电迁移对线状Cu/Sn/Cu和Cu/Sn/Ni互连金属间化合物形成的影响

L. D. Chen, M. Huang, S. M. Zhou
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In the case of Cu/Sn/Cu interconnect, the same types of IMCs, Cu<inf>6</inf>Sn<inf>5</inf> and Cu<inf>3</inf>Sn, formed at the Sn/Cu interface, which was independent of electric current. EM caused a polarity effect, i.e., the interfacial IMCs on the anode side were significantly thicker than those on the cathode side. The growth kinetics of the interfacial IMCs on the anode side during EM were significantly enhanced compared with that of the aging (the no-current case), and still followed a t<sup>1/2</sup> law with time. The temperature was one of the critical factors that influenced the EM. The effect of EM became more significant at higher temperature under the same current density. The growth behavior of the interfacial IMCs on the cathode sides was complicated. When the initial interfacial IMCs were very thin, the inward atomic fluxes were larger than the outward fluxes and thus the interfacial IMCs grew. After the IMCs reached a critical thickness, the inward atomic fluxes were less than the outward fluxes and thus the thickness of the interfacial IMCs decreased. In the case of Cu/Sn/Ni interconnects, Ni<inf>3</inf>Sn<inf>4</inf> and Cu<inf>6</inf>Sn<inf>5</inf> IMCs formed at the as-soldered Sn/Ni and Sn/Cu interfaces, respectively. The Cu content in the IMCs at the Sn/Ni interface increased with the increasing aging time, and the original Ni<inf>3</inf>Sn<inf>4</inf> IMC at the Sn/Ni interface transformed into (Cu<inf>0.56</inf>Ni<inf>0.44</inf>)<inf>6</inf>Sn<inf>5</inf> after aging at 150 °C for 200h; while the IMC at the Sn/Cu interface remained Cu<inf>6</inf>Sn<inf>5</inf>, which contained less than 0.5 at% Ni even after aging at 150 °C for 200h. When electrons flowed from Cu side to Ni side in the Cu/Sn/Ni interconnects during EM at 150 °C, the original interfacial Ni<inf>3</inf>Sn<inf>4</inf> IMC at the Sn/Ni interface (anode side) had already transformed into (CuNi)<inf>6</inf>Sn<inf>5</inf> type after EM for 100h. After EM for 200h, (Cu<inf>0.60</inf>Ni<inf>0.40</inf>)<inf>6</inf>Sn<inf>5</inf> formed at the Sn/Ni interface and Cu<inf>6</inf>Sn<inf>5</inf> (containing less than 0.1 at% Ni) formed at the Sn/Cu interface. When the direction of electron flow was reversed, after EM at 150 °C for 200h, the types of IMCs remained unchanged, i.e., Ni<inf>3</inf>Sn<inf>4</inf> (containing 2 at% Cu) and Cu<inf>6</inf>Sn<inf>5</inf> (containing less than 2 at% Ni) formed at the Sn/Ni and Sn/Cu interfaces, respectively. The diffusivity of Cu atoms in Sn is two orders of magnitude higher than that of Ni in Sn. Thus, Cu atoms would easily diffuse across the bulk solder than Ni atoms and influence the interfacial reactions on both the anode and cathode sides when electrons flowed from Cu side to Ni side. However, the diffusion of Cu atoms was blocked while against the electron wind, i.e., when electrons flowed from Ni side to Cu side.","PeriodicalId":429629,"journal":{"name":"2010 Proceedings 60th Electronic Components and Technology Conference (ECTC)","volume":"189 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2010-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"16","resultStr":"{\"title\":\"Effect of electromigration on intermetallic compound formation in line-type Cu/Sn/Cu and Cu/Sn/Ni interconnects\",\"authors\":\"L. D. Chen, M. Huang, S. M. 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引用次数: 16

