Abstract
Aging treatment was implemented for the Sn2·5Ag0·7Cu0·1RExNi/Cu solder joint under various temperatures simulating the service environment. The growing behaviour of the intermetallic compound at the soldering interface during aging was investigated. In the case of adding 0·1Ni aged solder joint, the maximum growth activation energies of (Cu,Ni)6Sn5 and Cu3Sn are 86·8 and 93·7 kJ mol−1 respectively. The results reveal that the growth of intermetallic compound in the soldering interface can be suppressed, and the solder joint can be strengthened by adding proper quantities of Ni in the solder.
Introduction
Pollution caused by Pb and Pb containing compounds in microelectronic devices has attracted much attention in academia and industry.1 Hence, it is necessary to develop environmentally friendly and highly reliable lead free solder.1,2 SnAgCu system lead free solder, which is considered as one of the most potential succedanea of SnPb solder, has been adopted now and is expected to be extensively used in the future due to its excellent comprehensive properties.2–4 The preceding studies reveal that adding 0·1 rare earth (RE) in the solder can enhance the physical properties and creep strength of SnAgCu solder alloys.5 In order to further improve the wettability, tensile strength and elongation of SnAgCuRE lead free solder, minor Ni has been added into the solder during manufacturing.6–8 As is well known, the formation of intermetallic compound (IMC) at the solder/substrate interface would affect the reliability of the solder joint. Especially, the sustained growth of IMC at the interface would degenerate the solder joint quality under service environment.9,10 Thus, understanding the growth characteristics of IMC at the interface of the solder joint during its service process is essential to restrain the growth of IMC so as to obtain a sound joint. However, few studies have been reported on the effect of Ni on IMC's growth characteristics at the solder/substrate interface during aging so far.
In the present study, to simulate the service environment, aging treatment was applied for the Sn2·5Ag0·7Cu0·1RExNi/Cu solder joint under different temperatures. The growing behaviour of IMC at the joining interface during aging was explored in order to provide some fundamental information for improving the reliability of the solder joint. Results indicate that adding appropriate Ni into Sn2·5Ag0·7Cu0·1RE solder can limit the growth of IMC at the interface of Sn2·5Ag0·7Cu0·1RExNi/Cu solder joint.
Experimental
The Sn2·5Ag0·7Cu0·1RExNi solder alloy was fabricated in a non-consumable melting furnace. Figure 1 shows the shape and dimension of solder joint; Fig. 1a shows the shape of the copper belt base metal. The flux was a water solution containing 22ZnCl2 and 2NH4Cl, with a soldering temperature of 270°C. The aging was achieved for the solder joint in the mediator of molybdenum disulphide to avoid the oxidation of the soldering seam surface, with temperatures of 80, 120 and 150°C. At each temperature, four aging times were considered, namely 50, 100, 200 and 500 h.

