Engineering of band gap states of amorphous SiZnSnO semiconductor as a function of Si doping concentration

被引:45
作者
Choi, Jun Young [1 ]
Heo, Keun [1 ]
Cho, Kyung-Sang [2 ]
Hwang, Sung Woo [2 ]
Kim, Sangsig [1 ]
Lee, Sang Yeol [3 ]
机构
[1] Korea Univ, Dept Elect Engn, Seoul 136701, South Korea
[2] Samsung Adv Inst Technol, Device Lab, Suwon 443803, South Korea
[3] Cheongju Univ, Dept Semicond Engn, Cheongju 360764, South Korea
来源
SCIENTIFIC REPORTS | 2016年 / 6卷
基金
新加坡国家研究基金会;
关键词
ROOM-TEMPERATURE FABRICATION; THIN-FILM TRANSISTORS; WORK FUNCTION; ELECTRON-TRANSPORT; ATOMIC GEOMETRY; HIGH-MOBILITY; OXIDE; PERFORMANCE; STABILITY; SURFACES;
D O I
10.1038/srep36504
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
We investigated the band gap of SiZnSnO (SZTO) with different Si contents. Band gap engineering of SZTO is explained by the evolution of the electronic structure, such as changes in the band edge states and band gap. Using ultraviolet photoelectron spectroscopy (UPS), it was verified that Si atoms can modify the band gap of SZTO thin films. Carrier generation originating from oxygen vacancies can modify the band-gap states of oxide films with the addition of Si. Since it is not easy to directly derive changes in the band gap states of amorphous oxide semiconductors, no reports of the relationship between the Fermi energy level of oxide semiconductor and the device stability of oxide thin film transistors (TFTs) have been presented. The addition of Si can reduce the total density of trap states and change the band-gap properties. When 0.5 wt% Si was used to fabricate SZTO TFTs, they showed superior stability under negative bias temperature stress. We derived the band gap and Fermi energy level directly using data from UPS, Kelvin probe, and high-resolution electron energy loss spectroscopy analyses.
引用
收藏
页数:8
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共 44 条
  • [1] Toward High-Performance Amorphous GIZO TFTs
    Barquinha, P.
    Pereira, L.
    Goncalves, G.
    Martins, R.
    Fortunato, E.
    [J]. JOURNAL OF THE ELECTROCHEMICAL SOCIETY, 2009, 156 (03) : H161 - H168
  • [2] Crystalline In-Ga-Zn-O Density of States and Energy Band Structure Calculation Using Density Function Theory
    Chen, Charlene
    Cheng, Kai-Chen
    Chagarov, Evgeniy
    Kanicki, Jerzy
    [J]. JAPANESE JOURNAL OF APPLIED PHYSICS, 2011, 50 (09)
  • [3] Indirect band gap of light-emitting BC2N
    Chen, Y
    Barnard, JC
    Palmer, RE
    Watanabe, MO
    Sasaki, T
    [J]. PHYSICAL REVIEW LETTERS, 1999, 83 (12) : 2406 - 2408
  • [4] High-Performance a-IGZO Thin-Film Transistor Using Ta2O5 Gate Dielectric
    Chiu, C. J.
    Chang, S. P.
    Chang, S. J.
    [J]. IEEE ELECTRON DEVICE LETTERS, 2010, 31 (11) : 1245 - 1247
  • [5] Effect of hafnium addition on Zn-Sn-O thin film transistors fabricated by solution process
    Choi, Jun Young
    Kim, Sang Sig
    Lee, Sang Yeol
    [J]. APPLIED PHYSICS LETTERS, 2012, 100 (02)
  • [6] First-principle study of amorphous SiZnSnO thin-film transistor with excellent stability
    Chong, Eugene
    Kang, Iljoon
    Park, Chul Hong
    Lee, Sang Yeol
    [J]. THIN SOLID FILMS, 2013, 534 : 609 - 613
  • [7] Role of silicon in silicon-indium-zinc-oxide thin-film transistor
    Chong, Eugene
    Kim, Seung Han
    Lee, Sang Yeol
    [J]. APPLIED PHYSICS LETTERS, 2010, 97 (25)
  • [8] Transparent thin-film transistors with zinc indium oxide channel layer
    Dehuff, NL
    Kettenring, ES
    Hong, D
    Chiang, HQ
    Wager, JF
    Hoffman, RL
    Park, CH
    Keszler, DA
    [J]. JOURNAL OF APPLIED PHYSICS, 2005, 97 (06)
  • [9] CALCULATION OF LOW-ENERGY-ELECTRON-DIFFRACTION INTENSITIES FROM ZNO (1010) .2. INFLUENCE OF CALCULATIONAL PROCEDURE, MODEL POTENTIAL, AND 2ND-LAYER STRUCTURAL DISTORTIONS
    DUKE, CB
    MEYER, RJ
    PATON, A
    MARK, P
    [J]. PHYSICAL REVIEW B, 1978, 18 (08): : 4225 - 4240
  • [10] ATOMIC GEOMETRY OF CLEAVAGE SURFACES OF TETRAHEDRALLY COORDINATED COMPOUND SEMICONDUCTORS
    DUKE, CB
    LUBINSKY, AR
    LEE, BW
    MARK, P
    [J]. JOURNAL OF VACUUM SCIENCE & TECHNOLOGY, 1976, 13 (04): : 761 - 768