We present a comprehensive study of field emitter arrays with or without an integrated focus electrode. The former configuration is referred to as field emitter with integrated focus (IFE-FEA) or double-gate FEA (DG-FEA). The main application of IFE-FEA is to improve the resolution of field emission displays (FEDs). We developed the first analytical model of conical field emitters that captures all details of device geometry and produces quantitatively accurate closed-form expressions for the FN coefficients. A novel CMP-based process for making IFE-FEA is presented. We obtained devices with gate and focus apertures of 0.8 and 1.2 gm diameter, respectively, which is 1.5 times smaller than in any previously reported IFE-FEA. Single-gate FEAs whose gate was identical to the lower gate of the IFE-FEA were also fabricated. Their emission current was 100 nA/tip at 45 V; for IFE-FEAs with the gate and focus biased at the same potential (VG=VF) this figure was 100 nA/tip at 42 V, in agreement with the analytical model. It was deduced that the tip radius of curvature (ROC) is 2.4-3.6 nm. Analytical model, numerical simulation, and TEM micrographs all gave tip ROC values in this range. We generalized the FN equation to IFE-FEA and used 4-terminal measurements to determine gate and focus field factors, [3G and 13F. Their ratio was found to vary from 0.15 (emission current independent of focus voltage) to 2.7. We demonstrated via numerical simulation that this ratio is probably determined by the degree of gate shielding of the tip.
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机译:我们对有或没有集成聚焦电极的场发射器阵列进行了全面的研究。前一种配置称为集成聚焦场发射器(IFE-FEA)或双栅极FEA(DG-FEA)。 IFE-FEA的主要应用是提高场发射显示器(FED)的分辨率。我们开发了第一个圆锥形场发射器分析模型,该模型捕获了器件几何结构的所有细节,并为FN系数生成了定量精确的闭合形式表达式。提出了一种新颖的基于CMP的制造IFE-FEA的方法。我们获得的器件的栅孔和聚焦孔的直径分别为0.8和1.2 gm,比以前报道的IFE-FEA小1.5倍。还制作了其栅极与IFE-FEA的下部栅极相同的单栅极FEA。它们的发射电流在45 V时为100 nA / tip;对于具有相同电位(VG = VF)的栅极和聚焦偏置的IFE-FEA,该数字在42 V时为100 nA /尖端,与分析模型一致。推断出尖端的曲率半径(ROC)为2.4-3.6nm。分析模型,数值模拟和TEM显微照片均给出了该范围内的尖端ROC值。我们将FN方程推广到IFE-FEA,并使用4端子测量来确定栅极和聚焦场因子[3G和13F。发现它们的比率从0.15(与聚焦电压无关的发射电流)变化到2.7。我们通过数值模拟证明了该比率可能由尖端的栅极屏蔽程度决定。
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