dataSend commands to the calibration system,the calibration system is used to read the target device data,and the PC is uesd to save the returned data
    Current and voltage monitoringDisplay the voltage and current data sent back
    InputEnter the radiation source information,including particle type,energy,etc.,and save it
    TransferInquire,select and other operations to obtain the entered radiation source information
    Calibration system reference data displayDraw the reference data curve of the calibration system
    Field data annotationCalculate the field cross-section and standardize it in the graph
    Addition,deletion,and modificationManage the calibration data of the radiation source that has been verified to be correct,including data addition,deletion,and modification
    Calibration data queryInquire or display historical calibration data
    Table 1. Functional design of software
    IonAngle /(°)LET /(MeV·cm2·mg-1Data modeFluence rate /(cm-2·s-1Fluence /cm-2ExperimentphenomenonWrong numberCross section size per 1 bit /cm2
    C01.73009.50×1031.00×106SEU966.00×10-12
    C01.73FF9.50×1031.00×106SEU976.06×10-12
    C452.45009.50×1035.00×105SEU961.20×10-11
    C452.45FF9.50×1035.00×105SEU718.88×10-12
    C603.46009.50×1032.50×105SEU1774.43×10-11
    C603.46FF9.50×1032.50×105SEU1263.15×10-11
    F04.70FF1.10×1041.00×106SEU1156897.23×10-9
    F04.70001.10×1041.00×105SEU134538.41×10-9
    F04.70FF4.80×1031.00×105SEU119837.49×10-9
    F456.60004.80×1035.00×104SEU88341.10×10-8
    F456.60FF4.80×1035.00×104SEU78379.80×10-9
    F609.40004.80×1032.50×104SEU59231.48×10-8
    F609.40FF4.80×1032.50×104SEU57881.45×10-8
    I065.60005.00×1021.00×104SEU104666.54×10-8
    I065.60FF5.00×1021.00×104SEU70534.41×10-8
    I4592.80005.00×1025.00×103SEU50776.35×10-8
    I4592.80FF5.00×1025.00×103SEU41825.23×10-8
    I60131.20005.00×1025.00×103SEU52846.61×10-8
    I60131.20FF1.00×1035.00×103SEU49176.15×10-8
    Li00.44002.30×1042.00×106SEU175.31×10-13
    Li00.44FF2.30×1042.00×106SEU165.00×10-13
    Li450.62002.30×1041.00×106SEU74.38×10-13
    Li450.62FF2.30×1041.00×106SEU63.75×10-13
    Li600.88002.30×1045.00×105SEU33.75×10-13
    Li600.88FF2.30×1045.00×105SEU78.75×10-13
    O03.10001.30×1031.00×105SEU12908.06×10-10
    O03.10FF1.30×1031.00×105SEU6173.86×10-10
    O03.10FF1.30×1031.00×105SEU5053.16×10-10
    O454.40001.30×1031.00×105SEU118117.38×10-9
    O454.40FF1.30×1031.00×105SEU62753.92×10-9
    O606.20001.30×1031.00×105SEU137048.57×10-9
    O606.20FF1.30×1031.00×105SEU112957.06×10-9
    Si09.00003.90×1025.00×104SEU220082.75×10-8
    Si09.00FF3.90×1025.00×104SEU175222.19×10-8
    Si4512.70003.90×1025.00×104SEU264233.30×10-8
    Si4512.70FF3.90×1023.00×104SEU190593.97×10-8
    Si6018.00003.90×1023.00×104SEU171143.57×10-8
    Si6018.00FF3.90×1023.00×104SEU168323.51×10-8
    Ge037.30002.50×1041.50×106SEU7467913.11×10-8
    Ge037.30FF1.35×1048.10×105SEU3386162.61×10-8
    Ge037.30001.28×1037.70×104SEU384403.12×10-8
    Ge037.30FF1.42×1038.50×104SEU380482.80×10-8
    Ti021.84001.90×1031.20×105SEU327361.70×10-8
    Ti021.84FF1.80×1031.10×105SEU294741.70×10-8
    Cl013.40001.70×1031.00×105SEU238441.50×10-8
    Cl013.40FF5.00×1023.00×104SEU68161.42×10-8
    Ta081.35001.01×1041.01×106SEU788486.19×10-8
    Kr020.30FF2.50×1041.01×106SEU220101.31×10-8
    Kr020.30002.50×1041.01×106SEU228241.35×10-8
    Table 2. Summary of single particle irradiation test data[7-8]
    IonThis paperCIAEESA
    LET /(MeV·cm2·mg-1Cross section size per 1 bit /cm2①LET /(MeV·cm2·mg-1Cross section size per 1 bit /cm2Error /%LET /(MeV·cm2·mg-1Cross section size per 1 bit /cm2②Error /%
    Li0.445.16×10-13
    Li0.624.07×10-13
    Li0.886.25×10-13
    C1.736.03×10-121.84.90×10-1218.741.681.46×10-11⑥142.12
    C2.451.04×10-112.51.00×10-113.852.342.68×10-11⑥157.69
    C3.463.79×10-113.64.67×10-1123.22
    O3.105.96×10-103.039.42×10-10⑥58.05
    O4.405.65×10-94.35.37×10-94.964.554.54×10-9⑥19.65
    O6.207.82×10-96.27.07×10-99.596.297.11×10-9⑥9.08
    F4.707.95×10-9
    F6.601.04×10-8
    F9.401.47×10-88.81.03×10-829.939.971.53×10-8⑥4.08
    Si9.002.47×10-8
    Si12.703.64×10-813.861.98×10-8⑥45.60
    Si18.003.54×10-820.342.39×10-8⑥32.49
    Cl13.401.46×10-813.81.93×10-8
    Kr20.301.34×10-820.92.30×10-871.60
    Ti21.841.70×10-820.92.30×10-835.30
    Ge37.002.28×10-833.53.14×10-837.70
    Ge37.302.91×10-833.53.14×10-87.90
    Ge52.303.28×10-8
    I65.605.48×10-867.44.99×10-88.9464.406.79×10-8⑥23.91
    Ta81.356.19×10-8
    Ta92.805.79×10-8
    Ta131.206.38×10-8111.921.08×10-7⑥69.28
    Table 3. Comparison of single particle flip cross section data
    Haolin Liu, Qing Liu, Xiaohui Zhang, Jing Sun, Song Gu, Zhengyu Zhong. Heavy Ion Single Event Effect Test Calibration System[J]. Laser & Optoelectronics Progress, 2021, 58(17): 1732001
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