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微波烧结制备钨锇混合基扩散阴极及其发射性能

刘伟, 胡志凯, 李世磊, 周帆, 杨韵斐, 张小可, 谢元峰, 王金淑

刘伟, 胡志凯, 李世磊, 周帆, 杨韵斐, 张小可, 谢元峰, 王金淑. 微波烧结制备钨锇混合基扩散阴极及其发射性能[J]. 粉末冶金技术, 2023, 41(3): 199-209. DOI: 10.19591/j.cnki.cn11-1974/tf.2021090011
引用本文: 刘伟, 胡志凯, 李世磊, 周帆, 杨韵斐, 张小可, 谢元峰, 王金淑. 微波烧结制备钨锇混合基扩散阴极及其发射性能[J]. 粉末冶金技术, 2023, 41(3): 199-209. DOI: 10.19591/j.cnki.cn11-1974/tf.2021090011
LIU Wei, HU Zhikai, LI Shilei, ZHOU Fan, YANG Yunfei, ZHANG Xiaoke, XIE Yuanfeng, WANG Jinshu. Preparation and emission performance of tungsten-osmium mixed matrix dispenser cathode by microwave sintering[J]. Powder Metallurgy Technology, 2023, 41(3): 199-209. DOI: 10.19591/j.cnki.cn11-1974/tf.2021090011
Citation: LIU Wei, HU Zhikai, LI Shilei, ZHOU Fan, YANG Yunfei, ZHANG Xiaoke, XIE Yuanfeng, WANG Jinshu. Preparation and emission performance of tungsten-osmium mixed matrix dispenser cathode by microwave sintering[J]. Powder Metallurgy Technology, 2023, 41(3): 199-209. DOI: 10.19591/j.cnki.cn11-1974/tf.2021090011

微波烧结制备钨锇混合基扩散阴极及其发射性能

详细信息
    通讯作者:

    王金淑: E-mail: wangjsh@bjut.edu.cn

  • 中图分类号: TF124

Preparation and emission performance of tungsten-osmium mixed matrix dispenser cathode by microwave sintering

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  • 摘要:

    采用固–液混合法制备出不同锇(Os)含量(原子数分数)的亚微米级钨锇混合粉体,通过微波烧结获得了孔道结构均匀的钨锇混合基扩散型阴极。电子发射测试结果表明,元素Os的加入使浸渍型钨基阴极的发射性能有明显提高。对比不同锇含量的混合基阴极,发现W–25Os阴极(Os原子数分数为25%)具有相对较低的逸出功和较高的发射电流密度,其在1100 ℃时脉冲发射电流密度为42.86 A·cm−2,斜率为1.40,发射电流密度是同等工作条件下传统钡钨阴极的1.7倍,达到了覆膜M型阴极的电子发射水平。W–25Os混合基阴极的有效逸出功最低为1.93 eV,有利于活性自由钡(Ba)的生成,表层元素摩尔比Ba:(W+Os)为0.83:1.00,比传统钡钨阴极中Ba:W(约为0.50:1.00)摩尔比有了明显提高。

    Abstract:

    Submicron tungsten-osmium mixed powders with the different content of Os (atomic number fraction) were prepared by solid‒liquid mixing method. The tungsten-osmium mixed matrix disperser cathodes with the uniform pore structure were obtained by microwave sintering. The electron emission testing results show that, the addition of Os obviously improves the emission performance of the impregnated tungsten-based dispenser cathode. The W–25Os cathode (Os atomic number fraction is 25%) exhibits the relatively low work function and high emission current density. At 1100 ℃, the pulse emission current density of the W–25Os cathode is 42.86 A·cm−2 with the emission slope of 1.40, which is 1.7 times of the conventional barium-tungsten dispenser cathodes under the same working conditions and up to the electron emission level of M-type cathodes. The W–25Os cathode shows the low effective work function as 1.93 eV, which is conducive to the generation of active free barium source. The molar ratio of surface elements Ba:(W+Os) is 0.83:1.00, which is significantly higher than that of the traditional barium tungsten cathode (about 0.50:1.00).

