TW201504459A - Cu核球 - Google Patents
Cu核球 Download PDFInfo
- Publication number
- TW201504459A TW201504459A TW103113348A TW103113348A TW201504459A TW 201504459 A TW201504459 A TW 201504459A TW 103113348 A TW103113348 A TW 103113348A TW 103113348 A TW103113348 A TW 103113348A TW 201504459 A TW201504459 A TW 201504459A
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- ball
- nucleus
- solder
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
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- H01L24/00—Arrangements for connecting or disconnecting semiconductor or solid-state bodies; Methods or apparatus related thereto
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B22—CASTING; POWDER METALLURGY
- B22F—WORKING METALLIC POWDER; MANUFACTURE OF ARTICLES FROM METALLIC POWDER; MAKING METALLIC POWDER; APPARATUS OR DEVICES SPECIALLY ADAPTED FOR METALLIC POWDER
- B22F1/00—Metallic powder; Treatment of metallic powder, e.g. to facilitate working or to improve properties
- B22F1/17—Metallic particles coated with metal
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K35/00—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting
- B23K35/02—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting characterised by mechanical features, e.g. shape
- B23K35/0222—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting characterised by mechanical features, e.g. shape for use in soldering, brazing
- B23K35/0244—Powders, particles or spheres; Preforms made therefrom
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B23—MACHINE TOOLS; METAL-WORKING NOT OTHERWISE PROVIDED FOR
- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K35/00—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting
