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CONDUCTION MECHANISMS IN THICK FILM RESISTORS.

机译:厚膜电阻的传导机制。

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The work reported here has focused on the influence of substrate dissolution during the high temperature firing on the electrical properties of ruthenium dioxide-lead borosilicate thick film resistors. A resistor 25 (mu)m thick that is fired for 10 minutes at 840(DEGREES)C will dissolve 4 (mu)m of the substrate surface. The presence of the alumina in the glass phase retards the growth of the resistor microstructure or chains of conducting particles by increasing the glass viscosity and slightly decreasing the solubility of RuO(,2). These physical changes brought about measurable changes in the electrical properties.; Four glasses were made: a standard glass with 63 w/o PbO:25 w/o B(,2)O(,3):12 w/o SiO(,2); 4 w/o 614 AlSiMag substrate and 96 w/o standard glass; 6 w/o substrate and 94 w/o standard glass; 10 w/o substrate and 90 w/o standard glass. These glasses were powdered and mixed with 5 w/o RuO(,2) powder then blended with screening agents. Four terminal resistors were fired onto 614 AlSiMag substrates under various conditions of time and temperature. The sheet resistance, hot (+ 125(DEGREES)C) and cold (-55(DEGREES)C) temperature coefficients of resistance, normalized resistance versus temperature (-55 to +125(DEGREES)C), and noise index were measured. As predicted, resistors with increasing amounts of substrate in the glass phase demonstrated slower development of electrical properties. It took about 14 minutes at 800(DEGREES)C for a 10 w/o substrate resistor to reach its minimum sheet resistance compared to only 8 minutes for the standard glass resistor.; The hot and cold TCR's increased from large negative values (< -400 ppm/(DEGREES)C) for short firing times or low firing temperatures to near-zero values at longer firing times or higher firing temperatures. The noise index, in general, decreased with increasing firing time or temperature from about 40 dB down to 5 dB. With increasing weight percent substrate, the noise index increased.; A second group of experiments was performed to determine conduction mechanisms in thin films of the standard and 10 w/o substrate glasses. The glass was rf sputtered onto gold-coated, oxidized silicon wafers, then counter-electrodes of gold were evaporated on these films. Both ac and dc measurements were made. The parallel capacitance was a slowly decreasing function of frequency from 10('2) to 10('5) Hz. The conductivity increased linearly with frequency while the dissipation factor often showed a broad maximum implying the presence of an ionic impurity relaxation. The dielectric constants were found to be 11.5 and 11.2 for the standard and 10 w/o substrate glasses, respectively. The dielectric breakdown voltages were 2.6 x 10('6) V/cm for the standard glass and 5.5 x 10('6) V/cm for the 10 w/o substrate glass. The dc measurements indicate the conduction mechanism in the glass films is Schottky emission with an activation energy of approximately 0.38 eV.; Using the normalized resistance versus temperature data for the thick film resistors, a unit model consisting of sintered particles of RuO(,2) and non-sintered contacts with RuO(,2) particles separated by a thin layer of the glass phase has been proposed. The temperature dependence of the theoretical unit has been derived and related to the experimental data by a curve-fitting process.
机译:此处报道的工作集中在高温烧成过程中基材溶解对二氧化钌-硼硅酸铅厚膜电阻器电性能的影响上。 25微米厚的电阻器在840°C下烧制10分钟,将溶解4微米的基板表面。玻璃相中氧化铝的存在通过增加玻璃粘度并略微降低RuO(,2)的溶解性而阻碍了电阻器微结构或导电颗粒链的生长。这些物理变化导致电性能的可测量变化。制作了四块玻璃:标准玻璃,其中PbO:63 w / o B(2)O(25)O(3):SiO(12)w / o:12 w / o 4 w / o 614 AlSiMag基板和96 w / o标准玻璃; 6 w / o基板和94 w / o标准玻璃; 10 w / o基板和90 w / o标准玻璃。将这些玻璃粉化并与5 w / o RuO(,2)粉末混合,然后与屏蔽剂混合。在各种时间和温度条件下,将四个终端电阻烧制到614 AlSiMag基板上。测量了薄层电阻,电阻的热(+ 125(DEGREES)C)和冷(-55(DEGREES)C)温度系数,归一化电阻与温度的关系(-55至+125(DEGREES)C)和噪声指数。如所预测的,在玻璃相中具有增加的衬底量的电阻器显示出电性能的发展较慢。一个10 w / o的衬底电阻在800°C的温度下大约要花14分钟,而标准玻璃电阻只有8分钟。冷热TCR从较短的点火时间或较低的点火温度的大负值(<-400 ppm /(DEGREES)C)增加到较长的点火时间或较高的点火温度时的接近零值。通常,噪声指数随着发射时间或发射时间的增加而降低,从大约40 dB降低到5 dB。随着基质重量百分比的增加,噪声指数增加。进行第二组实验,以确定标准玻璃和10 w / o衬底玻璃的薄膜中的传导机制。将玻璃射频溅射到镀金的氧化硅晶片上,然后将金的反电极蒸发在这些膜上。进行了交流和直流测量。并联电容是频率从10('2)到10('5)Hz的缓慢下降函数。电导率随频率线性增加,而耗散因数通常显示出很大的最大值,这意味着存在离子杂质弛豫。发现标准玻璃和10 w / o基板玻璃的介电常数分别为11.5和11.2。对于标准玻璃,介电击穿电压为2.6 x 10('6)V / cm,对于10 w / o的基底玻璃为5.5 x 10('6)V / cm。直流测量表明,玻璃膜中的传导机制是肖特基发射,其活化能约为0.38 eV。利用厚膜电阻器的归一化电阻与温度数据,提出了一个单元模型,该模型由RuO(,2)的烧结颗粒和通过玻璃相薄层隔开的RuO(,2)颗粒的非烧结接触组成。通过曲线拟合过程得出了理论单位的温度依赖性,并将其与实验数据相关联。

著录项

  • 作者

    HIMELICK, JAMES MAX.;

  • 作者单位

    Purdue University.;

  • 授予单位 Purdue University.;
  • 学科 Engineering Materials Science.
  • 学位 Ph.D.
  • 年度 1980
  • 页码 204 p.
  • 总页数 204
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 工程材料学;
  • 关键词

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