搜索

x

留言板

尊敬的读者、作者、审稿人, 关于本刊的投稿、审稿、编辑和出版的任何问题, 您可以本页添加留言。我们将尽快给您答复。谢谢您的支持!

姓名
邮箱
手机号码
标题
留言内容
验证码

退火温度和Ga含量对溶液法制备InGaZnO薄膜晶体管性能的影响

张世玉 喻志农 程锦 吴德龙 栗旭阳 薛唯

引用本文:
Citation:

退火温度和Ga含量对溶液法制备InGaZnO薄膜晶体管性能的影响

张世玉, 喻志农, 程锦, 吴德龙, 栗旭阳, 薛唯

Effects of annealing temperature and Ga content on properties of solution-processed InGaZnO thin film

Zhang Shi-Yu, Yu Zhi-Nong, Cheng Jin, Wu De-Long, Li Xu-Yang, Xue Wei
PDF
导出引用
  • 采用溶液法在玻璃衬底上制备InGaZnO薄膜, 并以InGaZnO为沟道层制备底栅顶接触型薄膜晶体管, 研究了退火温度和Ga含量对InGaZnO薄膜和晶体管电学性能的影响. 研究表明, 退火可以明显改善溶液法制备InGaZnO薄膜晶体管的电学性能. 退火温度的升高会导致薄膜晶体管阈值电压的负向漂移, 并且饱和迁移率和电流开关比增大. X射线光电子能谱测量表明, 随退火温度的增加, InGaZnO薄膜表面吸附氧减少, 沟道层中氧空位增多导致电子浓度增大. 退火温度为380 ℃时, 晶体管获得最佳性能. 饱和迁移率随Ga含量的增加而减小. In:Ga:Zn 摩尔比为5:1.3:2时, 晶体管达到最佳性能: 饱和迁移率为0.43 cm2/(Vs), 阈值电压为1.22 V, 开关电流比为4.7104, 亚阈值摆幅为0.78 V/decade.
    Oxide thin film transistor with an oxide channel layer is investigated to cater to the requirements of transparent electronics for the high mobility, good uniformity, and large band gap. Owing to its special conduction mechanism, high carrier mobility can be realized even in the amorphous phase. Oxide-based thin films have been prepared by using a number of methods, such as pulsed laser deposition, chemical vapor deposition, radio-frequency sputtering and solution-derived process. Solution processing is commonly used in TFT applications because of its simplicity and potential application in printed device fabrication. In the solution process, the conductivity of multicomponent oxide films can be controlled by incorporating charge-controlling cations. In this paper, bottom-gat topcontact thin film transistors are fabricated by using solution processed InGaZnO channel layers. The effects of annealing temperature and Ga content on the properties of thin film transistor are examined. Optical transmittance of InGaZnO thin film is greater than 80% in the visible region. Electrical characteristics of InGaZnO thin film transistor are improved by increasing annealing temperature. The threshold voltage of solution-processed InGaZnO transistor decreases from 6.74 to -0.62 V with annealing temperature increasing from 250 to 400 ℃, owing to the increase in electron concentration in the active layer. A lower annealing temperature suppresses the generation of carriers outside of the control of Ga cations. X-ray photoelectron spectrum measurement shows that the electron concentration increases because oxygen vacancies generate electrons. The incorporation of Ga into a InZnO compound system results in reducing the carrier concentration of the film and an off-current of thin film transistor. As the Ga ratio is increased at an identical In and Zn content, the carrier concentration of the film decreases and the threshold voltage of thin film transistor shifts towards the positive direction. As the content of Ga is increased in the oxide active layer of transistor, the subthreshold amplitude decreases, and the on/off ratio is improved. This is a consequence of the Ga ions forming strong chemical bonds with oxygen as compared with the Zn and In ions, acting as a carrier suppressor. The performances of thin film transistor with an atomic ratio of In: Ga: Zn=5:1.3:2 are optimized as follows: saturation mobility of 0.43 cm2/(Vs), threshold voltage of -1.22 V, on/off current ratio of 4.7104, subthreshold amplitude of 0.78 V/decade.
      通信作者: 喻志农, znyu@bit.edu.cn
    • 基金项目: 国家重点基础研究发展计划(批准号: 2014CB643600)资助的课题.
      Corresponding author: Yu Zhi-Nong, znyu@bit.edu.cn
    • Funds: Project supported by the National Basic Research Program of China (Grant No. 2014CB643600).
    [1]

    Hoffman R L, Norris B J, Wager J F 2003 Appl. Phys. Lett. 82 733

    [2]

    Wager J F 2003 Science 300 1245

    [3]

    Hosono H, Yasukawa M, Kawazoe H 1996 J. Non-Cryst. Solids 203 334

    [4]

    Choi H S, Jeon S, Kim H, Shin J, Kim C, Chung U I 2012 Appl. Phys. Lett. 100 173501

    [5]

