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Simulations of emission characteristics of a multigated single carbon nanotube field emitter

机译:多层单碳纳米管场致发射体发射特性的仿真

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In this study, a two-dimensional, particle-in-cell computer simulation code magic was used to investigate the field emission characteristics from a single closed-capped multiwalled carbon nanotube (MWCNT) in a particular quadruple-gated focusing configuration. Simulations have been done on a single MWCNT assuming it is a cylinder with an ellipsoidal cap of 40 nm major radius and 10 nm minor radius, 20 nm in base diameter, and 0.2 or 0.3 μm in height. Other simulation parameters in the base case are 0.1 μm thickness for each gate, uniform gate hole radius of 0.45 μm, and an anode-cathode distance of 20 μm. A particular quadruple-gated focusing configuration has been investigated with individual gate bottom to cathode top distances of 1.1, 1.8, 2.9, and 3.9 μm, respectively. For this particular quadruple-gated structure with a cathode voltage of 0 V, 85 V in voltage of the first gate, 224 V in voltage of the second gate, 1320 V in voltage of the third gate, 1331 V in voltage of the fourth gate, and an anode voltage of 1331 V, simulation result showed that a current-weighted beam spot radius on the anode plane can be reduced to 17.4 nm for a MWCNT height of 200 nm. The emission current, however, varies only slightly from 0.311 to 0.375 pA, as the voltage on the third gate is changed from 200 to 1500 V. The region in the vicinity of the second gate acts to focus the emitted electron beam, while that of the third gate acts to diverge the beam. It was also found that using a higher MWCNT would reduce the applied voltages, but the emitted electrons could not be as well focused as the case with shorter MWCNT. For a MWCNT height of 300 nm at about 0.3 pA emission current, the weighted beam radius is increased slightly to 28.8 nm at the optimum focusing condition. For the MWCNT height of 300 nm at a higher emission current about 3 nA, the weighted beam radius was found to increase to 46.4 nm at the optimum focusing condition. This study shows that it is possible to design a quadruple-gated MWCNT field emitter having few tens of nanometer focused beam size at picoampere to nanoampere emission current range and the designed field emitter is suitable for parallel electron-beam lithography applications.
机译:在这项研究中,使用二维粒子模拟计算机魔术代码来研究特定四重聚焦结构中单个封闭式多壁碳纳米管(MWCNT)的场发射特性。在单个MWCNT上进行了模拟,假设它是一个圆柱体,其椭圆形帽的长半径为40 nm,短半径为10 nm,基径为20 nm,高度为0.2或0.3μm。在基本情况下,其他模拟参数是每个浇口的厚度为0.1μm,均匀的浇口孔半径为0.45μm,阳极-阴极距离为20μm。已经研究了特殊的四重门聚焦配置,其中单个栅极底部到阴极顶部的距离分别为1.1、1.8、2.9和3.9μm。对于这种特殊的四栅极结构,其阴极电压为0 V,第一栅极的电压为85 V,第二栅极的电压为224 V,第三栅极的电压为1320 V,第四栅极的电压为1331 V仿真结果表明,阳极电压为1331 V,对于MWCNT高度为200 nm的阳极,电流加权的束斑半径可以减小到17.4 nm。然而,当第三栅极的电压从200 V变为1500 V时,发射电流仅在0.311至0.375 pA范围内变化。第二栅极附近的区域用于聚焦发射的电子束,而第三扇门发散光束。还发现使用较高的MWCNT会降低施加的电压,但是所发射的电子不能像较短的CNT那样集中。对于在约0.3 pA发射电流下的MWCNT高度为300 nm的情况,在最佳聚焦条件下,加权光束半径会稍微增加到28.8 nm。对于在约3 nA的较高发射电流下300纳米的CNT高度,发现在最佳聚焦条件下,加权束半径增加到46.4纳米。这项研究表明,有可能设计出一个四栅极MWCNT场发射器,该发射器在皮安至纳安发射电流范围内具有几十纳米的聚焦束大小,并且该设计的场发射器适用于平行电子束光刻应用。

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