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Deposition of TiO_2/Al_2O_3 bilayer on hydrogenated diamond for electronic devices: Capacitors, field-effect transistors, and logic inverters

机译:在电子设备的氢化金刚石上沉积TiO_2 / Al_2O_3双层:电容器,场效应晶体管和逻辑逆变器

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摘要

The wide bandgap semiconductor diamond has been studied to develop high-power and high-frequency electronic devices. Here, high dielectric constant (high-A:) TiO_2/Al_2O_3 bilayers are deposited on hydrogenated diamond (H-diamond) channel layers using sputter deposition (SD) and atomic layer deposition (ALD) techniques. Thin ALD-Al_2O_3 films are employed as buffer layers for the SD-TiO_2 and ALD-TiO_2 on H-diamond to suppress plasma discharge effect and to decrease leakage current density (J), respectively. The electrical properties of the resulting TiO_2/Al_2O_3/H-diamond metal-oxide-semiconductor (MOS) capacitors, MOS field-effect transistors (MOSFETs), and MOSFET logic inverters are investigated. With the same thickness (4.0 nm) for ALD-A1_2O_3 buffer layer, the ALD-TiO_2/ALD-Al_2O_3/H-diamond MOS capacitor shows a lower / and better capacitance-voltage characteristics than the SD-TiO_2/ALD-Al_2O_3/H-diamond capacitor. The maximum capacitance of the ALD-TiO_2/ALD-Al_2O_3/H-diamond capacitor and the k value of the ALD-TiO_2/ALD-AL_2O_3 bilayer are 0.83 µF cm~(-2) and 27.2, respectively. Valence band offset between ALD-TiO_2 and H-diamond is calculated to be 2.3 ± 0.2 eV based on the element binding energies measured using an X-ray photoelectron spectroscopy technique. Both the SD-TiO_2/ALD-Al_2O_3/ H-diamond and ALD-TiO_2/VALD-Al_2O_3/H-diamond MOSFETs show p-type, pinch-off, and enhancement mode characteristics with on/off current ratios around 10~9. The subthreshold swings of them are 115 and as low as 79 mV dec~(-1), respectively. The ALD-TiO_2/ALD-Al_2O_3/H-diamond MOSFET logic inverters, when coupled with load resistors, show distinct inversion characteristics with gains of 6.2-12.7.
机译:已经研究了宽带隙半导体金刚石以开发高功率和高频电子设备。在这里,使用溅射沉积(SD)和原子层沉积(ALD)技术将高介电常数(high-A :) TiO_2 / Al_2O_3双层沉积在氢化金刚石(H-金刚石)通道层上。 ALD-Al_2O_3薄膜用作H-金刚石上SD-TiO_2和ALD-TiO_2的缓冲层,分别抑制等离子体放电效果和降低漏电流密度(J)。研究了所得的TiO_2 / Al_2O_3 / H金刚石金属氧化物半导体(MOS)电容器,MOS场效应晶体管(MOSFET)和MOSFET逻辑反相器的电性能。在ALD-A1_2O_3缓冲层具有相同的厚度(4.0 nm)的情况下,ALD-TiO_2 / ALD-Al_2O_3 / H金刚石MOS电容器显示出比SD-TiO_2 / ALD-Al_2O_3 / H更低/更好的电容电压特性。 -金刚石电容器。 ALD-TiO_2 / ALD-Al_2O_3 / H金刚石电容器的最大电容和ALD-TiO_2 / ALD-AL_2O_3双层的k值分别为0.83 µF cm〜(-2)和27.2。基于使用X射线光电子能谱技术测量的元素结合能,ALD-TiO_2和H-金刚石之间的价带偏移被计算为2.3±0.2eV。 SD-TiO_2 / ALD-Al_2O_3 / H-金刚石和ALD-TiO_2 / VALD-Al_2O_3 / H-金刚石MOSFET均具有p型,夹断和增强模式特性,开/关电流比约为10〜9。它们的亚阈值摆幅分别为115和低至79 mV dec〜(-1)。当与负载电阻耦合时,ALD-TiO_2 / ALD-Al_2O_3 / H金刚石MOSFET逻辑反相器表现出明显的反相特性,增益为6.2-12.7。

著录项

  • 来源
    《Journal of Applied Physics》 |2017年第22期|224502.1-224502.10|共10页
  • 作者单位

    Research Center for Functional Materials, National Institute for Materials Science (NIMS), 1-1 Namiki,Tsukuba, Ibaraki 305-0044, Japan;

    Research Center for Functional Materials, National Institute for Materials Science (NIMS), 1-1 Namiki,Tsukuba, Ibaraki 305-0044, Japan;

    Research Center for Functional Materials, National Institute for Materials Science (NIMS), 1-1 Namiki,Tsukuba, Ibaraki 305-0044, Japan;

    Research Center for Functional Materials, National Institute for Materials Science (NIMS), 1-1 Namiki,Tsukuba, Ibaraki 305-0044, Japan;

    Research Network and Facility Services Division, NIMS, 1-2-1 Sengen, Tsukuba, Ibaraki 305-0047, Japan;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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