• 대한용접접합학회:학술대회논문집
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• 대한용접접합학회 2006년 추계학술발표대회 개요집
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• pp.181-183
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• 2006

This paper studies the mechanical behaviors of Sn-3.5Ag solder joint against substrate(such as Au/Ni/Cu, Au/cu, Ni/Cu and Cu pad) after induction heating, a new soldering method. It was found that the solder bump formation depends on the time and current of the induction heating system. Also the heating value of the solder bump were found to vary with respect to the thermal conductivity of the pads on the substrate. In case of Au/Ni/Cu pad and Au/Cu pad, solder bump's shear strength were high for the heating time of $1.5{\sim}2sec$. For Ni/Cu pad, solder bump's shear strength were found to increase with time increment.

• 한국표면공학회지
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• 제36권5호
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• pp.386-392
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• 2003

The electroplating process for a solder bump which can be applied for a flip chip was studied. Si-wafer was used for an experimental substrate, and the substrate were coated with UBM (Under Bump Metallization) of Al(400 nm)/Cu(300 nm)Ni(400 nm)/Au(20 nm) subsequently. The compositions of the bump were Sn-Cu and eutectic Sn-Pb, and characteristics of two bumps were compared. Experimental results showed that the electroplated thickness of the solders were increased with time, and the increasing rates were TEX>$0.45 <\mu\textrm{m}$/min for the Sn-Cu and $ 0.35\mu\textrm{m}$/min for the Sn-Pb. In the case of Sn-Cu, electroplating rate increased from 0.25 to $2.7\mu\textrm{m}$/min with increasing current density from 1 to 8.5 $A/dm^2$. In the case of Sn-Pb the rate increased until the current density became $4 A/dm^2$, and after that current density the rate maintains constant value of $0.62\mu\textrm{m}$/min. The electro plated bumps were air reflowed to form spherical bumps, and their bonded shear strengths were evaluated. The shear strength reached at the reflow time of 10 sec, and the strength was of 113 gf for Sn-Cu and 120 gf for Sn-Pb.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2010년도 춘계학술대회 논문집
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• pp.665-666
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• 2010

• 대한용접접합학회:학술대회논문집
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• 대한용접접합학회 2002년도 춘계학술발표대회 개요집
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• pp.276-277
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• 2002

• Journal of Welding and Joining
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• 제29권6호
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• pp.65-70
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• 2011

The effect of flip chip bonding parameters on formation of intermetallic compounds (IMCs) between Au stud bumps and Sn-3.5Ag solder was investigated. In this study, flip chip bonding temperature was performed at $260^{\circ}C$ and $300^{\circ}C$ with various bonding times of 5, 10, and 20 sec. AuSn, $AuSn_2$ and $AuSn_4$ IMCs were formed at the interface of joints and (Au, Cu)$_6Sn_5$ IMC was observed near Cu pad side in the joint. At bonding temperature of $260^{\circ}C$, $AuSn_4$ IMC was dominant in the joint compared to other Au-Sn IMCs as bonding time increased. At bonding temperature of $300^{\circ}C$, $AuSn_2$ IMC clusters, which were surrounded by $AuSn_4$ IMC, were observed in the solder joint due to fast diffusivity of Au to molten solder with increased bonding temperature. Bond strength of Au stud bump joined with Sn-3.5Ag solder was about 23 gf/bump and fracture mode of the joint was intergranular fracture between $AuSn_2$ and $AuSn_4$ IMCs regardless bonding conditions.

• 대한금속재료학회지
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• 제49권5호
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• pp.411-418
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• 2011

The current study investigates the electroplating characteristics of Sn-Cu eutectic micro-bumps electroplated on a Si chip for flip chip application. Under bump metallization (UBM) layers consisting of Cr, Cu, Ni and Au sequentially from bottom to top with the aim of achieving Sn-Cu bumps $10\times10\times6$ ${\mu}m$ in size, with 20${\mu}m$ pitch. In order to determine optimal plating parameters, the polarization curve, current density and plating time were analyzed. Experimental results showed the equilibrium potential from the Sn-Cu polarization curve is -0.465 V, which is attained when Sn-Cu electro-deposition occurred. The thickness of the electroplated bumps increased with rising current density and plating time up to 20 mA/$cm^2$ and 30 min respectively. The near eutectic composition of the Sn-0.72wt%Cu bump was obtained by plating at 10 mA/$cm^2$ for 20 min, and the bump size at these conditions was $10\times10\times6$ ${\mu}m$. The shear strength of the eutectic Sn-Cu bump was 9.0 gf when the shearing tip height was 50% of the bump height.

