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1.
A Si wafer was sequentially sputter-coated with Ti (20 nm), Cu (6 μm), Sn (4 μm), and In (4 μm). The specimen was then diffusion-soldered at temperatures between 150 and 300°C with an alumina substrate deposited with Cu (4 μm) and Au (6 μm). Experimental results showed that a multilayer of intermetallic phases with the compositions of (Cu0.99Au0.01)6(Sn0.52In0.48)5/(Au0.87Cu0.13)(In0.94Sn0.06)2/(Au0.98Cu0.02) (In0.95Sn0.05) formed at the Au/Cu interface. Kinetic analyses revealed that the growth of (Cu0.99Au0.01)6 (Sn0.52In0.48)5 and (Au0.87Cu0.13)(In0.94Sn0.06)2/(Au0.98Cu0.02)(In0.95Sn0.05) intermetallics were diffusion-controlled with activation energies of 21.5 and 31.3 kJ/mol, respectively. Sound tensile strengths of 42 and 48 kg/cm2 have been obtained under the bonding conditions of 150°C for 40 min. and 200°C for 30 min., respectively.  相似文献   

2.
The intermetallic compounds formed at the interfaces between In-49Sn solder balls and Au/Ni/Cu pads during the reflow of In-49Sn solder, ball-grid array (BGA) packages are investigated. Various temperature profiles with peak temperatures ranging from 140°C to 220°C and melting times ranging from 45 sec to 170 sec are plotted for the reflow processes. At peak temperatures below 170°C, a continuous double layer of intermetallics can be observed, showing a composition of Au(In,Ni)2/Au(In,Ni). Through selective etching of the In-49Sn solders, the intermetallic layer is made up of irregular coarse grains. In contrast, a number of cubic-shaped AuIn2 intermetallic compounds appear at the interfaces and migrate toward the upper domes of In-49Sn solder balls after reflow at peak temperatures above 200°C for longer melting times. The upward floating of the AuIn2 cubes can be explained by a thermomigration effect caused by the temperature gradient present in the liquid solder ball. The intermetallic compounds formed under various reflow conditions in this study exhibit different types of morphology, yet the ball shear strengths of the solder joints in the In-49Sn BGA packages remain unaffected.  相似文献   

3.
The interfacial reactions between liquid In-49Sn solder and Ni substrates at temperatures ranging from 150°C to 450°C for 15 min to 240 min have been investigated. The intermetallic compounds formed at the In-49Sn/Ni interfaces are identified to be a ternary Ni33In20Sn47 phase using electron-probe microanalysis (EPMA) and x-ray diffraction (XRD) analyses. These interfacial intermetallics grow with increasing reaction time by a diffusion-controlled mechanism. The activation energy calculated from the Arrhenius plot of reaction constants is 56.57 kJ/mol.  相似文献   

4.
The kinetics of the intermetallic layer formation at Sn-37wt.%Pb solder/Cu pad interface during reflow soldering were studied. The growth kinetics were analyzed theoretically by assuming that the mass flux of Cu through channels between scalloplike grains primarily contributes to the growth. Rate-controlling steps considered for the mass flux were the Cu dissolution from the bottom of the channels, diffusion through the channel, and the formation reaction of the intermetallic layer. These results indicated that a transition in the growth rate observed around 120–150 sec of reflow time may be associated with transition of the rate-controlling step from the Cu dissolution to the Cu diffusion through the channel.  相似文献   

5.
We have studied the microstructure of the Sn-9Zn/Cu joint in soldering at temperatures ranging from 230°C to 270°C to understand the growth of the mechanism of intermetallic compound (IMC) formation. At the interface between the Sn-9Zn solder and Cu, the results show a scallop-type ε-CuZn4 and a layer-type γ-Cu5Zn8, which grow at the interface between the Sn-9Zn solder and Cu. The activation energy of scallop-type ε-CuZn4 is 31 kJ/mol, and the growth is controlled by ripening. The activation energy of layer-type γ-Cu5Zn8 is 26 kJ/mol, and the growth is controlled by the diffusion of Cu and Zn. Furthermore, in the molten Sn-9Zn solder, the results show η-CuZn grains formed in the molten Sn-9Zn solder at 230°C. When the soldering temperature increases to 250°C and 270°C, the phase of IMCs is ε-CuZn4.  相似文献   

6.
The interfacial reaction between liquid In-49Sn solders and Ag substrates results in the formation of a thicker Ag2In intermetallic compound accompanied with the development of a thin AgIn2 layer. Through further aging of the In-49Sn/Ag soldered specimens at various temperatures ranging from room to 100°C, solid/solid trnasitions between Ag2In and AgIn2 intermetallic compounds can be observed. When the temperature drops below 75°C, Ag2In will react with the In-49Sn solder to form the dominant AgIn2 phase. Conversely, AgIn2 is consumed at a higher temperature (e.g., 100°C) when reacting with the Ag substrate to create a now dominant Ag2In phase. Lastly, the different mechanical, electrical, magnetic, and corrosion behaviors of both intermetallic compounds are respectively made known through direct measurements of the material properties of the individual Ag2In and AgIn2 bulk samples.  相似文献   

