共查询到17条相似文献,搜索用时 109 毫秒
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稀土相表面Sn晶须生长的研究 总被引:3,自引:3,他引:0
研究了Sn-3.8Ag-0.7Cu-RE(RE为Ce、Er或Y)焊料在空气中室温与高温时效过程中稀土相CeSn3、ErSn3与YSn3表面Sn晶须的生长情况。结果表明,Sn晶须的开始生长时间、形态及数量与稀土相的种类及时效条件有密切关系。稀土相因氧化产生的体积膨胀提供了Sn晶须生长的驱动力。稀土与氧的化学亲和力参数及时效温度共同影响稀土相表面Sn晶须的生长。室温实效条件下,三种稀土相表面Sn晶须的直径为0.1~2.0μm,长度可达几百微米;150℃时效条件下,Sn晶须的直径为0.1~0.2μm,长度也可达上百微米。 相似文献
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通过回流焊工艺制备了Sn0.7Cu-x Er/Cu(x=0,0.1,0.5)钎焊接头,研究钎焊温度及等温时效时间对接头的界面金属间化合物(IMC)的形成与生长行为的影响。结果表明:Sn0.7Cu钎料中微量稀土Er元素的添加,能有效抑制钎焊及时效过程中界面IMC的形成与生长。在等温时效处理过程中,随着时效时间的延长,界面反应IMC层不断增厚,在相同时效处理条件下,Sn0.7Cu0.5Er/Cu焊点界面IMC层的厚度略小于Sn0.7Cu0.1Er/Cu焊点界面的厚度。通过线性拟合方法,得到Sn0.7Cu0.1Er/Cu和Sn0.7Cu0.5Er/Cu焊点界面IMC层的生长速率常数分别为3.03×10–17 m2/s和2.67×10–17 m2/s。 相似文献
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采用SEM观察等手段研究了Sn58BixEr(x=0,0.1,0.5;表示添加质量分数0.01%,0.5%的Er)/Cu钎焊接头界面反应以及在120℃时效过程中金属间化合物(IMC)的生长行为。实验结果表明:Sn58BixEr/Cu钎焊接头IMC层厚度随着钎焊温度的升高而增厚,添加微量的Er能够有效抑制界面IMC的生长。在时效过程中,界面IMC层的厚度随着时效时间的增加而逐渐增厚。通过对实验数据进行拟合,得出120℃时效温度下Sn58Bi0.1Er/Cu和Sn58Bi0.5Er/Cu的IMC层的生长速率常数分别为3.42×10–16 m2/s和2.84×10–16 m2/s。 相似文献
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常用无铅钎料熔点的升高以及Sn含量的增加使得300系列不锈钢在使用几个月之后就会出现溶蚀现象。Fe-Sn金属间化合物的生长行为特点以及叶轮、喷嘴接触钎料的特点决定了材料表面的溶蚀形貌特征。 相似文献
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It has been discovered for the first time that Sn whiskers appeared in Sn3Ag0.5Cu0.5Ce solder joints of ball grid array (BGA)
packages after storage at room temperature (natural aging) for less than 3 days and they grew at a high rate of 2.9 ?/sec.
In one particular case, whiskers even formed after 1 day of storage at an extremely high growth rate of 8.6 ?/sec. Experimental
investigations showed that a number of CeSn3 clusters existed in the Sn3Ag0.5Cu0.5Ce solder matrix after the reflow process. Further natural aging in air for several
days caused the CeSn3 phases to oxidize rapidly, from which many Sn whiskers sprouted and grew to a length of hundreds of micrometers. The most
commonly observed whiskers have been long fiber-shaped ones of 0.1 μm to 0.3 μm in diameter (type I), while short whiskers
larger than 1 μm in diameter can also be found (type II). Here in our case, the surface oxide of the CeSn3 phase possessed a higher content of Ce than of Sn, which implied that a Ce-depleted region (nearly of pure Sn) was left beneath
the oxide layer. The abnormal whisker growth was attributed to the compressive stress squeezing the Sn atoms in the Ce-depleted
region of CeSn3 phase out of the oxide layer. 相似文献
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K. -W. Moon C. E. Johnson M. E. Williams O. Kongstein G. R. Stafford C. A. Handwerker W. J. Boettinger 《Journal of Electronic Materials》2005,34(9):L31-L33
Localized cracking of surface oxide has been proposed as a necessary step in the nucleation of Sn whiskers in Sn electrodeposited
films. To evaluate the effects of the oxide film on Sn whisker growth, a bright Sn-Cu electrodeposited film was inserted into
an ultrahigh vacuum Auger system, cleaned using an Ar− ion beam to remove the oxide film, and aged in the 2×10−9 Pa Auger system chamber. Whiskers and other features present during Ar+ ion cleaning left visible “shadows” on the surface. During aging in the ultrahigh vacuum system, new whiskers, identified
by the absence of the telltale shadows, nucleated and grew. Based on these observations, the presence or absence of an oxide
film has a minimal effect on Sn whisker nucleation and growth. 相似文献
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Equi-Axed Grain Formation in Electrodeposited Sn-Bi 总被引:1,自引:0,他引:1
E. Sandnes M.E. Williams M.D. Vaudin G.R. Stafford 《Journal of Electronic Materials》2008,37(4):490-497
Sn is widely used as a coating in the electronics industry because it provides excellent solderability, ductility, electrical
conductivity, and corrosion resistance. However, Sn whiskers have been observed to grow spontaneously from Sn electrodeposits
and are known to cause short circuits in fine-pitched pre-tinned electrical components. We report here a deposition strategy
that produces an equi-axed and size-tunable grain structure in Sn-Bi alloys electrodeposited from a commercial bright Sn electrolyte.