• 마이크로전자및패키징학회지
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• 제10권2호
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• pp.61-67
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• 2003

고집적 플립 칩 기술을 위한 $50{\mu}m$ 직경의 극미세 58Bi-42Sn 솔더 범프와 Au/Ni/Ti UBM의 계면 반응에 따른 금속간 화합물을 분석하였다. 증발증착법과 lift-off 방법으로 극미세 Bi-Sn 솔더 범프를 형성하고 급속열처리 장비를 이용하여 리플로 공정을 실시하였다. 리플로 공정에서의 냉각속도를 변화시키면서 제작한 솔더 범프의 표면과 단면을 주사전자현미경으로 관찰하였다 $Au(0.1{\mu}m)$/Ni/Ti UBM 위의 극미세 58Bi-42Sn 솔더 범프의 표면과 내부에서 facet 특성을 갖는 다각형의 금속간 화합물들이 다수 관찰되었다. 주사전자현미경의 EDS 분석과 X-선 회절분석으로 확인한 결과 이 금속간 화합물은 $(Au_xBi_yNi_{1-x-y})Sn_2$상임을 확인하였다.

• 한국재료학회지
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• 제10권12호
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• pp.853-863
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• 2000

Cu 칩의 Cu 패드 위에 솔더 플립칩 공정에 응용하기 위한 무전해 구리/니켈 UBM (Under Bump Metallurgy) 층을 형성하고 그 특성을 조사하였다. Sn-36Pb-2Ag 솔더 범프와 무전해 구리 및 무전해 니켈 충의 사이의 계면 반응을 이해하고, UBM의 종류와 두계에 따른 솔더 범프 접합(joint) 강도 특성의 변화를 살펴보았다. UBM의 종류에 따른 계면 미세 구조, 특히 금속간 화합물 상 및 형태가 솔더 접합 강도에 크게 영향을 미치는 것을 확인하였다. 무전해 구리 UBM의 경우에는 솔더와의 계면에서 연속적인 조가비 모양의 Cu$_{6}$Sn$_{5}$상이 빠르게 형성되어 파단이 이 계면에서 발생하여 낮은 범프 접합 강도 값을 나타내었다. 무전해 니켈/무전해 구리 UBM에서는 금속간 화합물 성장이 느리고, 비정질로 도금되는 무전해 Ni의 륵성으로 인해 금속간 화합물과의 결정학적 불일치가 커져 다각형의 Ni$_3$Sn$_4$상이 형성되어 무전해 구리 UBM의 경우에 비해 범프 접합 강도가 높게 나타났다. 따라서 무전해 도금을 이용하여 Cu 칩의 Cu pad 위에 솔더 플립칩 공정에 응용하기 위한 UBM 제작시 무전해 니켈/무전해 구리 UBM을 선택하는 것이 접합 강도 측면에서 유리하다는 것을 확인하였다.다.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2012년도 추계학술대회 논문집
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• pp.477-478
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• 2012

• 한국재료학회지
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• 제17권2호
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• pp.91-95
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• 2007

Electromigration characteristics of Sn-3.5Ag flip chip solder bump were analyzed using flip chip packages which consisted of Si chip substrate and electroplated Cu under bump metallurgy. Electromigration test temperatures and current densities peformed were $140{\sim}175^{\circ}C\;and\;6{\sim}9{\times}10^4A/cm^2$ respectively. Mean time to failure of solder bump decreased as the temperature and current density increased. The activation energy and current density exponent were found to be 1.63 eV and 4.6, respectively. The activation energy and current density exponent have very high value because of high Joule heating. Evolution of Cu-Sn intermetallic compound was also investigated with respect to current density conditions.