Ge interface engineering using ultra-thin La2O3 and Y2O3 films: A study into the effect of deposition temperature

被引:48
作者
Mitrovic, I. Z. [1 ]
Althobaiti, M. [2 ,3 ]
Weerakkody, A. D. [1 ]
Dhanak, V. R. [2 ,3 ]
Linhart, W. M. [2 ,3 ]
Veal, T. D. [2 ,3 ]
Sedghi, N. [1 ]
Hall, S. [1 ]
Chalker, P. R. [4 ]
Tsoutsou, D. [5 ]
Dimoulas, A. [5 ]
机构
[1] Univ Liverpool, Dept Elect Engn & Elect, Liverpool L69 3GJ, Merseyside, England
[2] Univ Liverpool, Dept Phys, Liverpool L69 7ZF, Merseyside, England
[3] Univ Liverpool, Stephenson Inst Renewable Energy, Liverpool L69 7ZF, Merseyside, England
[4] Univ Liverpool, Dept Engn, Liverpool L69 3GH, Merseyside, England
[5] NCSR Demokritos, MBE Lab, Inst Mat Sci, Athens 15310, Greece
基金
英国工程与自然科学研究理事会;
关键词
YTTRIUM-OXIDE FILMS; K GATE OXIDES; BAND OFFSETS; PHOTOELECTRON-SPECTROSCOPY; GERMANIUM OXIDES; LAYER; HFO2; DEFECTS; OXIDATION; MOSFETS;
D O I
10.1063/1.4868091
中图分类号
O59 [应用物理学];
学科分类号
摘要
A study into the optimal deposition temperature for ultra-thin La2O3/Ge and Y2O3/Ge gate stacks has been conducted in this paper with the aim to tailor the interfacial layer for effective passivation of the Ge interface. A detailed comparison between the two lanthanide oxides (La2O3 and Y2O3) in terms of band line-up, interfacial features, and reactivity to Ge using medium energy ion scattering, vacuum ultra-violet variable angle spectroscopic ellipsometry (VUV-VASE), X-ray photoelectron spectroscopy, and X-ray diffraction is shown. La2O3 has been found to be more reactive to Ge than Y2O3, forming LaGeOx and a Ge sub-oxide at the interface for all deposition temperature studied, in the range from 44 degrees C to 400 degrees C. In contrast, Y2O3/Ge deposited at 400 degrees C allows for an ultra-thin GeO2 layer at the interface, which can be eliminated during annealing at temperatures higher than 525 degrees C leaving a pristine YGeOx/Ge interface. The Y2O3/Ge gate stack deposited at lower temperature shows a sub-band gap absorption feature fitted to an Urbach tail of energy 1.1 eV. The latter correlates to a sub-stoichiometric germanium oxide layer at the interface. The optical band gap for the Y2O3/Ge stacks has been estimated to be 5.7 +/- 0.1 eV from Tauc-Lorentz modelling of VUV-VASE experimental data. For the optimal deposition temperature (400 degrees C), the Y2O3/Ge stack exhibits a higher conduction band offset (>2.3 eV) than the La2O3/Ge (similar to 2 eV), has a larger band gap (by about 0.3 eV), a germanium sub-oxide free interface, and leakage current (similar to 10(-7) A/cm(2) at 1V) five orders of magnitude lower than the respective La2O3/Ge stack. Our study strongly points to the superiority of the Y2O3/Ge system for germanium interface engineering to achieve high performance Ge Complementary Metal Oxide Semiconductor technology. (C) 2014 AIP Publishing LLC.
引用
收藏
页数:16
相关论文
共 50 条
  • [31] Multiple ablation resistance of La2O3/Y2O3-doped C/SiC-ZrC composites
    Luo, Lei
    Liu, Junpeng
    Duan, Liuyang
    Wang, Yiguang
    CERAMICS INTERNATIONAL, 2015, 41 (10) : 12878 - 12886
  • [32] Interaction between vacancies and the α-Fe/Y2O3 interface: A first-principles study
    Peng, Meng-Meng
    Lai, Wen-Sheng
    NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS, 2015, 352 : 67 - 71
  • [33] Effect of Y2O3 Supporter on the Catalytic Hydrogen Production from an Aqueous Formaldehyde Solution Catalyzed by Metal Cu Loaded on Y2O3
    Tian Yi
    Li Yuexiang
    Peng Shaoqin
    CHEMICAL JOURNAL OF CHINESE UNIVERSITIES-CHINESE, 2017, 38 (10): : 1841 - 1849
  • [34] Investigation on catalytic activity of CuO/La2O3, CuO/Gd2O3 and CuO/La2O3/Gd2O3 nanocatalysts prepared via novel two step approach
    Sankaran, A.
    Kumaraguru, K.
    Balraj, B.
    Sridevi, A.
    Magesh, R.
    MATERIALS SCIENCE AND ENGINEERING B-ADVANCED FUNCTIONAL SOLID-STATE MATERIALS, 2021, 263
  • [35] The diffusion of silicon atoms in stack structures of La2O3 and Al2O3
    Lee, W. J.
    Ma, J. W.
    Bae, J. M.
    Kim, C. Y.
    Jeong, K. S.
    Cho, M. -H.
    Chung, K. B.
    Kim, H.
    Cho, H. J.
    Kim, D. C.
    CURRENT APPLIED PHYSICS, 2013, 13 (04) : 633 - 639
  • [36] Temperature-dependent luminescence of intrinsic defects and excitons in nanocrystalline monoclinic Y2O3 films
    Kuznetsova, Yu A.
    Zatsepin, D. A.
    Zatsepin, A. F.
    Gavrilov, N. V.
    JOURNAL OF LUMINESCENCE, 2022, 250
  • [37] The effect of growth temperature on the irreversibility line of MPMG YBCO bulk with Y2O3 layer
    Kurnaz, Sedat
    Cakir, Bakiye
    Aydiner, Alev
    CRYOGENICS, 2017, 85 : 51 - 57
  • [38] Effect of pack aluminizing filler Y2O3 on aluminide coatings
    Zhao, YG
    Zhou, W
    Zhao, YQ
    Liang, YH
    Qin, QD
    RARE METAL MATERIALS AND ENGINEERING, 2005, 34 (10) : 1574 - 1577
  • [39] Deposition and post-deposition annealing of thin Y2O3 film on n-type Si in argon ambient
    Quah, Hock Jin
    Cheong, Kuan Yew
    MATERIALS CHEMISTRY AND PHYSICS, 2011, 130 (03) : 1007 - 1015
  • [40] The preparation and properties of Y2O3/AlN anti-reflection films on chemical vapor deposition diamond
    Yan, Feng
    Liu, Zhengtang
    Liu, Wenting
    THIN SOLID FILMS, 2011, 520 (02) : 734 - 738