7.
The interfacial reactions between In49Sn solders and Ag thick films at temperatures ranging from 200°C to 350°C have been studied. The intermetallic compound formed at the Ag/In49Sn interface is Ag2In enveloped in a thin layer of AgIn2. Through the measurement of the thickness decrease of Ag thick films, it has been determined that the reaction kinetics of Ag2In has a linear relation to reaction time. Morphology observations indicated that the linear reaction of Ag2In was caused by the floating of Ag2In into the In49Sn solder as a result of the In49Sn solder penetrating into the porous Ag thick film. A sound joint can be obtained when a sufficient thickness of the Ag thick film (over 19.5 μm) reacts with the In49Sn solder. In this case, the tensile tested specimens fracture in the In49Sn matrix.  相似文献   

8.
Extensive microstructural and kinetic studies on the formation and growth of the intermetallics of Sn-rich solder/Cu couples have been reported. However, experimental data on the interdiffusion mechanisms during soldering reactions are limited and in conflict. The interdiffusion processes for soldering of Sn-3.5Ag alloy/Cu couples were investigated by using the Cr-evaporated surface as a reference line. At the beginning of soldering, Cu was observed to outdiffuse to the molten Sn−3.5Ag alloy until saturation, and the Sn−Ag solder dissolved with Cu collapsed below the reference line. As a result, the scallop-shaped Cu6Sn5 intermetallic compound was formed at the newly-formed Sn−Ag−Cu solder/Cu interface below the original Cu surface. When the soldered joint was reflowed at the lower temperature to suppress the Cu dissolution, the Cu6Sn5/Cu interface moved into the Cu substrate. Therefore, Sn is the dominant diffusing species for the intermetallic formation during the soldering process, although the extensive Cu dissolution occurs at the early stage of soldering.  相似文献   

9.
The formation and the growth of the intermetallic compound (IMC, hereafter) at the interface between the Sn-3.5Ag (numbers are all in wt.% unless otherwise specified) solder alloy and the Cu substrate were investigated. Solder joints were prepared by changing the soldering time at 250°C from 30 sec to 10 h and the morphological change of IMCs with soldering time was observed. It resulted from the competition between the growth of IMC and the dissolution of Cu from the substrate and IMCs. They were further aged at 130°C up to 800 h. During aging, the columnar morphology of IMCs changed to a more planar type while the scallop morphology remained unchanged. It was observed that the growth behavior of IMCs was closely related with the initial soldering condition.  相似文献   

10.
The growth of Cu-Sn intermetallic compounds (IMCs) at the molten Pb-Sn solder/Cu interface was studied over a range of temperatures and for a range of solder compositions. Strong peaks of and planes of η-phase (Cu6Sn5) were detected by x-ray diffraction when the Sn content was high. In the low Sn solder (27Sn-73Pb), the η-phase peaks were absent at the two high temperatures, but the (2 12 0) peak of the ε-phase (Cu3Sn) was prominent. A texture was detected in both layers in and (002) pole figures constructed for the η phase and ε phase, respectively. The growth directions were identified to be 〈101〉 and 〈102〉 for the η phase and 〈102〉 and 〈031〉 for the ε phase, normal to the Cu surface. The growth direction does not change with the morphology and the thickness of the IMC layer. The morphology of the η layer varied gradually from a cellular film with a rugged interface to a dense film with a scalloped interface as the Pb content, temperature, and reaction time increased. The ε layer was always dense and nearly planar.  相似文献   

11.
Phase field simulations of the microstructural evolution of the intermetallic compound (IMC) layer formed during isothermal soldering reactions between Sn-Cu solder alloys and a Cu substrate are presented. The simulation accounts for the fast grain boundary (GB) diffusion in the IMC layer, the concurrent IMC grain coarsening along with the IMC layer growth, and the dissolution of Cu from the substrate and IMC layer. The simulation results support the previous suggestions that the growth kinetics of the IMC layer during soldering is predominantly governed by the fast GB diffusion and the concurrent coarsening rate of the IMC grains. The IMC grain coarsening is initiated by a competitive growth of the IMC grains at the solder/IMC interface. It is also shown that the dissolution of Cu into an unsaturated solder reduces the coarsening rate of the IMC grains, consequently decreasing the temporal growth exponent of the IMC layer.  相似文献   