    Choi W S 2012 Electron. Mater. Lett. 8 87

    [6]

    Sangwook K, Jae Chul P, Dae Hwan K, Jang-Sik L 2013 Jpn. J. Appl. Phys. 52 041701

    [7]

    Li X F, Xin E L, Shi J F, Chen L L, Li C Y, Zhang J H 2013 Acta Phys. Sin. 62 108503 (in Chinese) [李喜峰, 信恩龙, 石继锋, 陈龙龙, 李春亚, 张建华 2013 62 108503]

    [8]

    Lee S Y, Kim D H, Chong E, Jeon Y W, Kim D H 2011 Appl. Phys. Lett. 98 122105

    [9]

    Liu K H, Chang T C, Wu M S, Hung Y S, Hung P H, Hsieh T Y, Chou W C, Chu A K, Sze S M, Yeh B L 2014 Appl. Phys. Lett. 104 133503

    [10]

    Nomura K, Ohta H, Ueda K, Kamiya T, Hirano M, Hosono H 2003 Science 300 1269

    [11]

    Kim G H, Shin H S, Ahn B D, Kim K H, Park W J, Kim H J 2009 J. Electrochem. Soc. 156 H7

    [12]

    Kamiya T, Nomura K, Hosono H 2010 Phys. Status Solidi A 207 1698

    [13]

    Fan J C C, Goodenough J B 1977 J. Appl. Phys. 48 3524

    [14]

    Kumar B, Gong H, Akkipeddi R 2005 J. Appl. Phys. 97 063706

    [15]

    Ahn B D, Shin H S, Kim G H, Park J S, Kim H J 2009 Jpn. J. Appl. Phys. 48 03B019

    [16]

    Takechi K, Nakata M, Eguchi T, Yamaguchi H, Kaneko S 2009 Jpn. J. Appl. Phys. 48 011301

    [17]

    Kim D, Koo C Y, Song K, Jeong Y, Moon J 2009 Appl. Phys. Lett. 95 103501

    [18]

    Choi J H, Hwang S M, Lee C M, Kim J C, Park G C, Joo J, Lim J H 2011 J. Cryst. Growth 326 175

  • [1]

    Hoffman R L, Norris B J, Wager J F 2003 Appl. Phys. Lett. 82 733

    [2]

    Wager J F 2003 Science 300 1245

    [3]

    Hosono H, Yasukawa M, Kawazoe H 1996 J. Non-Cryst. Solids 203 334

    [4]

    Choi H S, Jeon S, Kim H, Shin J, Kim C, Chung U I 2012 Appl. Phys. Lett. 100 173501

    [5]

    Choi W S 2012 Electron. Mater. Lett. 8 87

    [6]

    Sangwook K, Jae Chul P, Dae Hwan K, Jang-Sik L 2013 Jpn. J. Appl. Phys. 52 041701

    [7]

    Li X F, Xin E L, Shi J F, Chen L L, Li C Y, Zhang J H 2013 Acta Phys. Sin. 62 108503 (in Chinese) [李喜峰, 信恩龙, 石继锋, 陈龙龙, 李春亚, 张建华 2013 62 108503]

    [8]

    Lee S Y, Kim D H, Chong E, Jeon Y W, Kim D H 2011 Appl. Phys. Lett. 98 122105

    [9]

    Liu K H, Chang T C, Wu M S, Hung Y S, Hung P H, Hsieh T Y, Chou W C, Chu A K, Sze S M, Yeh B L 2014 Appl. Phys. Lett. 104 133503

    [10]

    Nomura K, Ohta H, Ueda K, Kamiya T, Hirano M, Hosono H 2003 Science 300 1269

    [11]

    Kim G H, Shin H S, Ahn B D, Kim K H, Park W J, Kim H J 2009 J. Electrochem. Soc. 156 H7

    [12]

    Kamiya T, Nomura K, Hosono H 2010 Phys. Status Solidi A 207 1698

    [13]

    Fan J C C, Goodenough J B 1977 J. Appl. Phys. 48 3524

    [14]

    Kumar B, Gong H, Akkipeddi R 2005 J. Appl. Phys. 97 063706

    [15]

    Ahn B D, Shin H S, Kim G H, Park J S, Kim H J 2009 Jpn. J. Appl. Phys. 48 03B019

    [16]

    Takechi K, Nakata M, Eguchi T, Yamaguchi H, Kaneko S 2009 Jpn. J. Appl. Phys. 48 011301

    [17]

    Kim D, Koo C Y, Song K, Jeong Y, Moon J 2009 Appl. Phys. Lett. 95 103501

    [18]

    Choi J H, Hwang S M, Lee C M, Kim J C, Park G C, Joo J, Lim J H 2011 J. Cryst. Growth 326 175

