温度梯度下Co-20%P/焊点界面金属间化合物的生长行为

Haotong Qin, Donghua Yang, Tao Fan, Tao Chen, Chunhong Zhang, Yuqian Chen
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As the loading time of the temperature gradient increased, the fine needle-shaped $\\mathbf{CoSn_{3}}$ near the Sn solder became plate-shaped CoSn3, and finally formed a bulk shape. Compared with ${2215^{\\mathrm{o}}\\mathrm{C}/\\text{cm}}$, the interfacial CoSn3 was relatively continuous and dense, because of the better combination of fine needle-shaped $\\mathbf{CoSn_{3}}$ and bulk-shaped CoSn3 under ${3260^{\\mathrm{o}}\\mathrm{C}/\\text{cm}}$, With the loading time increased, the growth of CoSn3 at the hot and cold ends of the solder joints interface showed obvious differences. Intuitively, the thickness of the cold end increases more rapidly than that of the hot end. After loading time of 400h under ${2215^{\\circ}\\mathrm{C}/\\text{cm}}$, the total thickness growth of CoSn3 was 18.10μm. After loading time of 400h under ${3260^{\\mathrm{o}}\\mathrm{C}/\\text{cm}}$, the total thickness growth of CoSn3 was 46.74μm. 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摘要

本文研究了Co-P/SAC105/Co-P焊点在${2215^{\circ}\ mathm {C}/\text{cm}}$和$\mathbf{3260^{\circ}\mathbf{C}/\mathbf{cm}}$温度梯度下界面IMC的生长行为。将P含量为20%的Co-P UBMs电镀在铜衬底上。采用回流焊工艺制备Co-p/SAC105/ Co-p焊点。BGA焊锡球为Sn-1.0wt.%Ag-0.5%Cu焊锡球,直径为${400\mu\ mathm {m}}$。将所得焊点进行以上两种温度梯度试验,加载时间分别为Oh、100h、200h和400h。发现Co-Sn-P层出现在Co-P膜和CoSn3层之间。随着温度梯度加载时间的增加,锡焊料附近细小的针状$\mathbf{CoSn_{3}}$变为片状CoSn3,最终形成块状。与${2215^{\ mathm {o}}}\ mathm {C}/\text{cm}}$相比,由于${3260^{\ mathm {o}}\ mathm {C}/\text{cm}}$下细针状的$\mathbf{CoSn_{3}}$和块状的CoSn3结合较好,界面CoSn3相对连续致密,随着加载时间的增加,焊点界面冷热端CoSn3的生长表现出明显的差异。直观地看,冷端的厚度比热端的厚度增加得更快。${2215^{\circ}\ mathm {C}/\text{cm}}$加载400h后,CoSn3的总厚度增长为18.10μm。${3260^{\ mathm {o}}\ mathm {C}/\text{cm}}$加载400h后,CoSn3的总厚度增长46.74μm。结果表明,在较大的温度梯度下,冷端和热端CoSn3的生长表现出更明显的不对称生长趋势,说明较大的温度梯度可以诱导界面CoSn3的生长。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Growth Behavior of Interfacial Intermetallic Compounds of Co-20%P/Solder Joint under Temperature Gradient
In this paper, the growth behavior of interfacial IMC of Co-P/SAC105/Co-P solder joints under the temperature gradients of ${2215^{\circ}\mathrm{C}/\text{cm}}$ and $\mathbf{3260^{\circ}\mathbf{C}/\mathbf{cm}}$ were studied. Co-P UBMs with 20% P content were electroplated on the copper substrates. Co-p/SAC105/Co-P solder joints were prepared by reflow welding process. BGA solder balls were Sn-1.0wt.%Ag-0.5%Cu solder balls with diameters of ${400\mu\mathrm{m}}$. The obtained solder joints were used to two above temperature gradients test, and the loading times were Oh, 100h, 200h and 400h, respectively. It found that the Co-Sn-P layer appeared between the Co-P film and the CoSn3 layer. As the loading time of the temperature gradient increased, the fine needle-shaped $\mathbf{CoSn_{3}}$ near the Sn solder became plate-shaped CoSn3, and finally formed a bulk shape. Compared with ${2215^{\mathrm{o}}\mathrm{C}/\text{cm}}$, the interfacial CoSn3 was relatively continuous and dense, because of the better combination of fine needle-shaped $\mathbf{CoSn_{3}}$ and bulk-shaped CoSn3 under ${3260^{\mathrm{o}}\mathrm{C}/\text{cm}}$, With the loading time increased, the growth of CoSn3 at the hot and cold ends of the solder joints interface showed obvious differences. Intuitively, the thickness of the cold end increases more rapidly than that of the hot end. After loading time of 400h under ${2215^{\circ}\mathrm{C}/\text{cm}}$, the total thickness growth of CoSn3 was 18.10μm. After loading time of 400h under ${3260^{\mathrm{o}}\mathrm{C}/\text{cm}}$, the total thickness growth of CoSn3 was 46.74μm. It showed that the growth of CoSn3 at the cold and hot ends shows the more significant asymmetric growth trend under a larger temperature gradient, revealing that the growth of interfacial CoSn3 could be induced by the larger temperature gradient.
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