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- B23K35/24—Selection of soldering or welding materials proper
- B23K35/26—Selection of soldering or welding materials proper with the principal constituent melting at less than 400 degrees C
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- B—PERFORMING OPERATIONS; TRANSPORTING
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- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K35/00—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting
- B23K35/22—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting characterised by the composition or nature of the material
- B23K35/24—Selection of soldering or welding materials proper
- B23K35/26—Selection of soldering or welding materials proper with the principal constituent melting at less than 400 degrees C
- B23K35/262—Sn as the principal constituent
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- B—PERFORMING OPERATIONS; TRANSPORTING
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- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K35/00—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting
- B23K35/22—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting characterised by the composition or nature of the material
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- B—PERFORMING OPERATIONS; TRANSPORTING
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- B23K—SOLDERING OR UNSOLDERING; WELDING; CLADDING OR PLATING BY SOLDERING OR WELDING; CUTTING BY APPLYING HEAT LOCALLY, e.g. FLAME CUTTING; WORKING BY LASER BEAM
- B23K35/00—Rods, electrodes, materials, or media, for use in soldering, welding, or cutting
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- B23K35/302—Cu as the principal constituent
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- C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
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Abstract
本發明提供可抑制軟錯誤減低連接不良之Cu核球。
形成於Cu球表面的鍍焊料披膜,係由鍍Sn焊料披膜或以Sn為主成分的無Pb焊料合金所構成,U的含量為5ppb以下,Th的含量為5ppb以下,該Cu球的純度為99.9%以上99.995%以下,Pb及/或Bi的含量的合計量為1ppm以上,真球度為0.95以上,所得Cu核球的α射線量為0.0200cph/cm2以下。
Description
本發明係關於,α射線量少的Cu核球。
近年,因小型資訊機器的發達,於搭載的電子零件進行急速的小型化。電子零件,因小型化的要求為對應連接端子的狹小化或構裝面積的縮小化,使用於背面設置電極之球柵陣列(以下,稱為「BGA」。)。
於使用BGA的電子零件,例如有半導體封裝。於半導體封裝,係將具有電極之半導體晶片以樹脂密封。於半導體晶片的電極,形成有焊料凸塊。該焊料凸塊,係藉由將焊料凸塊接合於半導體晶片的電極而形成。使用BGA的半導體封裝,係藉由使加熱熔融之焊料凸塊與印刷電路板的導電性焊墊接合,而搭載於印刷電路板。此外,為對應更高密度構裝的要求,亦有將半導體封裝於高度方向疊層之3維高密度構裝的研究。
但是,在3維高密度構裝的半導體封裝使用BGA,則有因半導體封裝的自重而將焊料球壓潰之情形。如果發生如此之情形,則焊料由電極溢出,可能使電極間連接,而發生短路。
因此,有由接合於電子零件的電極的Cu核球所構
成之焊料凸塊的研究。所謂Cu核球,係指於Cu球的表面形成焊料披膜者。使用Cu核球形成之焊料凸塊,在將電子零件構裝於印刷電路板時,即使半導體封裝的重量施加於焊料凸塊,藉由以焊料的熔點並不會熔融之Cu球支撐半導體封裝。因此,並不會因半導體封裝的自重而壓潰。關聯技術可舉例如專利文獻1。
於專利文獻1揭示有真球度高的Cu球的發明,亦有於Cu球披覆之Cu核球之記載。於同文獻,例示構成元素為Pb及Sn所構成的Pb-Sn焊料。此外,於同文獻,作為披膜的形成方法,揭示有鍍敷法、熔接法、焊接法等作為等價的方法。該等之中,鍍敷法,揭示有筒式電鍍等的電鍍法。
然而,電子零件的小型化雖可高密度構裝,但高密度構裝有容易引起軟錯誤的問題。軟錯誤係指因α射線射入半導體積體電路(以下,稱為「IC」。)的記憶胞中而有將記憶內如改寫的可能性者。α射線,可認為係焊料合金中的U、Th、210Po等的放射性元素因α衰變而輻射者。因此,於近年有減低放射性元素含量的低α射線焊料材料的開發的進行。關聯文獻,可舉例如專利文獻2。
於專利文獻2,揭示有α射線低的Sn晶棒的發明,記載有為減低α射線,並不單只進行電解晶練,藉由在電解液懸浮吸附劑將Pb或Bi吸附而減低α射線。
[先前技術文獻]
[專利文獻]
[專利文獻1]國際公開95/24113號
[專利文獻2]日本專利第4472752號公報
本發明的課題,係在於提供抑制軟錯誤的發生的Cu核球,具體而言係α射線少的Cu核球。
但是,於專利文獻1,完全沒有考慮減低Cu核球的α射線量的課題。此外,於同文獻,構成焊料披膜的焊料合金,唯一揭示Pb-Sn合金作為先前技術。α射線係包含於Sn的雜質之Pb的同位素210Pb,衰變210Pb→210Bi→210Po→206Pb的過程,由210Pb放射。由於同文獻所唯一揭示的Pb-Sn合金包含多量的Pb,可認為亦包含放射性元素210Pb。因此,即使將該焊料合金使用於Cu核球的焊料披膜,由於在專利文獻1,完全沒有考慮減低α射線的課題,故很難認為同文獻所揭示的Cu核球顯示低的α射線量。
於專利文獻2,如上所述,有藉由電解液或電極以靜止的狀態進行的電解精煉,去除Sn晶棒中的Pb或Bi減低α射線量的記載。但是,於同文獻,完全沒有揭示關於對Cu球進行鍍Sn,或Cu球及電解液在流動的狀態進行電鍍。此外,同文獻所記載的電解精煉,由於電解析出面僅限於一方向,故無法對如Cu球等的微小工件形成均勻的鍍層。