  • [1] 张雪, KimBokyung, LeeHyeonju, ParkJaehoon. 低温快速制备基于溶液工艺的高性能氧化铟薄膜及晶体管.  , 2024, 73(9): 096802. doi: 10.7498/aps.73.20240082
    [2] 况丹, 徐爽, 史大为, 郭建, 喻志农. 基于铝纳米颗粒修饰的非晶氧化镓薄膜日盲紫外探测器.  , 2023, 72(3): 038501. doi: 10.7498/aps.72.20221476
    [3] 荆斌, 徐萌, 彭聪, 陈龙龙, 张建华, 李喜峰. 高负偏光照稳定性的溶液法像素级IZTO TFT.  , 2022, 71(13): 138502. doi: 10.7498/aps.71.20220154
    [4] 邓小庆, 邓联文, 何伊妮, 廖聪维, 黄生祥, 罗衡. InGaZnO薄膜晶体管泄漏电流模型.  , 2019, 68(5): 057302. doi: 10.7498/aps.68.20182088
    [5] 覃婷, 黄生祥, 廖聪维, 于天宝, 罗衡, 刘胜, 邓联文. 铟镓锌氧薄膜晶体管的悬浮栅效应研究.  , 2018, 67(4): 047302. doi: 10.7498/aps.67.20172325
    [6] 覃婷, 黄生祥, 廖聪维, 于天宝, 邓联文. 同步对称双栅InGaZnO薄膜晶体管电势模型研究.  , 2017, 66(9): 097101. doi: 10.7498/aps.66.097101
    [7] 兰林锋, 张鹏, 彭俊彪. 氧化物薄膜晶体管研究进展.  , 2016, 65(12): 128504. doi: 10.7498/aps.65.128504
    [8] 徐飘荣, 强蕾, 姚若河. 一个非晶InGaZnO薄膜晶体管线性区陷阱态的提取方法.  , 2015, 64(13): 137101. doi: 10.7498/aps.64.137101
    [9] 谭再上, 吴小蒙, 范仲勇, 丁士进. 热退火对等离子体增强化学气相沉积SiCOH薄膜结构与性能的影响.  , 2015, 64(10): 107701. doi: 10.7498/aps.64.107701
    [10] 徐华, 兰林锋, 李民, 罗东向, 肖鹏, 林振国, 宁洪龙, 彭俊彪. 源漏电极的制备对氧化物薄膜晶体管性能的影响.  , 2014, 63(3): 038501. doi: 10.7498/aps.63.038501
    [11] 张耕铭, 郭立强, 赵孔胜, 颜钟惠. 氧对IZO低压无结薄膜晶体管稳定性的影响.  , 2013, 62(13): 137201. doi: 10.7498/aps.62.137201
    [12] 李喜峰, 信恩龙, 石继锋, 陈龙龙, 李春亚, 张建华. 低温透明非晶IGZO薄膜晶体管的光照稳定性.  , 2013, 62(10): 108503. doi: 10.7498/aps.62.108503
    [13] 吴萍, 张杰, 李喜峰, 陈凌翔, 汪雷, 吕建国. 室温生长ZnO薄膜晶体管的紫外响应特性.  , 2013, 62(1): 018101. doi: 10.7498/aps.62.018101
    [14] 陈晓雪, 姚若河. 基于表面势的氢化非晶硅薄膜晶体管直流特性研究.  , 2012, 61(23): 237104. doi: 10.7498/aps.61.237104
    [15] 赵孔胜, 轩瑞杰, 韩笑, 张耕铭. 基于氧化铟锡的无结低电压薄膜晶体管.  , 2012, 61(19): 197201. doi: 10.7498/aps.61.197201
    [16] 强蕾, 姚若河. 非晶硅薄膜晶体管沟道中阈值电压及温度的分布.  , 2012, 61(8): 087303. doi: 10.7498/aps.61.087303
    [17] 王雄, 才玺坤, 原子健, 朱夏明, 邱东江, 吴惠桢. 氧化锌锡薄膜晶体管的研究.  , 2011, 60(3): 037305. doi: 10.7498/aps.60.037305
    [18] 徐天宁, 吴惠桢, 张莹莹, 王雄, 朱夏明, 原子健. In2O3 透明薄膜晶体管的制备及其电学性能的研究.  , 2010, 59(7): 5018-5022. doi: 10.7498/aps.59.5018
    [19] 罗翀, 孟志国, 王烁, 熊绍珍. 溶液法铝诱导晶化制备多晶硅薄膜.  , 2009, 58(9): 6560-6565. doi: 10.7498/aps.58.6560
    [20] 辛煜, 宁兆元, 程珊华, 陆新华, 甘肇强, 黄松. ECR-CVD法制备的a-C:F:H薄膜在N2气氛中的热退火研究.  , 2002, 51(2): 439-443. doi: 10.7498/aps.51.439
计量
  • 文章访问数:  6637
  • PDF下载量:  208
  • 被引次数: 0
出版历程
  • 收稿日期:  2016-01-20
  • 修回日期:  2016-03-22
  • 刊出日期:  2016-06-05

/

返回文章
返回
Baidu
map