An equi-axed grain structure should allow a more uniform creep to relieve compressive stress with no localized surface disturbance.
The standard potential for Bi is about 0.45 V more positive than Sn. Pulsed deposition can selectively turn on and off the
Sn deposition reaction. During the off cycle, a displacement reaction between metallic Sn on the electrode surface and Bi3+ in solution selectively dissolves Sn and deposits Bi, effectively terminating the growth from the previous cycle and forcing
the Sn to nucleate a new grain on the Bi-enriched surface. The grain size is tunable by varying the pulsing conditions, and
an equi-axed structure can be obtained with as little as 3 at.% Bi. This surface enrichment of Bi by potential modulation
is similar to that which occurs naturally in Sn-Pb, and provides an avenue for breaking up the columnar grain structure inherent
to pure Sn, thus providing an additional diffusion path for Sn that may prevent whisker growth. 相似文献
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《Microelectronics Reliability》2014,54(11):2494-2500
The formation of intermetallic compound Cu6Sn5 gives rise to the internal stress in the lead-free coating, which causes the growth of Sn whiskers. This phenomenon is characterized with the expansion of inclusion in a plate perfectly bonded between two infinite solids. Based on the grain boundary diffusion mechanism, a model is established to evaluate the growth rate of Sn whiskers. The results show that the growth rate of whisker varies with the relative site between whisker and inclusion. When the distance between the whisker and inclusion exceeds a critical value, negative growth rate will appear, and it approaches zero as the distance increases. They explain some phenomena observed in experiments. 相似文献
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Whisker growth on surface treatment in the pure tin plating 总被引:2,自引:0,他引:2
Whisker behavior at various surface treatment conditions of pure Sn plating are presented. The temperature cycling test for
600 cycles and the ambient storage for 1 year was performed, respectively. From the temperature cycling test, bent-shaped
whiskers were observed on matte and semibright Sn plating, and flower-shaped whisker on bright Sn plating. The bright Sn plating
has smaller whiskers than the other types of Sn plating, and the whisker growth density per unit area is also lower than the
others. After 1 year under ambient storage, nodule growth of FeNi42 lead frame (LF) was observed in some parts. The Cu LF
showed about a 9.0 μm hillock-shaped whisker. This result demonstrated that the main determinant of whisker growth was the
number of temperature cycling (TC) in the FeNi42 LF, whereas it was the time and temperature in the Cu LF. Also, whisker growth
and shape varied with the type of surface treatment and grain size of plating. 相似文献
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Many possible mechanisms for whisker growth exist, each possible in various scenarios investigated in the literature. This
contribution addresses the importance of residual mechanical stress in a solder alloy for providing some of the energy necessary
to drive possible whisker growth. We investigate the indentations made on bulk lead-free solder (Sn3.5Ag) to introduce various
levels of residual energy associated with localized residual stresses. We confirm that localized residual stresses, in the
absence of a thin-film geometry, significant oxide thickness, and interdiffusional stresses from intermetallic Cu-Sn compounds,
do not result in the formation of whiskers in bulk Sn3.5Ag. Thus, the combination of stresses associated with thin films (either thermal misfit, plating, or chemical) and the oxidation of Sn at the surface
is likely required for continuous whisker growth. 相似文献
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Tin Whisker Growth Induced by High Electron Current Density 总被引:1,自引:0,他引:1
Y. W. Lin Yi-Shao Lai Y. L. Lin Chun-Te Tu C. R. Kao 《Journal of Electronic Materials》2008,37(1):17-22
The effect of electric current on the tin whisker growth on Sn stripes was studied. The Sn stripes, 1 μm in thickness, were patterned on silicon wafers. The design of the Sn stripes allowed the simultaneous study of the effect
of current crowding and current density. Current stressing was performed in ovens set at 30, 50, or 70°C, and the current
density used ranged from 4.5 × 104 A/cm2 to 3.6 × 105 A/cm2. It was found that the stress induced by the electric current caused the formation of many Sn whiskers. A higher current
density caused more Sn whiskers to form. Of the three temperatures studied, 50°C was the most favorable one for the formation
of the Sn whiskers. In addition, the current-crowding effect also influenced whisker growth. 相似文献