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无窗X射线能谱在荧光样品与金属锂成分分析中的优势与经验摸索

万鹏 蔡蕊 李勇 孟祥玉 周雨萌 高晓霞 徐强 闫肃

万鹏, 蔡蕊, 李勇, 孟祥玉, 周雨萌, 高晓霞, 徐强, 闫肃. 无窗X射线能谱在荧光样品与金属锂成分分析中的优势与经验摸索[J]. 分析测试技术与仪器, 2023, 29(3): 313-320. doi: 10.16495/j.1006-3757.2023.03.011
引用本文: 万鹏, 蔡蕊, 李勇, 孟祥玉, 周雨萌, 高晓霞, 徐强, 闫肃. 无窗X射线能谱在荧光样品与金属锂成分分析中的优势与经验摸索[J]. 分析测试技术与仪器, 2023, 29(3): 313-320. doi: 10.16495/j.1006-3757.2023.03.011
WAN Peng, CAI Rui, LI Yong, MENG Xiangyu, ZHOU Yumeng, GAO Xiaoxia, XU Qiang, YAN Su. Advantage and Experience of Windowless X-ray Energy Dispersive Spectroscopy at Composition Analysis of Fluorescent Sample and Lithium Metal[J]. Analysis and Testing Technology and Instruments, 2023, 29(3): 313-320. doi: 10.16495/j.1006-3757.2023.03.011
Citation: WAN Peng, CAI Rui, LI Yong, MENG Xiangyu, ZHOU Yumeng, GAO Xiaoxia, XU Qiang, YAN Su. Advantage and Experience of Windowless X-ray Energy Dispersive Spectroscopy at Composition Analysis of Fluorescent Sample and Lithium Metal[J]. Analysis and Testing Technology and Instruments, 2023, 29(3): 313-320. doi: 10.16495/j.1006-3757.2023.03.011

无窗X射线能谱在荧光样品与金属锂成分分析中的优势与经验摸索

doi: 10.16495/j.1006-3757.2023.03.011
详细信息
    作者简介:

    万鹏(1981−),女,博士,主要从事电子显微分析,E-mail:pengwan@dlut.edu.cn

  • 中图分类号: O657. 62

Advantage and Experience of Windowless X-ray Energy Dispersive Spectroscopy at Composition Analysis of Fluorescent Sample and Lithium Metal

  • 摘要: 用扫描电子显微镜搭载的有窗X射线能谱仪(EDS能谱)对荧光样品进行分析时,由于电子束的激发作用,样品受激自发产生的荧光将严重干扰EDS能谱探头对特征X射线的分析,最终导致定量困难甚至难以定性. 新型无窗EDS能谱由于其优异的低能量端信号采集与分析能力,结合单颗粒小区域采集的方法,可以成功实现荧光样品的正常EDS能谱分析. 由于无窗EDS能谱仪没有传统薄膜窗口的吸收作用,其最低可分析元素为锂. 通过优化加速电压,并借助样品表面钝化膜的保护作用,克服了背景噪音与样品污染的干扰,成功实现对单质锂的检测.
  • 图  1  有窗EDS能谱在15 kV加速电压下分析两种荧光粉得到的异常EDS能谱图

    (a)铈掺杂钇铝石榴石荧光粉的EDS能谱图,(a-1)为其荧光发射光谱图,(b)铕掺杂氮化物荧光粉的EDS能谱图,(b-1)为其荧光发射光谱图

    Figure  1.  Abnormal EDS spectra of two fluorescent powder samples obtained by windowed EDS at 15 kV

    (a) EDS spectrum of Y3Al5O12:Ce, (a-1) fluorescence spectrum of Y3Al5O12:Ce, (b) EDS spectrum of SrAlSiN3:Eu, (b-1) fluorescence spectrum of SrAlSiN3:Eu

    图  2  电子束加速电压和采集区域大小对铈掺杂钇铝石榴石荧光粉EDS能谱分析的影响

    (a-1) ~ (c-1)分别为大区域采集下电子束加速电压为15、10和5 kV时的EDS能谱图,(a-2) ~ (c-2)分别为单颗粒采集下电子束加速电压为15、10和5 kV时的EDS能谱图

    Figure  2.  Effect of accelerating voltages and scanning areas on EDS spectra of Y3Al5O12:Ce

    (a-1) ~ (c-1) accelerating voltages of 15, 10 and 5 kV, respectively, focused on large scanning area, (a-2) ~ (c-2) accelerating voltages of 15, 10 and 5 kV, respectively, focused on single particle

    图  3  利用无窗EDS能谱得到的无荧光干扰EDS能谱图

    (a)铈掺杂钇铝石榴石荧光粉,(b)铕掺杂氮化物荧光粉

    Figure  3.  EDS spectra without fluorescence interference of (a) Y3Al5O12:Ce and (b) SrAlSiN3:Eu by windowless EDS

    图  4  不同条件下锂峰的出峰与峰形

    (a)电子束加速电压为5 kV时样品表面氧化严重,电子束加速电压为(b)1 kV,(c)10 kV,(d)5 kV时受表面钝化膜保护的样品,电子束加速电压为(e)3 kV,(f)5 kV时样品表面经过长时间电子束辐照

    Figure  4.  Emergence and shape of peaks of lithium under different conditions (a) severely oxidized samples of surfaces under 5 kV, samples protected by passivation films under (b) 1 kV, (c) 10 kV, (d) 5 kV, sample areas of surfaces under repeated radiation by electron beam under (e) 3 kV, (f) 5 kV

    表  1  有窗EDS能谱在不同电子束加速电压下对铈掺杂钇铝石榴石荧光粉的定量分析结果

    Table  1.   Compositional analysis of Y3Al5O12:Ce by windowed EDS under different accelerating voltages /%

    Y重量分数Al重量分数O重量分数Ce重量分数Y∶Al∶O原子比
    (理论值1∶1.67∶4)
    15 kV大区域NullNullNullNullNull
    10 kV大区域100000Null
    5 kV大区域51.022.024.02.91∶1.42∶2.64
    15 kV单颗粒51.024.123.11.01∶1.55∶1.78
    10 kV单颗粒48.023.127.41.51∶1.52∶1.64
    5 kV单颗粒48.321.328.91.51∶1.44∶3.30
    下载: 导出CSV

    表  2  铈掺杂钇铝石榴石荧光粉和铕掺杂氮化物荧光粉的无窗EDS能谱定量分析结果

    Table  2.   Compositional analysis of Y3Al5O12:Ce and SrAlSiN3:Eu analyzed by windowless EDS /%

    物质元素质量分数原子
    百分比
    Y3Al5O12∶Ce(Y∶Al∶O原子比理论值为1∶1.67∶4)Y4113.1
    Al22.523.6
    O35.663.1
    Ce0.90.2
    SrAlSiN3∶Eu(Sr∶Al∶Si∶N原子比理论值为1∶1∶1∶3)N23.750.1
    Al1617.5
    Si16.917.8
    Sr42.114.3
    Eu1.30.3
    下载: 导出CSV
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出版历程
  • 收稿日期:  2023-05-26
  • 录用日期:  2023-07-14
  • 修回日期:  2023-07-14
  • 刊出日期:  2023-09-25

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