再者,根據專利文獻2,由於Pb或Bi與Sn的標準電極電位接近,僅以一般的電解精煉進行使Sn對平板電極的電解析出,難以減低α射線量。假如,將專利文獻2所記載
的電解精煉使用於形成Cu球的鍍敷披膜,將鍍敷液懸浮於吸附劑進行筒式電鍍,則鍍敷液或工件被攪拌,吸附劑亦同時被攪拌。此時,吸附於吸附劑的Pb離子或Bi離子有成為載體與吸附劑一起取入焊料披膜內的可能性。取入吸附劑的焊料披膜,會放射很高的α射線。此外,吸附劑的粒徑為次微米程度而非常的小,故可認為由邊流動的鍍敷液分離.回收懸浮後的吸附劑非常的難。因此,難以不使吸附Pb或Bi的吸附劑取入披膜。
加上該等,於專利文獻1雖揭示Pb-Sn合金,但係揭示鍍敷法、熔接法、焊接法等作為等價的方法,故反而是否定減低α射線的記載。專利文獻1的課題,係在於製造真球度高的Cu核球。另一方面,專利文獻2,為解決減低α射線量的課題,揭示以電解精煉盡可能去除Sn中的Pb。因此,知道專利文獻1的業者,並不會想到專利文獻2所揭示之減低Cu核球的α射線量的課題,並且,由於焊料組成亦相反,故想到減低α射線量的課題,想到進一步取代構成焊料披膜的Pb-Sn焊料合金,由無數存在的焊料合金中使用Sn系焊料,需要進行多次的嘗試錯誤。
如此地,即使是該業者,並無法組合專利文獻1與專利文獻2。更言之,即使是該業者,難以使用專利文獻2所揭示之α射線量低的Sn晶棒製作鍍敷液,藉由專利文獻1所揭示的鍍敷法形成Cu核球。
如此地,使用專利文獻1或專利文獻2所記載的先前技術製造的Cu核球,用於形成接點,則存在於Cu核球的
焊料披膜中的放射線元素擴散至接點的電極,而射出α射線的可能性高。因此,即使組合先前的技術,並無法減低Cu核球的α射線量,故藉由高密度構裝而無法避免成為新問題的軟錯誤。
本發明者們,首先進行使用於Cu核球之Cu球之選定。結果,發現只要在Cu球不含有一定量的Pb及/或Bi,則會使Cu球的真球度降低,進行焊料鍍敷時對Cu球的焊料鍍敷不均勻,結果,所得Cu核球的真球度會降低。
其次,為減低構成Cu核球之焊料披膜的α射線,著眼於使用鍍敷法形成焊料鍍敷披膜之點進行銳意研究。本發明者們,為減低鍍敷液中的Pb、Bi,或由該等元素的衰變所生成之Po,使Cu球或鍍敷液流動於Cu球形成鍍敷披膜時,意外地,即使不懸浮吸附劑該等Pb、Bi、Po元素形成鹽。因此,該鹽由於係電中性,故並不會在鍍敷披膜取入該等元素,而得到可減低構成Cu核球之鍍敷披膜之α射線量之見識。
在此,本發明如下。
(1)一種Cu核球,包括:Cu球;及披覆於該Cu球的表面之焊料鍍敷披膜之Cu核球,其特徵在於:上述焊料鍍敷披膜,係Sn焊料鍍敷披膜或以Sn為主成分的無Pb焊料合金所構成之焊料鍍敷披膜,U的含量為5ppb以下,Th的含量為5ppb以下,該Cu球的純度為99.9%以上99.995%以下,Pb及/或Bi
的含量的合計量為1ppm以上,真球度為0.95以上,然後,Cu核球的α射線量為0.0200cph/cm2以下。
在此,所謂「以Sn為主成分」係指焊料鍍敷披膜中的Sn含量對披膜質量為40質量%以上。因此,構成本發明之焊料鍍敷披膜包含Sn焊料鍍敷披膜。
(2)根據上述(1)之Cu核球,其中上述Cu核球的α射線量為0.0020cph/cm2以下。
(3)根據上述(1)之Cu核球,其中上述Cu核球的α射線量為0.0010cph/cm2以下。
(4)根據上述(1)至(3)中任一項之Cu核球,其中上述Cu球中的Pb及Bi的含量合計為1ppm以上。
(5)根據上述(1)至(4)中任一項之Cu核球,其直徑為1~1000μm。
(6)根據上述(1)至(5)中任一項之Cu核球,其中上述Cu球,在以上述焊料鍍敷披膜披覆之前預先以選自由Ni及Co之1元素以上所組成的鍍敷層披覆。
(7)一種接點,使用上述(1)至(6)中任一項之Cu核球所形成。
第1圖係使用純度為99.9%的Cu錠所製造的Cu球之SEM照片。
第2圖係使用純度為99.995%以下的Cu線所製造的Cu球之SEM照片。