Dimensions of solder joint specimen
The solder joint was polished and etched with 4HNO3+1HCl+95 alcohol solution for 3 s. The microstructure and composition analysis were evaluated using scanning electron microscopy (SEM), energy dispersive spectroscopy (EDS) and X-ray diffraction (XRD). The thickness of the IMC layer was measured using AutoCAD. In order to observe the top view morphology of IMC, most of the solder on the specimens was first ground away, and then the specimens were etched with a solution made up of 13HNO3 and 87 alcohol under ultrasonic wave for 5 min to allow the remaining solder to dissolve. The average intercept length (L) of the IMC grain was measured according to the quantitative metallography theory11 to quantify the IMC grain dimension. The shear strength of the aged solder joint was tested under a crosshead velocity of 1 mm min−1 at room temperature.
Results and discussion
Interfacial IMC microstructure of solder joint during aging
Figure 2 presents the SEM images of cross-sectional micrographs of Sn2·5Ag0·7Cu0·1RExNi/Cu interfaces aged under various durations at 150°C. It can be seen from the graph that when the solder joint was not aged (aging time was 0), a reaction layer was observed in its interface. The reaction layer had a relatively flat front in the Cu matrix side and scallop type morphology in the solder bulk side. Figure 2 illustrates that the thickness of the reaction layer varied with the changes in Ni content in the solder (to be mentioned). Judging from the results of EDS and XRD, the reaction layer was mainly made up of Cu6Sn5 phase. As the Sn content in the solder alloys is >95, the interfacial reaction product should also be Cu6Sn5 according to the Cu–Sn phase diagram.12 In addition, the XRD analysis results confirmed that no sulphide was detected at the solder joint. The results show that the diffusion of molybdenum disulphide to the joint does not occur during aging. In the case of the aged solder joint, two reaction layers were discovered in the interface. Layer 1, beside Cu matrix, displayed a laminar appearance, whereas layer 2, close to solder bulk with light contrast, had a scallop type appearance. Like the joints without aging treatment, the thickness of reaction layers also varied with content changes of Ni in the solder. Figure 3a shows the results of XRD analysis obtained from the cross-section of the aged Sn2·5Ag0·7Cu0·1RE/Cu solder joint (500 h). As is shown in the graph, reaction layers formed at the interface were mainly comprised of Cu6Sn5 and Cu3Sn. Figure 3b and c shows the EDS results of layers 1 and 2 respectively. It can be seen that no Ni was detected in layer 1, and layer 2 only contains a small amount of Ni. Based on the XRD results, layer 1 was Cu3Sn, and layer 2 was (Cu,Ni)6Sn5, a solid solution based upon Cu6Sn5.13 As mentioned above, no Cu3Sn was detected at the interface of the solder joint without aging. It is likely that the driving force for Cu6Sn5 phase formation was higher than that of Cu3Sn based on thermodynamical consideration;14 therefore, the Cu6Sn5 formed at the initial stage of soldering. However, limited diffusion of Sn towards the Cu substrate via the intermetallic layer would result in the formation of Cu3Sn in the process of aging.

Cross-sectional micrographs of Sn2·5Ag0·7Cu0·1RExNi/Cu interfaces aged under various durations at 150°C

X-ray diffusion and EDS patterns of Sn2·5Ag0·7Cu0·1RExNi/Cu aged solder joint
Reaction layers that formed at the interface of aged Sn2·5Ag0·7Cu0·1RExNi/Cu solder joint exhibited the following characteristics in comparison with that of the solder joint without aging. First, the thickness of reaction layers rose with the increase in aging time. Second, the boundary between (Cu,Ni)6Sn5 layer and soldering seam was also made of irregularities orientated towards the soldering seam; however, these irregularities were found to decrease with the increase in aging time. In other words, the (Cu,Ni)6Sn5 morphology changed from rough scallop type to smooth planar type. This can be attributed to two reasons. One is the IMC grain growth, which results in large grains merging small grains. The other is the solution of top IMC (away from the interface) into solder bulk. Otherwise, some cracks could be seen in the IMC, which may be caused by high stress concentration existing in the thicker hard brittle IMC. Moreover, After 500 h of aging, the layer of (Cu,Ni)6Sn5 formed at the interface of the solder joint where 0·1Ni was added was thin. As the growth of IMC is mainly determined by the diffusion mechanism during aging, it was likely that the addition of Ni would somehow reduce the driving force for the diffusion of Sn and Cu through the intermetallic layer,12,15 decrease the diffusion rate of Sn and Cu and consequently suppress the growth of (Cu,Ni)6Sn5. The (Cu,Ni)6Sn5 layer could be over thick under the condition that excessive Ni was added, but the reason for it stays unclear. In addition, adding trace Ni to solder alloy could also suppress the growth of Cu3Sn during aging, and the inhibiting effect was especially obvious with a Ni concentration of 0·1. The formation of Cu3Sn is affected by the phase stability of Cu6Sn5 according to the reaction Cu6Sn5+9Cu→5Cu3Sn. The thermodynamic affinity in Cu6Sn5 is stronger between Ni and Sn than between Cu and Sn. Thus, the phase stability is greater for (Cu,Ni)6Sn5 than for Cu6Sn5.16 This finding suggests that the addition of Ni to the solder effectively suppresses the growth of Cu3Sn compounds.
Figures 4 and 5 show the top view morphology of (Cu,Ni)6Sn5 in the solder joint unaged and aged for 500 h. From Fig. 4, cobblestone type (Cu,Ni)6Sn5 grains with size of 3–4 μm were observed in the unaged solder joint. However, the (Cu,Ni)6Sn5 grains changed to polyhedron type and grew in size when aged for 500 h. The morphology transformation violates the law of thermodynamics. Though the reason for it is unclear, the result is interesting. Figure 6 represents the relationship between average intercept length of (Cu,Ni)6Sn5 grain and aging time. After being aged for 500 h, both the average intercept length and the number of edges of (Cu,Ni)6Sn5 grain dropped to the bottom. Both the average intercept length and the number of edges of (Cu,Ni)6Sn5 grain increased if excessive Ni was added. It can be concluded that adding proper quantities of Ni can suppress the growth of (Cu,Ni)6Sn5 during aging.

