首页> 外文学位 >Ballistic electron emission microscopy and internal photoemission study on metal bi-layer/oxide/silicon, high-k oxide/silicon, and 'end-on' metal contacts to vertical silicon nanowires.
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Ballistic electron emission microscopy and internal photoemission study on metal bi-layer/oxide/silicon, high-k oxide/silicon, and 'end-on' metal contacts to vertical silicon nanowires.

机译:金属双层/氧化物/硅,高k氧化物/硅以及垂直硅纳米线的“端对端”金属触点的弹道电子发射显微镜和内部光发射研究。

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摘要

In this thesis, three separate experiments involving electronic materials are described. Nanometer-spatial resolution ballistic electron emission microscopy (BEEM) is used to study the inhomogeneity of metal-bialyer/SiO2 interface, and small size and restricted geometry effect of "end-on" metal contacts to vertical Si NWs embedded in spin-on glass. BEEM and internal photoemission (Int-PE) are also combined for the first time to study conduction band and valence band offsets between Si and promising high-k (high dielectric constant) oxides: Sc2O3 and Lu 2O3.;In the first experiment, a comparison of the dependence on gate voltage of the average energy barrier measured by BEEM of a metal bi-layer Pt/Al/SiO 2/Si sample and a Pt/SiO2/Si sample suggests that the metal/oxide interface of the Pt/Al/SiO2/Si sample is laterally inhomogeneous at nm length scales. However, BEEM images of the bi-layer sample do not show significantly larger lateral variations than observed on a (uniform) Pt/SiO 2/Si sample, indicating that any inhomogeneous "patches" of lower energy barrier height have size smaller than the lateral resolution of BEEM, estimated for these samples to be ~10 nm. Finite element electrostatic simulations of an assumed inhomogeneous interface with nm size patches of different effective work function can fit the experimental data of the bi-layer sample much better than an assumed homogenous interface, indicating that bi-layer film is in fact laterally inhomogeneous at the nm scale.;Int-PE measurements on 20 nm-thick epitaxial Sc2O3 and Lu2O3 film on Si (111) show the existence of a lower "tail state" conduction band (CB) extending ~1 eV below the upper CB (similar to that reported for amorphous Sc2O3 and Lu2O3 films), indicating that these states are not simply due to disorder in amorphous films. BEEM measurements on epitaxial Sc 2O3/Si also show that this lower CB supports elastic hot-electron transport even against an applied electric field, indicating transport via extended rather than localized states.;BEEM measurements on "end-on" Au contacts to vertical Si NWs show strong suppression of hot-electron injection at higher injected current in the NWs (produced either by increasing the tip voltage or the tunneling current) comparing to a regular Au/Si junction, suggesting that this current suppression is due to a steady-state charge build-up in the NW that increase as more current is injected into the NW. The BEEM current suppression of most NWs was also found to increase strongly as the temperature was decreased, indicating more charge build-up at lower temperature. Time-dependent current suppression due to changing steady-state charge build-up in the NWs was observed when the tunnel current was abruptly increased and decreased, directly supporting a model in which the BEEM current suppression is due to (temperature-dependent) steady-state charge build up. Those electrons might be trapped at the Si NW/SiO 2 interface close to the metal/Si NW contact, which is consistent with finite element electrostatic simulations. Our BEEM measurements also show that the local Schottky barrier height (SBH) at the edge of two separate NWs is ~20 meV lower than at the NWs center. Finite element simulation suggests that the lower SBH at the contact edge might be due to the NW/oxide interface states charge together with the geometry enhanced electric field effect (the NWs protruding ~8 nm out of the spin-on glass).
机译:本文介绍了三个涉及电子材料的独立实验。纳米空间分辨率弹道电子发射显微镜(BEEM)用于研究金属-偏压/ SiO2界面的不均匀性,以及“端接式”金属触点对嵌入在旋涂玻璃中的垂直Si NW的小尺寸和受限的几何效应。还首次将BEEM和内部光发射(Int-PE)结合起来研究Si与有前景的高k(高介电常数)氧化物Sc2O3和Lu 2O3之间的导带和价带偏移。比较金属双层Pt / Al / SiO 2 / Si样品和Pt / SiO2 / Si样品的BEEM测量的平均能垒对栅极电压的依赖性,表明Pt / Al的金属/氧化物界面/ SiO2 / Si样品在纳米长度尺度上横向不均匀。但是,双层样品的BEEM图像没有显示出比在(均匀的)Pt / SiO 2 / Si样品上观察到的大的横向变化,这表明较低能垒高度的任何不均匀“斑块”的尺寸均小于横向尺寸。 BEEM的分辨率,估计这些样品约为10 nm。假设的具有不同有效功函数的纳米尺寸斑片的不均匀界面的有限元静电模拟可以比假设的均匀界面更好地拟合双层样品的实验数据,表明双层膜实际上在横向上是不均匀的。在Si(111)上20 nm厚的外延Sc2O3和Lu2O3膜上进行的Int-PE测量显示,存在一个较低的“尾态”导带(CB),该导带在上方CB下方延伸〜1 eV(类似于关于非晶态Sc2O3和Lu2O3薄膜的研究报道),表明这些状态不仅仅是由于非晶态薄膜中的无序。在外延Sc 2O3 / Si上进行的BEEM测量还表明,这种较低的CB即使在施加电场的情况下也支持弹性热电子传输,表明是通过扩展状态而不是局部状态进行传输。与常规的Au / Si结相比,NW在NW中以较高的注入电流(通过增加尖端电压或隧穿电流产生)对热电子注入具有强烈的抑制作用,这表明这种电流抑制是由于稳态随着更多的电流注入到NW中,NW中的电荷积累会增加。随着温度的降低,大多数NW的BEEM电流抑制也显着增加,表明在较低温度下更多的电荷积聚。当隧道电流突然增加和减少时,可以观察到由于NW中稳态电荷积累的变化而引起的与时间有关的电流抑制,这直接支持了一个模型,其中BEEM电流抑制是由(与温度有关的)稳态引起的。国家电荷积累。这些电子可能会在靠近金属/ Si NW接触的Si NW / SiO 2界面处被捕获,这与有限元静电模拟是一致的。我们的BEEM测量还显示,两个独立NW边缘处的局部肖特基势垒高度(SBH)比NW中心低约20 meV。有限元模拟表明,接触边缘较低的SBH可能是由于NW /氧化物界面态电荷以及几何形状增强的电场效应(NW从旋涂玻璃伸出约8 nm)引起的。

著录项

  • 作者

    Cai, Wei.;

  • 作者单位

    The Ohio State University.;

  • 授予单位 The Ohio State University.;
  • 学科 Physics Condensed Matter.
  • 学位 Ph.D.
  • 年度 2010
  • 页码 205 p.
  • 总页数 205
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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