第3圖係使用純度超過99.995%的Cu板所製造的Cu球之SEM照片。
以下,更詳細地說明本發明。在於本說明書,關於Cu核球之鍍敷披膜的組成之單位(ppm、ppb、及%),若無特別指定係表示對鍍敷披膜之質量之比例(質量ppm、質量ppb、及質量%)。此外,關於Cu球的組成之單位(ppm、ppb、及%),若無特別指定係表示對Cu球之質量之比例(質量ppm、質量ppb、及質量%)。
關於本發明之Cu核球,包括:Cu球;及披覆於該Cu球的表面之焊料鍍敷披膜。本發明之焊料鍍敷披膜,係主要對工件之Cu球,使鍍敷液流動而形成。藉由鍍敷液的流動於鍍敷液中Pb、Bi、Po的元素形成鹽而沉澱。一旦形成鹽之析出物,則會穩定地存在於鍍敷液中。因此,關於本發明之Cu核球並不會被取入鍍敷披膜,可減低包含於鍍敷披膜之放射性元素的含量,可減低Cu核球本身的α射線量。
以下,詳述關於Cu核球之構成要素之焊料鍍敷披膜及Cu球。
1.焊料鍍敷披膜
.焊料鍍敷披膜的組成
焊料鍍敷披膜的組成,以合金之情形,只要是以Sn為主成分的無Pb焊料合金之合金組合,並無特別限定。此外,焊料鍍敷披膜,可為Sn鍍敷披膜。可舉例如,Sn、Sn-Ag合金、Sn-Cu合金、Sn-Ag-Cu合金、Sn-In合金、即對該等添加既定
的合金元素者。均為Sn含量為40質量%以上。添加的合金元素,例如有Ag、Cu、In、Ni、Co、Sb、Ge、P、Fe等。該等之中,焊料鍍敷披膜的合金組成,由落下衝擊特性的觀點,以Sn-3Ag-0.5Cu為佳。
焊料鍍敷披膜的厚度,並無特別限定,以100μm(單邊)以下即充分。一般以20~50μm即可。
.U:5ppb以下,Th:5ppb以下
U及Th係放射性元素,為抑制軟錯誤需要抑制該等的含量。U及Th的含量,在為使焊料鍍敷披膜的α射線量在0.0200cph/cm2以下,需要各為5ppb以下。此外,於現在或未來的高密度構裝抑制軟錯誤的觀點,U及Th的含量,各以2ppb以下為佳。
.α射線量:0.0200cph/cm2以下
關於本發明之Cu核球的α射線量為0.0200cph/cm2以下。此係,在於電子零件的高密度構裝軟錯誤不會成為問題的程度的α射線量。關於本發明之Cu核球之α射線量,可藉由構成Cu核球的焊料鍍敷披膜的α射線量在0.0200cph/cm2以下而達成。本發明之焊料鍍敷披膜頂多以100℃形成,故難以認為可藉由U、Th、210Po、Bi及Pb等的放射性元素的汽化而減低放射性元素的減低。但是,邊使鍍敷液或Cu球流動進行鍍敷,則U、Th、Pb、Bi、及210Po會在鍍敷液中形成鹽而沉澱。由於沉澱的鹽係電中性,即使鍍敷液流動,並不會混入焊料鍍敷披膜中。可顯著地減低該等在焊料鍍敷披膜中的含量。因此,關於本發明之Cu核球,由於係以如此之焊料鍍敷披膜批覆,
故顯示較低的α射線量。α射線量,在更進一步的高密度構裝抑制軟錯誤的觀點,以0.0020cph/cm2以下為佳,以0.0010cph/cm2以下更佳。
構成本發明之焊料鍍敷披膜的純度越高,即雜質的含量越少,可減低放射性元素的含量,減低α射線量,故雜質量的下限值並無特別限定。另一方面,上限值,由減低α射線量的觀點,以150ppm以下為佳,以100ppm以下更佳,進一步以50ppm以下為佳,以10ppm以下特別佳。
再者,焊料鍍敷披膜為Sn焊料時,焊料鍍敷披膜的純度,係焊料鍍敷披膜中的Sn以外的雜質的合計量。此外,焊料鍍敷披膜為Sn-3Ag-0.5Cu的焊料合金時,焊料鍍敷披膜的純度,係焊料鍍敷披膜中的Sn、Ag、及Cu以外的雜質的含量的合計。
包含於焊料鍍敷披膜的雜質,於Sn焊料鍍敷披膜之情形,可舉Ag、Ni、Pb、Au、U、Th等。由Sn-Ag-Cu合金所構成的焊料鍍敷披膜時,可舉Sn、Fe、As、In、Ni、Pb、Au、U、Th等。於雜質,特別是以Bi的含量較少為佳。一般而言,於Bi的原料包含微量的放射性同位素之210Bi。因此,藉由減低Bi的含量,可認為可顯著地減低焊料鍍敷披膜的α射線量。Bi的含量,以15ppm以下為佳,以10ppm以下更佳,以0ppm特別佳。
2.Cu球
其次,詳述關於構成本發明之Cu球。
