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基于尺寸效应的Cu/CuNi薄膜热电偶灵敏度研究 总被引:1,自引:1,他引:0
采用磁控溅射法在镀有SiO2阻挡层的基底上制备了一系列的Cu/CuNi薄膜热电偶,其厚度分别为0.5,1.0,1.5和2.0 μm,测得四种Cu/CuNi薄膜热电偶的灵敏度,分别为46.47,45.23,44.32和43.98 μV/℃,通过实验和理论研究了薄膜热电偶灵敏度S与厚度δ之间的关系.结果表明:Cu/CuNi... 相似文献
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磁控溅射工艺参数对Cu薄膜电阻率的影响 总被引:1,自引:1,他引:0
在确定Cu薄膜临界尺寸的基础上,选定基底温度、靶基距、溅射功率和工作气压为影响因素设计正交试验,研究了磁控溅射制备工艺对Cu薄膜电阻率的影响。研究结果表明:基底温度是影响薄膜电阻率的最主要因素,电阻率随着基底温度的升高而减小;在工艺条件为基底温度200℃、靶基距45 mm、溅射功率100 W、工作气压0.5 Pa时,所制薄膜的电阻率将会达到最小。最后,结合薄膜微观形貌对试验结论进行了分析,并对最佳工艺条件进行了实验验证。 相似文献
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采用直流反应磁控溅射法在玻璃基底上用Zn(99.99%)掺杂Al(1.5%)靶制备出高质量的Al掺杂的ZnO(AZO)薄膜。用X射线光电子能谱仪对退火处理后的薄膜进行了成分和元素的价态分析,并用Van der Pauw方法对样品的电学特性进行了测量。实验结果表明,Zn和Al元素都以氧化态的形式存在,O元素主要是以晶格氧和吸附氧的形式存在。AZO薄膜的电学性质受退火温度和氧氩比的影响较大。随着退火温度的升高,电阻率减小,载流子浓度和迁移率增大。随着氧氩比的增大,电阻率增大,迁移率减小。因此可得到用直流反应磁控溅射法制备AZO薄膜的最佳氧氩比和退火温度分别为0.3/27和400℃,在此条件下制备出的薄膜电阻率可低至10-4Ω.cm,载流子浓度可达1020cm-3。 相似文献
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采用直流反应磁控溅射法在玻璃基底上用Zn(99.99%)掺杂Al(1.5%)靶制备出高质量的Al掺杂的ZnO(AZO)薄膜.用X射线光电子能谱仪对退火处理后的薄膜进行了成分和元素的价态分析,并用Van der Pauw方法对样品的电学特性进行了测量.实验结果表明,Zn和Al元素都以氧化态的形式存在,O元素主要是以晶格氧和吸附氧的形式存在.AZO薄膜的电学性质受退火温度和氧氩比的影响较大.随着退火温度的升高,电阻率减小,载流子浓度和迁移率增大.随着氧氩比的增大,电阻率增大,迁移率减小.因此可得到用直流反应磁控溅射法制备AZO薄膜的最佳氧氩比和退火温度分别为0.3/27和400 ℃,在此条件下制备出的薄膜电阻率可低至10-4 Ω·cm,载流子浓度可达1020 cm-3. 相似文献
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CoSiN薄膜可以作为超大规模集成电路Cu布线互连材料使用。利用磁控溅射技术制备了CoSiN/Cu/CoSiN/SiO2/Si薄膜,利用四探针测试仪、薄膜测厚仪、原子力显微镜、X射线光电子能谱仪等来检测多层膜电阻率、薄膜厚度、表面形貌、元素含量及价态等。考察亚45 nm级工艺条件下CoSiN薄膜对Cu的扩散阻挡性能。实验结果表明,在氩气气氛条件下经500℃,30 min热退火处理后多层膜的电阻率和成分没有发生明显变化,CoSiN薄膜能够保持良好的铜扩散阻挡性能;经600℃,30 min热退火处理后,Cu大量出现在表面,CoSiN薄膜对Cu失去扩散阻挡性能。 相似文献
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SnSb4.5CuNi/Cu焊点在175℃进行等温时效,分析了不同时效时间的SnSb4.5CuNi/Cu焊点中金属间化合物(IMC)组织形貌演变,通过纳米压痕法测量SnSb4.5CuNi/Cu焊点界面IMC的硬度和弹性模量,对焊接接头进行拉伸强度和低周疲劳测试。结果表明,时效48 h的焊缝中Cu6Sn5呈曲率半径均匀的半圆扇贝状特征,IMC的弹性模量与铜基板很接近,在恒幅对称应变条件下焊点的抗低周疲劳的性能最佳,焊点的抗拉强度高;当时效时间大于48 h,焊接接口的抗疲劳性能和抗拉伸强度逐渐变差。 相似文献
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T. M. Korhonen P. Su S. J. Hong M. A. Korhonen C. -Y. Li 《Journal of Electronic Materials》2000,29(10):1194-1199
We have done experimental research on the dissolution rate and intermetallic growth on Cu, Ni, and CuNi-alloy substrates as
a function of time and Cu/Ni ratio of the substrate. Reactions that occur when CuNi metallizations are soldered with lead-free
solders were investigated. The experiments were performed using Sn-3.5Ag and Sn-3.8Ag-0.7Cu solders and different CuNi alloys.