12.
The interfacial reactions and shear properties of In-48wt.%Sn/Au/Ni/Cu solder joints were investigated in terms of reflow conditions, i.e., reflow temperature and duration time. The thickness of an AuIn2 intermetallic compound (IMC) layer, formed at the solder/substrate interface, slightly increased with the duration time. The spalling of the AuIn2 intermetallics in the solder led to the formation of a Ni3(Sn,In)4 IMC layer between the solder and exposed Ni layer. The longer duration time resulted in the spalling and grain growth of Ni3(Sn,In)4 intermetallics. The higher reflow temperature accelerated the interfacial reactions between the solder and substrate. From the ball shear test results, the formation and growth of a continuous plate-shaped AuIn2 IMC layer increased the shear force of the solder joints, whereas the spalling and grain growth of cubic-shaped AuIn2 intermetallics significantly decreased the shear force. The formation and spalling of cubic-shaped Ni3(Sn,In)4 intermetallics increased the shear force, whereas the spalling and grain growth of polyhedron-shaped Ni3(Sn,In)4 intermetallics decreased the shear force. The crack propagated at the Au-rich/AuIn2/solder interface in the initial reflow stage, then toward the AuIn2 intermetallics dispersed in the solder matrix, and finally along the Ni3(Sn,In)4 intermetallics spalling off in the solder.  相似文献   

13.
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   

14.
The multilayer thin-film systems of Cu/Ti/Si and Au/Cu/Al2O3 were diffusion-soldered at temperatures between 250°C and 400°C by inserting a Sn thin-film interlayer. Experimental results showed that a double layer of intermetallic compounds (IMCs) η-(Cu0.99Au0.01)6Sn5/δ-(Au0.87Cu0.13)Sn was formed at the interface. Kinetics analyses revealed that the growth of intermetallics was diffusion-controlled. The activation energies as calculated from Arrhenius plots of the growth rate constants for (Cu0.99Au0.01)6Sn5 and (Au0.87Cu0.13)Sn are 16.9 kJ/mol and 53.7 kJ/mol, respectively. Finally, a satisfactory tensile strength of 132 kg/cm2 could be attained under the bonding condition of 300°C for 20 min.  相似文献   

15.
The morphology and growth kinetics of intermetallic compounds formed during the interfacial reactions between liquid Sn-20In-2.8Ag solder and Ni substrates are investigated. Energy-dispersive x-ray (EDX) analysis identifies the composition of the interfacial intermetallics as Ni3(In0.99In0.01)4. The soldering reactions at lower temperatures (225–275°C) result in the predominant formation of a homogeneous intermetallic layer whose growth is diffusion controlled. At higher soldering temperatures (300–350°C), the interfacial intermetallics appear to be long needlelike crystals, and the grooves in between the intermetallics provide fast-diffusion paths for Ni atoms to react with Sn atoms at the intermetallic front, which leads to interface-controlled growth kinetics. The intermetallic needles turned out to be flat slablike after selective etching of the unreacted solder. Kinetics analysis showed that they not only lengthened in the longitudinal direction, but also coarsened transversely by the Ostwald ripening mechanism.  相似文献   

16.
Intermetallic compound formation and morphology evolution in the 95Pb5Sn flip-chip solder joint with the Ti/Cu/Ni under bump metallization (UBM) during 350°C reflow for durations ranging from 50 sec to 1440 min were investigated. A thin intermetallic layer of only 0.4 μm thickness was formed at the 95Pb5Sn/UBM interface after reflow for 5 min. When the reflow was extended to 20 min, the intermetallic layer grew thicker and the phase identification revealed the intermetallic layer comprised two phases, (Ni,Cu)3Sn2 and (Ni,Cu)3Sn4. The detection of the Cu content in the intermetallic compounds indicated that the Cu atoms had diffused through the Ni layer and took part in the intermetallic compound formation. With increasing reflow time, the (Ni,Cu)3Sn4 phase grew at a faster rate than that of the (Ni,Cu)3Sn2 phase. Meanwhile, irregular growth of the (Ni,Cu)3Sn4 phase was observed and voids formed at the (Ni,Cu)3Sn2/Ni interface. After reflow for 60 min, the (Ni,Cu)3Sn2 phase disappeared and the (Ni,Cu)3Sn4 phase spalled off the NI layer in the form of a continuous layer. The gap between the (Ni,Cu)3Sn4 layer and the Ni layer was filled with lead. A possible mechanism for the growth, disappearance, and spalling of the intermetallic compounds at the 95Pb5Sn/UBM interface was proposed.  相似文献   