摘要

在本研究中,采用线状Cu/Sn/Cu和Cu/Sn/Ni互连来测定界面金属间化合物(IMCs)在电迁移(EM)下的生长动力学,由于其对称结构,可望避免电流拥挤效应和热迁移。Cu/Sn/Cu互连体在100℃和150℃时的电流密度为5.0×103 A/cm2, Cu/Sn/Ni互连体在150℃时的电流密度相同。为了比较Cu/Sn/Cu和Cu/Sn/Ni互连在相同温度下时效的时间。在Cu/Sn/Cu互连的情况下,在Sn/Cu界面处形成了相同类型的imc Cu6Sn5和Cu3Sn,且与电流无关。EM引起极性效应,即阳极侧界面imc明显厚于阴极侧界面imc。阳极侧界面IMCs的生长动力学与时效(无电流情况)相比显著增强,且随时间仍遵循t1/2规律。温度是影响电磁效应的关键因素之一,在相同电流密度下,温度越高,电磁效应越显著。界面IMCs在阴极两侧的生长行为较为复杂。当初始界面IMCs很薄时,向内原子通量大于向外原子通量,界面IMCs增大。当IMCs达到临界厚度后,向内原子通量小于向外原子通量,界面IMCs的厚度减小。在Cu/Sn/Ni互连的情况下,Ni3Sn4和Cu6Sn5 IMCs分别在Sn/Ni和Sn/Cu界面形成。随着时效时间的延长,Sn/Ni界面IMC中Cu含量增加,在150℃时效200h后,Sn/Ni界面IMC由Ni3Sn4转变为(Cu0.56Ni0.44)6Sn5;而在150℃时效200h后,Sn/Cu界面处的IMC仍为Cu6Sn5,含镍量低于0.5 %。当电子在150℃的EM条件下从Cu侧流向Ni侧时,Sn/Ni界面(阳极侧)的原始界面Ni3Sn4 IMC在EM作用100h后已经转变为(CuNi)6Sn5型。EM作用200h后,Sn/Ni界面处形成(Cu0.60Ni0.40)6Sn5, Sn/Cu界面处形成Cu6Sn5 (% Ni含量小于0.1)。当电子流方向相反时,在150°C下电加热200h后,IMCs的类型保持不变,即在Sn/Ni和Sn/Cu界面处分别形成Ni3Sn4(含2 % Cu)和Cu6Sn5(含小于2 % Ni)。Cu原子在Sn中的扩散系数比Ni原子在Sn中的扩散系数高两个数量级。因此,当电子从Cu侧流向Ni侧时,Cu原子比Ni原子更容易在大块焊料中扩散,并影响阳极和阴极两侧的界面反应。然而,逆电子风,即电子从Ni侧流向Cu侧时,Cu原子的扩散受到阻碍。
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Effect of electromigration on intermetallic compound formation in line-type Cu/Sn/Cu and Cu/Sn/Ni interconnects
In this study, the line-type Cu/Sn/Cu and Cu/Sn/Ni interconnects were used to determine the growth kinetics of interfacial intermetallic compounds (IMCs) under electromigration (EM), and the current crowding effect and thermomigration are expected to be avoided in this line-type interconnects because of their symmetric structure. The Cu/Sn/Cu interconnect was under the current density of 5.0×103 A/cm2 at 100 °C and 150 °C, and the Cu/Sn/Ni interconnect was under the same current density at 150 °C. For the purpose of comparison, the Cu/Sn/Cu and Cu/Sn/Ni interconnects were aged at the same temperatures for the same durations. In the case of Cu/Sn/Cu interconnect, the same types of IMCs, Cu6Sn5 and Cu3Sn, formed at the Sn/Cu interface, which was independent of electric current. EM caused a polarity effect, i.e., the interfacial IMCs on the anode side were significantly thicker than those on the cathode side. The growth kinetics of the interfacial IMCs on the anode side during EM were significantly enhanced compared with that of the aging (the no-current case), and still followed a t1/2 law with time. The temperature was one of the critical factors that influenced the EM. The effect of EM became more significant at higher temperature under the same current density. The growth behavior of the interfacial IMCs on the cathode sides was complicated. When the initial interfacial IMCs were very thin, the inward atomic fluxes were larger than the outward fluxes and thus the interfacial IMCs grew. After the IMCs reached a critical thickness, the inward atomic fluxes were less than the outward fluxes and thus the thickness of the interfacial IMCs decreased. In the case of Cu/Sn/Ni interconnects, Ni3Sn4 and Cu6Sn5 IMCs formed at the as-soldered Sn/Ni and Sn/Cu interfaces, respectively. The Cu content in the IMCs at the Sn/Ni interface increased with the increasing aging time, and the original Ni3Sn4 IMC at the Sn/Ni interface transformed into (Cu0.56Ni0.44)6Sn5 after aging at 150 °C for 200h; while the IMC at the Sn/Cu interface remained Cu6Sn5, which contained less than 0.5 at% Ni even after aging at 150 °C for 200h. When electrons flowed from Cu side to Ni side in the Cu/Sn/Ni interconnects during EM at 150 °C, the original interfacial Ni3Sn4 IMC at the Sn/Ni interface (anode side) had already transformed into (CuNi)6Sn5 type after EM for 100h. After EM for 200h, (Cu0.60Ni0.40)6Sn5 formed at the Sn/Ni interface and Cu6Sn5 (containing less than 0.1 at% Ni) formed at the Sn/Cu interface. When the direction of electron flow was reversed, after EM at 150 °C for 200h, the types of IMCs remained unchanged, i.e., Ni3Sn4 (containing 2 at% Cu) and Cu6Sn5 (containing less than 2 at% Ni) formed at the Sn/Ni and Sn/Cu interfaces, respectively. The diffusivity of Cu atoms in Sn is two orders of magnitude higher than that of Ni in Sn. Thus, Cu atoms would easily diffuse across the bulk solder than Ni atoms and influence the interfacial reactions on both the anode and cathode sides when electrons flowed from Cu side to Ni side. However, the diffusion of Cu atoms was blocked while against the electron wind, i.e., when electrons flowed from Ni side to Cu side.
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