To determine the rate of dissolution of the substrate material into the solder, CuNi foils of different concentrations were
immersed in Sn-3.5Ag and Sn-3.8Ag-0.7Cu solder baths for soldering times ranging from 15 sec to 5 min at 250°C. In addition,
reflows of solder balls were made on top of bulk substrates to study the reaction when there is a practically infinite amount
of CuNi available compared to the amount of solder. Thin film experiments were also done, where Ni containing under bump metallizations
(UBMs) were fabricated and reflowed with eutectic SnAg solder balls. The nickel slows down the dissolution of the UBM into
the solder and the formation of intermetallics during reflow compared to Cu metallizations. The solder/UBM interfaces were
analyzed with SEM to find out how Ni concentration affects the reaction, and how much Ni is needed to obtain a sufficiently
slow reaction rate. 相似文献
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Cu diffusion onto an Ag-plated Cu leadframe surface was detected by Energy Dispersive X-ray (EDX) after de-capsulating the molded package. However, no Cu was detected by EDX on the Ag surfaces of bare leadframe, leadframe after die attachment including die attachment curing, or leadframe after wire bonding. Temperature simulation of molding and post-molding curing show that the temperature and its duration have some impact on the Cu diffusion, which is as expected. Interestingly, this study shows that the Cu diffusion onto the interface of the Ag-plated surface and mold compound is very much dependent on the type of mold compound used, which has never been reported in the literature so far. The Cu diffusion was detected by EDX only for certain types of mold compounds used. It is concluded that the mold compound is a major contributor to the Cu diffusion observed. This is possibly because S and O in the mold compound react with Cu and form copper sulfides and copper oxides, which accelerate the Cu diffusion from the Cu leadframe substrate onto the interface of the Ag surface and mold compound. 相似文献
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Interfacial Reactions in Cu/Ga and Cu/Ga/Cu Couples 总被引:1,自引:0,他引:1
Cu-to-Cu bonding to connect through-silicon vias in three-dimensional integrated-circuit packaging is the most important interconnection technology in the next-generation semiconductor industry. Soldering is an economic and fast process in comparison with diffusion bonding methods. Ga has high solubility of up to 20 at.% in the Cu-rich face-centered cubic (FCC) phase and high mobility at moderate temperatures. In this work, an attempt has been made to evaluate Ga-based Cu-to-Cu interconnection by transient liquid-phase (TLP) bonding. The Cu/Ga interfacial reactions at temperatures ranging from 160°C to 300°C were examined. For reactions at temperatures lower than 240°C, the reaction path is Cu/γ 3-Cu9Ga4/θ-CuGa2/liquid, where the γ 3-Cu9Ga4 and θ-CuGa2 phases are thin planar and thick scalloped layers, respectively, while for the reactions at 280°C and 300°C, the scalloped γ 3-Cu9Ga4 phase is the only reaction product. The phase transformation kinetics, reaction mechanisms, and microstructural evolution in the Cu/Ga couples are elaborated. In addition, reactions of Cu/Ga/Cu sandwich couples at 160°C were investigated. The original Cu/liquid/Cu couples isothermally transformed to Cu/γ 3-Cu9Ga4/ θ-CuGa2/γ 3-Cu9Ga4/Cu couples as the reaction progressed. However, cracks were observed in the θ-CuGa2 phase regions after metallographic processing. The brittle θ-CuGa2 phase is undesirable for Ga-based TLP bonding. 相似文献
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Hongqin Wang Hui Zhao Dusan P. Sekulic Yiyu Qian 《Journal of Electronic Materials》2008,37(10):1640-1647
Reactive wetting of solders on Cu and Cu6Sn5/Cu3Sn/Cu substrates was investigated using both (1) the wetting balance, and (2) the hot-stage real time, in situ visualization of the triple-line movement. To understand the phenomenology of the spreading behavior better, comprehensive
real-time in situ observations were performed. It was found that the wetting time during the wetting balance tests for both the lead solder
(63SnPb) and lead-free solder systems (Sn0.7Cu and Sn3.5Ag) is shorter on Cu substrates than it is on Cu6Sn5/Cu3Sn/Cu substrates. The wetting force was not remarkably different on these two substrates for the same solder system. The hot-stage
tests indicate a more pronounced spreading of 63Sn-Pb on Cu6Sn5/Cu3Sn/Cu substrates, along with a much larger spreading area. Spreading of lead-free solders in terms of the triple-line kinetics
studied by using the hot-stage visualization shows no significant difference in the spreading evolution either over Cu or
over Cu6Sn5/Cu3Sn/Cu substrates. 相似文献
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In this study, the different electromigration (EM) behaviors of eutectic Sn-Bi solder in the solid and molten states were
clarified using line-type Cu/Sn-Bi/Cu solder joints. When the eutectic Sn-Bi solder was in the solid state during the EM test,
a Bi-rich layer formed at the anode side while a Sn-rich band formed at the cathode side, and the intermetallic compound (IMC)
at the cathode side was thicker than that at the anode side. The growth of the Bi-rich layer exhibited a linear dependence
on the time of stressing. While the actual temperature of the solder joint increased to 140°C and the solder was in a molten
state or partially molten state, two separate Bi-rich layers formed at the anode side and a great many Cu6Sn5 IMC precipitates formed between the two Bi-rich layers. Also, the IMC layer at the cathode side was thinner than that at
the anode side. With a current-crowding-reduced structure, the products of diffusivity and effective charge number of Bi in
the eutectic Cu/Sn-Bi/Cu solder joints stressed with current density of 5 × 103 A/cm2 at 35°C, 55°C, and 75°C were calculated. 相似文献
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