李伊濛, 李南, 夏凌寒, 刘佳薇, 张鹏, 肖冰, 成永红, 孟国栋. 真空纳米间隙的脉冲击穿特性[J]. 高电压技术, 2025, 51(1): 450-458. DOI: 10.13336/j.1003-6520.hve.20240244
引用本文: 李伊濛, 李南, 夏凌寒, 刘佳薇, 张鹏, 肖冰, 成永红, 孟国栋. 真空纳米间隙的脉冲击穿特性[J]. 高电压技术, 2025, 51(1): 450-458. DOI: 10.13336/j.1003-6520.hve.20240244
LI Yimeng, LI Nan, XIA Linghan, LIU Jiawei, ZHANG Peng, XIAO Bing, CHENG Yonghong, MENG Guodong. Pulsed Breakdown Characteristics Across Vacuum Nanogap[J]. High Voltage Engineering, 2025, 51(1): 450-458. DOI: 10.13336/j.1003-6520.hve.20240244
Citation: LI Yimeng, LI Nan, XIA Linghan, LIU Jiawei, ZHANG Peng, XIAO Bing, CHENG Yonghong, MENG Guodong. Pulsed Breakdown Characteristics Across Vacuum Nanogap[J]. High Voltage Engineering, 2025, 51(1): 450-458. DOI: 10.13336/j.1003-6520.hve.20240244

真空纳米间隙的脉冲击穿特性

Pulsed Breakdown Characteristics Across Vacuum Nanogap

  • 摘要: 极端强电场下的绝缘可靠性问题是限制微纳电子器件性能提升的主要因素之一,因此认识纳米间隙的击穿特性以及绝缘失效机制极为重要。为此,利用高分辨成像技术与纳米级精密位移技术,基于透射电子显微镜与电学样品杆建立了真空纳米间隙脉冲击穿测试系统,实现了空间分辨率为1 nm的精准间隙调控,研究了纳米间隙距离(5~25 nm)、外施电压脉冲宽度(100~1 000 ns)对球-板真空间隙脉冲击穿阈值的影响,讨论了纳米间隙的脉冲击穿过程。结果表明:脉冲击穿电压与间隙距离呈线性关系即Ub=Ecd,且基本不随脉冲宽度变化,击穿场强阈值基本不变,约为8.8 GV/m;纳米间隙距离越小,径向电场梯度越大,场发射有效区域越小;球-板电极均匀场下的脉冲击穿过程为阳极金板在阴极钨球场发射电流的能量沉积下温度升高至接近熔点,进而发生热失控并诱导击穿;击穿过程的持续时间约为25 ns,与间隙距离以及脉冲宽度无关,且反映了阳极表面蒸发的原子在间隙内形成等离子体通道并导致阴极蒸发的时间。

     

    Abstract: The insulation reliability problem under an extremely strong electric field is a key factor limiting the performance improvement of micro and nano electronic devices, so it is very important to understand the breakdown characteristics and the insulation failure mechanisms of nanogaps. In this paper, we utilize high-resolution imaging technology and nanoscale precision displacement technology to establish a vacuum nanogap pulsed breakdown test system based on transmission electron microscope and electrical sample holder, which can achieve accurate gap regulation with a spatial resolution of 1 nm. The effects of nanogap distance (5~25 nm) and applied voltage pulse width (100~1 000 ns) on the pulsed breakdown threshold of sphere-plate vacuum gap are studied. The results show that the relationship between pulsed breakdown voltage and gap distance is linear, that is, Ub=Ecd, and does not change with pulsed width. The breakdown field strength threshold is basically unchanged, about 8.8 GV/m. A smaller nanogap distance leads to a more concentrated electric field distribution and a smaller effective field emission region. The pulsed breakdown process of sphere-plate electrode under a uniform field is that the temperature of anode gold plate rises to nearly melting point under the energy deposition of cathode tungsten field emission current, and then thermal runaway occurs, resulting in electrical breakdown. This process, lasting approximately 25 ns, is independent of both gap distance and pulse width, which reflects the time required for vaporized atoms on the anode surface to form a plasma channel within the gap and to facilitate the cathode evaporation.

     

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