Top view morphology of (Cu,Ni)6Sn5 in solder joint without aging

Top view morphology of (Cu,Ni)6Sn5 in solder joint after aging for 500 h

Relationship of (Cu,Ni)6Sn5 grain average intercept length and aging time
Intermetallic compound growth kinetics
The growth of the IMC layer is a function of temperature and time (see equation (1))
Generally, the thickness of the IMC layer and the square root of aging time present a linear relationship, which can be seen from Figs. 7 and 8 as well. The gradient of the line is regarded as the IMC growth rate constant K. As shown in Figs. 7 and 8, the growth rate constant of (Cu,Ni)6Sn5 and Cu3Sn reached the minimum at all temperatures when 0·1Ni was added. The growth rate constant of Cu3Sn decreased but that of (Cu,Ni)6Sn5 increased when 0·5Ni was supplemented. Proper quantities of Ni in the solder can reduce the growth rate constant of (Cu,Ni)6Sn5 and Cu3Sn.

Relationship between (Cu,Ni)6Sn5 thickness and square root of aging time

Relationship between Cu3Sn thickness and square root of aging time
The Arrhenius relationship concerning the IMC growth rate constant during aging can be expressed by equation (2) (see Ref. 17)
Equation (3) can be deduced from equation (2)

Growth activation energy of (Cu,Ni)6Sn5 and Cu3Sn
Shear strength of aged solder joint
Figure 10 exhibits the influence of aging time on the shear strength of the solder joint at an aging temperature of 150°C. The curves could be divided into three stages. In the first stage, the shear strength decreased dramatically, and then in the second stage, the drop rate slowed; finally, the line flattened in the subsequent stage. The reason is that the growth rate of IMC differs at distinct aging times. Under the same aging time, the shear strength of the solder joint where 0·1Ni was added took the lead in comparison with that of the other two curves. Consequently, adding a certain amount of Ni during aging can increase the reliability of the solder joint, but the reinforcement effect could be weakened when excessive Ni is added.

Shear strength of Sn2·5Ag0·7Cu0·1RExNi/Cu solder joint aging at 150°C
Conclusions
The present study has examined the interfacial evolution and shear strength of Sn2·5Ag0·7Cu0·1RE xNi/Cu solder joints during aging. The main conclusions are listed as follows:
The thickness and morphology of the IMC layer formed at the soldering interface vary with the changes in aging time.
The growth of IMC in the soldering interface can be suppressed by adding proper quantities of Ni.
Adding certain amounts of Ni during aging can increase the reliability of the solder joint, but the reinforcement effect could be weakened when excessive Ni is added.
Footnotes
Acknowledgements
The present work was supported by the Foundation of Henan Province Outstanding Youth Scientist (grant no. 074100510011) and the Natural Science Foundation of China (grant no. 50774029).