構成本發明之Cu球,係於Cu核球用於焊料凸塊
時,由於並不會在焊接的溫度熔融,可抑制焊料接點的高度的離散。因此,Cu球以真球度高而直徑的離散少者為佳。此外,如上所述,Cu球的α射線量亦與焊料披膜Cu樣地低為佳。以下記載Cu球的較佳的態樣。
.Cu球的純度:99.9%以上99.995%以下
構成本發明之Cu球以99.9%以上99.995%以下為佳。Cu球的純度在此範圍,則可於熔融Cu中確保充分量可提高Cu球的真球度的結晶核。提高真球度的理由,詳述如下。
製造Cu球時,形成為既定形狀的小片的Cu材,係藉由加熱熔融,熔融Cu藉由表面張力而成為球形,此凝固成為Cu球。在於熔融Cu由液體狀態凝固的過程,結晶粒在球形的熔融Cu中成長。此時,雜質多,則該雜質元素成為結晶核而抑制結晶粒的成長。因此,球形的熔融Cu,藉由抑制成長的細微結晶粒成為真球度高的Cu球。另一方面,雜質元素少,則相對地成為結晶核者少,無法抑制粒成長而帶著方向性成長。結果,球形的熔融Cu在表面的一部分凸出凝固。如此的Cu球真球度低。雜質元素,可考慮Sn、Sb、Bi、Zn、As、Ag、Cd、Ni、Pb、Au、P、S、U、Th等。
純度的下限值並無特別限定,由抑制α射線量,抑制因純度的降低而使Cu球的導電度或熱傳導率的惡化的觀點,以99.9%以上為佳。
在此,相對於焊料鍍敷披膜純度越高越可減低α射線量,於Cu球即使不使純度提高到必要以上,亦可減低α射線量。Cu熔點較Sn高,於製造時的加熱溫度Cu較高。於
本發明,製造Cu球時,由於如後所述對Cu球進行先前並未對Cu材進行之加熱處理,故210Pb、210Bi等的放射線元素會揮發。另一方面,使用以Sn為主成分之焊料形成焊料鍍敷披膜時,焊料合金僅加熱至100℃左右的溫度。由於在焊料鍍敷處理,上述放射性元素幾乎不會揮發而殘存於鍍敷液,故需要降低Pb或Bi等的雜質濃度,提高焊料鍍敷披膜的純度。
.α射線量:0.0200cph/cm2以下
構成本發明之Cu球的α射線量,較佳的是0.0200cph/cm2以下。此係,在於電子零件的高密度構裝軟錯誤不會成為問題的程度的α射線量。於本發明,加上用於製造Cu球通常進行的步驟,施以再度加熱處理。因此,些微殘存於Cu的原材料的210Po揮發,與Cu的原材料相比Cu球顯示更低的α射線量。α射線量,在更進一步的高密度構裝抑制軟錯誤的觀點,以0.0020cph/cm2以下為佳,以0.0010cph/cm2以下更佳。
.Pb及Bi的含量以合計為1ppm以上
構成本發明之Cu球,含有Sn、Sb、Bi、Zn、As、Ag、Cd、Ni、Pb、Au、P、S、U、Th等,特別是Pb及/或Bi的含量合計以含有1ppm以上為佳。於本發明,即使是在於焊料接點的形成時露出Cu球時,於減低α射線量上並沒有需要將Cu球的Pb及/或Bi的含量減低至極限。此係根據以下的理由。
210Pb及210Bi係藉由β衰變變化為210Po。為減低α射線量,雜質元素的Pb及Bi的含量盡量低為佳。
但是,包含於Pb及Bi的210Pb及210Bi的含有比低。只要某種程度減低Pb或Bi的含量,則可認為幾乎去除210Pb
及210Bi。關於本發明的Cu球,Cu的溶解溫度設定較先前稍高,或對Cu材及/或造粒後的Cu球施以加熱處理而製造。此溫度,由於即使是較Pb或Bi的沸點低之情形亦未發生氣化故可減低雜質元素量。此外,為提高Cu球的真球度雜質元素的含量高較佳。因此,本發明的Cu球,Pb及/或Bi的含量以合計為1ppm以上。Pb及Bi均包含時,Pb及Bi的合計含量為1ppm以上。
如此地,Pb及/或Bi由於在製造Cu球之後亦有某種程度的殘存而含量的測定誤差少。再者如前所述Bi及Pb在於Cu球的製造步驟之熔融時會成為結晶核,故藉由添加一定量的Bi或Pb可製造真球度高的Cu球。因此,Pb或Bi,係用於推測雜質元素的含量的重要的元素。由如此的觀點,Pb及/或Bi的含量以合計為1ppm以上為佳。Pb及/或Bi的含量,合計以10ppm以上更佳。上限值,並無特別限定,由抑制Cu球的導電度惡化的觀點,Pb及/或Bi的含量的含量合計以未滿1000ppm更佳,進一步以100ppm以下為佳。Pb的含量,以10ppm~50ppm為佳,Bi的含量,以10ppm~50ppm更佳。