  • 图  1   氢气还原W–Os混合粉末X射线衍射图谱

    Figure  1.   XRD patterns of the W–Os mixed powders after hydrogen reduction

    图  2   原始Os粉、氢气还原W粉末及W–Os混合粉末的扫描电子显微形貌:(a)原始Os粉;(b)氢气还原W粉;(c)W–15Os;(d)W–25Os;(e)W–50Os;(f)W–75Os

    Figure  2.   SEM images of the original Os powders, the hydrogen reduced W powders, and the W–Os mixed powders: (a) original Os powders; (b) hydrogen reduced W powders; (c) W–15Os; (d) W–25Os; (e) W–50Os; (f) W–75Os

    图  3   原始Os粉、氢气还原W粉末和W–Os混合粉末的粒度分布曲线:(a)原始Os粉;(b)氢气还原W粉;(c)W–15Os;(d)W–25Os;(e)W–50Os;(f)W–75Os

    Figure  3.   Particle size distribution curves of the original Os powders, the hydrogen reduced W powders, and the W–Os mixed powders: (a) original Os powders; (b) hydrogen reduced W powders; (c) W–15Os; (d) W–25Os; (e) W–50Os; (f) W–75Os

    图  4   W–25Os粉末能谱面扫图

    Figure  4.   EDS mapping images of the W–25Os mixed powders

    图  5   不同温度微波烧结的W–25Os基体表面扫描电子显微形貌:(a)1450 ℃;(b)1500 ℃;(c)1550 ℃;(d)1600 ℃

    Figure  5.   SEM images of the W–25Os mixed matrix surfaces sintered by microwave sintering: (a) 1450 ℃; (b) 1500 ℃; (c) 1550 ℃; (d) 1600 ℃

    图  6   微波烧结W–25Os基体断面扫描电子显微形貌(a)~(c)及能谱面扫图(d)~(f)

    Figure  6.   SEM ((a)~(c)) and EDS mapping images ((d)~(f)) of the W–25Os mixed matrix in the cross section after microwave sintering

    图  7   W–Os混合基体X射线衍射图谱

    Figure  7.   XRD patterns of the W–Os mixed matrix with the different osmium concentrations

    图  8   W–Os混合基阴极表面扫描电子显微形貌:(a)W–15Os;(b)W–25Os;(c)W–50Os;(d)W–75Os;(e)Ba–W

    Figure  8.   SEM images of the W–Os mixed matrix dispenser cathodes with the different osmium concentrations: (a) W–15Os; (b) W–25Os; (c) W–50Os; (d) W–75Os; (e) Ba–W

    图  9   W–25Os混合基阴极能谱面扫图

    Figure  9.   EDS mapping images of the W–25Os mixed matrix dispenser cathode

    图  10   W–Os混合基阴极与钡钨阴极脉冲发射曲线和逸出功曲线:(a)W–15Os;(b)W–25Os;(c)W–50Os;(d)W–75Os;(e)Ba–W

    Figure  10.   Pulsed emission curves and work function curves of the W–Os mixed matrix dispenser cathodes and the barium impregnated tungsten cathodes: (a) W–15Os; (b) W–25Os; (c) W–50Os; (d) W–75Os; (e) Ba–W

    图  11   W–25Os混合基阴极表面活性元素X射线光电子能谱图:(a)W4f;(b)Os4f;(c)O1s;(d)Ba3d

    Figure  11.   Surface active element XPS spectra of the W–25Os mixed matrix dispenser cathodes: (a) W4f; (b) Os4f; (c) O1s; (d) Ba3d

    图  12   浸渍411活性盐Ba–W(a)和W–25Os阴极(b)充分激活后表面俄歇谱图

    Figure  12.   AES spectra of the activated Ba–W (a) and W–25Os dispenser cathodes (b) impregnated with 411 salt

    表  1   W–Os混合基阴极与Ba‒W阴极逸出功

    Table  1   Work functions of the W–Os mixed matrix dispenser cathodes and the barium impregnated tungsten cathodes

    阴极编号功函数 / eV
    W–15Os1.97
    W–25Os1.93
    W–50Os1.96
    W–75Os1.94
    Ba–W2.03
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出版历程
  • 收稿日期:  2021-09-15
  • 录用日期:  2021-09-15
  • 网络出版日期:  2021-11-07
  • 刊出日期:  2023-06-27

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