17.
After reflow of Sn-3.8Ag-0.7Cu and Sn-20In-2Ag-0.5Cu solder balls on Au/Ni surface finishes in ball grid array (BGA) packages, scallop-shaped intermetallic compounds (Cu0.70Ni0.28Au0.02)6Sn5 (IM1a) and (Cu0.76Ni0.24)6(Sn0.86In0.14)5 (IM1b), respectively, appear at the interfaces. Aging at 100°C and 150°C for Sn-3.8Ag-0.7Cu results in the formation of a new intermetallic phase (Cu0.70Ni0.14Au0.16)6Sn5 (IM2a) ahead of the former IM1a intermetallics. The growth of the newly appeared intermetallic compound, IM2a, is governed by a parabolic relation with an increase in aging time, with a slight diminution of the former IM1a intermetallics. After prolonged aging at 150°C, the IM2a intermetallics partially spall off and float into the solder matrix. Throughout the aging of Sn-20In-2Ag-.5Cu solder joints at 75°C and 115°C, partial spalling of the IM1b interfacial intermetallics induces a very slow increase in thickness. During aging at 115°C for 700 h through 1,000 h, the spalled IM1b intermetallics in the solder matrix migrate back to the interfaces and join with the IM1b interfacial intermetallics to react with the Ni layers of the Au/Ni surface finishes, resulting in the formation and rapid growth of a new (Ni0.85Cu0.15)(Sn0.71In0.29)2 intermetallic layer (IM2b). From ball shear tests, the strengths of the Sn-3.8Ag-0.7Cu and Sn-20In-2Ag-0.5Cu solder joints after reflow are ascertained to be 10.4 N and 5.4 N, respectively, which drop to lower values after aging. An erratum to this article is available at .  相似文献   

18.
After Sn-20In-0.8Cu solder balls are reflowed on a ball grid array (BGA) substrate (substrate A) with an Au/Ni surface finish, scallop-shaped intermetallic compounds with a composition of 0.83[Cu6(Sn0.87In0.13)5] + 0.17[Ni3(Sn0.87In0.13)4] are formed at the solder/pad interface. The distribution of the intermetallics is not altered by gravity or by multiple reflows of the solder joints. As another substrate (substrate B) is further attached onto the primary reflowed BGA assembly to form a sandwich structure subjected to subsequent multiple reflows, the Cu6(Sn0.87In0.13)5 interfacial intermetallic scallops remain still on the side of substrate A while many Au(In0.91Sn0.09)2 intermetallics of cubic shape appear near the solder/Ni interface on the side of substrate B. When the Sn-20In-0.8Cu solder balls are assembled simultaneously in between two substrates (A and B), Au(In0.91Sn0.09)2 intermetallic cubes of equal proportion are observed to form on both sides of the assembly. In summarizing the results, it is proposed that the diffusion of Cu atoms in the Sn-20In-0.8Cu solder toward the Ni layers after Au thin-film dissolution on Au/Ni surface finishes led to the formation of Cu6(Sn0.87Zn0.17)5 intermetallic compounds, which prevailed over the gravitational effect so that no intermetallic sedimentation in the liquid solder would occur. The appearance of Au(In0.91Sn0.09)2 at the Ni/Sn-20In-0.8Cu interfaces was hindered by the preferential formation of Cu6(Sn0.87Zn0.17)5 until the Cu atoms in the Sn-20In-0.8Cu solder matrix were consumed to a lower content via the attachment of a second substrate to the assembly.  相似文献   

19.
Isothermal solidification of conventional Cu/Sn diffusional couples was performed to form thin (30 μm) joints consisting of Cu-Sn intermetallics. During initial stages of isothermal solidification, both Cu6Sn5 and Cu3Sn phases grow, even though the former is the dominant. After consumption of all available Sn, the Cu3Sn phase grows reactively at the expense of Cu and Cu6Sn5. Finally, we obtain solder joints that consist of only Cu3Sn. Indentation fracture-toughness measurements show that Cu3Sn is superior to Cu6Sn5. Furthermore, indentations of Cu3Sn exhibit the presence of shear bands, which are not observed in Cu6Sn5, implying that the former is more ductile than the latter. Ductile intermetallic-based joints formed by isothermal solidification are promising candidates to form thin (as thin as 5–10 μm or less) solder joints, as they are thermally and thermodynamically stable compared to conventional solder joints. Excess copper in the interconnect provides ductility to the interconnect.  相似文献   

20.
The interfacial reactions between liquid In and Cu substrates at temperatures ranging from 175°C to 400°C are investigated for the applications in bonding recycled sputtering targets to their backing plates. Experimental results show that a scallop-shaped Cu16In9 intermetallic compound is found at the Cu/In interface after solder reactions at temperatures above 300°C. A double-layer structure of intermetallic compounds containing scallop-shaped Cu11In9 and continuous CuIn is observed after the Cu/In interfacial reaction at temperatures below 300°C. The growth of all these intermetallic compounds follows the parabolic law, which implies that the growth is diffusion-controlled. The activation energies for the growth of Cu16In9, Cu11In9, and CuIn intermetallic compounds calculated from the Arrhenius plot of growth reaction constants are 59.5, 16.9, and 23.5 kJ/mole, respectively.  相似文献   

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