.Cu球的真球度:0.95以上
構成本發明之Cu球,由控制站立高度的觀點真球度為0.95以上。Cu球的真球度未滿0.95,則由於Cu球將成不定形狀,而於凸塊形成時形成高度不均勻的凸塊,提高發生接合不良的可能性。再者,對Cu球的鍍敷成為不均勻,將Cu核球搭載於電極進行回焊時,發生Cu核球的位移,而使自我對準性惡化。真球度,以0.990以上更佳。在於本發明,真球度係表
示由真球的偏移。真球度,可例如,以最小平方中心法(LSC法)、最小區域中心法(MZC法)、最大內接中心法(MIC法)、最小外接中心法(MCC法)等各種方法求得。
.Cu球的直徑:1~1000μm
構成本發明之Cu球的直徑以1~1000μm為佳。在於該範圍,則可穩定地製造球狀的Cu球,此外,端子間為窄間距時可抑制連接之短路。
在此,例如,關於本發明的Cu核球的直徑為1~300μm程度時,「Cu核球」的集合體亦可稱為「Cu核球粉」。在此,「Cu核球粉」,係將包括上述特性的各個Cu核球,多數Cu核球的集合體。例如,調合於焊膏中的粉末等,與使用單一Cu核球的形態有所區別。同樣地,用於形成焊料凸塊時,通常作為集合體使用,與以如此之形態使用之「Cu核球粉末」與單一的Cu核球有所區別。
關於本發明的Cu核球,可於形成焊料鍍敷披膜之前,預先於Cu球的表面以其他的金屬鍍敷層披覆。特別是,於Cu球表面預先披覆鍍Ni層或鍍Co層等,由於可減低Cu對焊料鍍敷披膜中的溶出,故可抑制Cu球的Cu蝕。此外,使用於鍍敷層之金屬並不限於單一金屬,亦可使用由Ni、Co等之中組合2元素以上的合金。
此外,關於本發明之Cu核球的真球度以0.95以上為佳。Cu核球的真球度低時,將Cu核球搭在於電極進行回焊時,引起Cu核球的位移,使自我對準性惡化。真球度,以0.990以上更佳。再者,關於本發明之Cu核球,亦可使用於形成將
電子零件的端子相互接合之焊料接點。
說明關於本發明之Cu核球之製造方法之一例。
成為材料之Cu材係置於如陶瓷等之耐熱性的板(以下,稱為「耐熱板」。),與耐熱板一起於爐中加熱。於耐熱板設有多數底部呈半球狀的圓形的溝。溝的直徑或深度,可按照Cu球的粒徑適宜設定,例如,直徑為0.8mm、深度為0.88mm。此外,切斷Cu細線而得之薄片形狀的Cu材(以下,稱為「薄片材」。),於耐熱板的溝內各投入一個。於構內投入薄片材之耐熱板,係於充填氨分解氣體的爐內升溫至1100~1300℃,進行30~60分鐘的加熱處理。此時,爐內溫度成為Cu的熔點以上,則薄片材熔融成球狀。之後,爐內被冷卻,於耐熱板的溝內將Cu球成形。冷卻後,成形之Cu球,係以未滿Cu的熔點的溫度之800~1000℃再度進行加熱處理。
此外,作為別的方法,由設於坩鍋的低部的孔滴下熔融Cu的液滴,該液滴被冷卻將Cu球造粒之噴霧法,或熱電漿將切Cu金屬加熱為1000℃以上而造粒的方法。如此地造粒之Cu球,亦可分別以800~1000℃的溫度施以30~60分鐘再加熱處理。
本發明的Cu核球的製造方法,亦可於Cu球的造粒之前將Cu球的原料之Cu材以800~1000℃加熱處理。
Cu球的原料的Cu材,例如可使用錠、線、柱等。Cu材的純度,由不過度降低純度的觀點,可為99.9~99.99%。
使用更高純度的Cu材時,亦可不進行上述加熱處理,將熔融Cu的保持溫度與先前Cu樣地降至1000℃左右。
如此地,上述加熱處理,亦可按照Cu材的純度或α射線量適宜省略或變更。此外,即使製造α射線量高的Cu球或異形的Cu球時,亦可將該等Cu球作為原料再利用,可進一步降低α射線量。
此外,如上所述地製作的Cu球或使鍍敷液流動於Cu球形成鍍敷披膜的方法,有習知之筒式鍍敷等的電鍍法、連接於鍍敷槽的幫浦使鍍敷槽中的鍍敷液發生高速亂流,藉由鍍敷液的亂流於Cu球形成鍍敷披膜的方法,於鍍敷槽設振動板以既定的頻率振動使鍍敷液高速亂流攪拌,藉由鍍敷液的亂流於Cu球形成鍍敷披膜的方法等。
於直徑100μm的Cu球形成膜厚(單測)20μm的Sn-Ag-Cu焊料鍍敷披膜,作成直徑約140μm的Cu核球作為一例說明之。
