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首页> 外文期刊>Journal of materials science >Temperature dependence of characteristic parameters of the Au/ C_(20)H_(12)-Si Schottky barrier diodes (SBDs) in the wide temperature range
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Temperature dependence of characteristic parameters of the Au/ C_(20)H_(12)-Si Schottky barrier diodes (SBDs) in the wide temperature range

机译:Au / C_(20)H_(12)/ n-Si肖特基势垒二极管(SBD)的特征参数在宽温度范围内的温度依赖性

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摘要

Au/C_(20)H_(12)-Si SBD was fabricated and its characteristic parameters such as reverse-saturation current (I_0), ideality factor (n), zero-bias barrier height (Φ_(bo)), series and shunt resistances (R_s, R_(sh)) were found as 1.974 x 10~(-7) A, 6.434, 0.351 eV, 30.22 Ω and 18.96 kΩ at 160 K and 1.061 x 10"6 A, 2.34, 0.836 eV, 5.82 Ω and 24.52 kΩ at 380 K, respectively. While the value of n decreases with increasing temperature, Φ_(bo) increases. The change in Φ_(bo) with temperature is not agreement with negative temperature coefficient of forbidden band-gap of semiconductor (Si). Thus, Φ_(bo) versus n, Φ_(bo) and (n~(-1) - 1) versus q/2kT plots were drawn to obtain an evidence of a Gaussian distribution (GD) of the BHs and all of them have a straight line. The mean value of BH (Φ_(bo)) was found as 0.983 eV from the intercept of Φ_(bo) versus n plot (for n = 1). Also, the value of Φ_(bo) and standard deviation (σ_s) were found as 1.123 eV and 0.151 V from the slope and intercept of Φ_(bo) versus q/2kT plot. By using the modified Richardson plot, the Φ_(bo) and Richardson constant (A*) values were obtained as 1.116 eV and 113.44 A cm~(-2) K~(-2) from the slope and intercept of this plot, respectively. It is clear that this value of A* (=113.44 A cm~(-2) K~(-2)) is very close to their theoretical value of 112 A cm~(-2) K~(-2) for n-Si. In addition, the energy density distribution profile of surface states (D_(it)) was obtained from the forward bias I-V data by taking into account the bias dependent of the effective barrier height (Φ_l) and ideality factor n(V) for four different temperatures (160, 200, 300, and 380 K). In conclusion, the I-V-T measurements of the Au/C_(20)H_(12)-Si SBD in the whole temperature range can be successfully explained on the basis of thermionic emission (TE) theory with GD of the BHs.
机译:制备了Au / C_(20)H_(12)/ n-Si SBD,其特征参数如反饱和电流(I_0),理想因子(n),零偏压势垒高度(Φ_(bo)),系列在160 K和1.061 x 10“ 6 A,2.34、0.836 eV时,分流电阻(R_s,R_(sh))为1.974 x 10〜(-7)A,6.434,0.351 eV,30.22Ω和18.96kΩ, 380 K时分别为5.82Ω和24.52kΩ,当n的值随温度升高而减小时,Φ_(bo)随温度的变化与半导体禁带隙的负温度系数不一致。因此,绘制了Φ_(bo)与n,Φ_(bo)和(n〜(-1)-1)与q / 2kT的关系图,以获得BH和BH的高斯分布(GD)的证据。它们都具有一条直线,从Φ_(bo)的截距与n图(对于n = 1)的截距中发现BH(Φ_(bo))的平均值为0.983 eV。 )和标准偏差(σ_s)从斜率和截距发现为1.123 eV和0.151 V Φ_(bo)与q / 2kT的关系图。通过使用改进的Richardson图,从该图的斜率和截距分别获得Φ_(bo)和Richardson常数(A *)值分别为1.116 eV和113.44 A cm〜(-2)K〜(-2)。 。显然,对于n,A *(= 113.44 A cm〜(-2)K〜(-2))的值非常接近其112 A cm〜(-2)K〜(-2)的理论值。 -Si此外,通过考虑与有效势垒高度(Φ_1)和理想因子n(V)有关的偏置,可以从前向偏置IV数据中获得表面状态(D_(it))的能量密度分布曲线温度(160、200、300和380 K)。总之,基于热离子发射(TE)理论和BHs的GD,可以成功地解释在整个温度范围内Au / C_(20)H_(12)/ n-Si SBD的I-V-T测量。

著录项

  • 来源
    《Journal of materials science 》 |2017年第5期| 3987-3996| 共10页
  • 作者单位

    Department of Physics, Faculty of Science, Gazi University, 06500 Ankara, Turkey;

    Department of Industrial Engineering, Faculty of Engineering, Baskent University, 06810 Ankara, Turkey;

    Department of Physics, Faculty of Sciences, Dumlupmar University, 43100 Kuetahya, Turkey;

    Department of Physics, Faculty of Science, Gazi University, 06500 Ankara, Turkey;

    Department of Physics, Faculty of Science, Gazi University, 06500 Ankara, Turkey;

  • 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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