關於本發明之一實施形態之含有Sn-Ag-Cu之鍍敷液,係以水為主體之媒體,含有磺酸類及金屬成分之Sn、Ag及Cu作為必要成分。
金屬成分係於鍍敷液中以Sn離子(Sn2+及/或Sn4+),Ag離子(Ag+)及Cu離子(Cu+/Cu2+)存在。鍍敷液,主要係藉由由水與磺酸類所組成的鍍敷母液與金屬化合物混合而得,為金屬離子的穩定性,含有有機錯合劑為佳。
鍍敷液中的金屬化合物,例如可例示如下者。
Sn化合物的具體例,可舉甲基磺酸、乙基磺酸、2-丙醇磺酸、對酚磺酸等的有機磺酸之錫鹽、硫酸錫、氧化錫、硝酸錫、氯化錫、嗅化錫、碘化錫、磷酸錫、焦磷酸錫、醋酸錫、蟻酸
錫、檸檬酸錫、葡糖酸錫、酒石酸錫、乳酸錫、琥珀酸錫、磺胺酸、硼氟化錫、矽氟化錫等的亞Sn化合物。該等的Sn化合物,可以一種單獨或混合兩種以上使用。
銅化合物,可舉上述有機磺酸之銅鹽、硫酸銅、氧化銅、硝酸銅、氯化銅、嗅化銅、碘化銅、磷酸銅、焦磷酸銅、醋酸銅、蟻酸銅、檸檬酸銅、葡糖酸銅、酒石酸銅、乳酸銅、琥珀酸銅、磺胺酸銅、硼氟化銅、矽氟化銅等。該等Cu化合物,可以一種單獨或混合兩種以上使用。
Ag化合物,可舉上述有機磺酸之銀鹽、硫酸銀、氧化銀、氯化銀、硝酸銀、嗅化銀、碘化銀、磷酸銀、焦磷酸銀、醋酸銀、蟻酸銀、檸檬酸銀、葡糖酸銀、酒石酸銀、乳酸銀、琥珀酸銀、磺胺酸銀、硼氟化銀、矽氟化銀等。該等Ag化合物,可以一種單獨或混合兩種以上使用。
此外,對直徑100μm的Cu球形成膜厚(單側)20μm的Sn-Ag-Cu焊料鍍敷披膜時,需要約0.0108庫倫的電量。
鍍敷液中的各金屬的調合量,Sn2+為0.21~2mol/L,以0.25~1mol/L為佳,Ag為0.01~0.1mol/L,以0.02~0.05mol/L為佳,Cu為0.002~0.02mol/L,以0.003~0.01mol/L為佳。在此,由於參與鍍敷的是Sn2+,故於本發明只要調整Sn2+的量即可。
此外,Ag離子濃度對Cu離子濃度(Ag/Cu莫耳比),以4.5~5.58的範圍為佳,於該範圍,則可形成如Sn-3Ag-0.5Cu合金等的熔點低的Sn-Ag-Cu鍍敷披膜。
再者,根據法拉第的電解法則,根據下式(1)估計所期望的
焊料鍍敷的析出量,算出電量,對鍍敷液通電流成算出之電量,使Cu球及鍍敷液流動進行鍍敷處理。鍍敷槽的容量可按照Cu球及鍍敷液的總投入量決定。
w(g)=(I×t×M)/(Z×F)...式(1)
式(1)中,w係電解析出量(g),I係電流(A),t係通電時間(秒),M係析出元素之原子量(Sn為118.71),z係原子價(Sn為2價),F係法拉第常數(96500庫倫),電量Q(A.秒)係以(I×t)表示。
於本發明,使Cu球及鍍敷液流動進行鍍敷,關於使之流動的方法,並無特別限定。例如,如筒式電鍍法,藉由筒的旋轉使Cu球及鍍敷液流動。
鍍敷處理後,於大氣中或N2氣氛中乾燥可得關於本發明之Cu核球。
此外,本發明,亦可應用於以Cu為管柱、柱或錠的形狀。
[實施例]
以下說明本發明之實施例,惟本發明並非限定於該等。於本實施例製作真球度高的Cu球,於該Cu球的比面形成焊料鍍敷披膜測定α射線量。
.Cu球的製作
調查製作真球度高的Cu球的條件。準備純度為99.9%的Cu錠、純度為99.995%以下的Cu線、及純度超過99.995%的銅板。分別投入坩鍋中之後,將坩鍋的溫度升溫至1200℃,進行45分鐘加熱處理,由設於坩鍋底部的孔使熔融Cu之液滴
滴下,將滴液冷卻將Cu球造粒。藉此,製作平均粒徑為250μm的Cu球。將製作之Cu球的元素分析結果及真球度示於第1表。以下,詳述真球度的測定方法。
.真球度
真球度係以CNC影像測定系統測定。裝置,係MITSUTOYO公司製之ULTRA QUICK VISION,ULTRA QV350-PRO。
此外,製作之各個Cu球的SEM照片示於第1~3圖。第1圖,係使用純度為99.9%的Cu錠製作之Cu球之SEM照片。第2圖係使用純度為99.995%以下的Cu線所製造的Cu球之SEM照片。第3圖係使用純度超過99.995%的Cu板所製造的Cu球之SEM照片。SEN照片的倍率為100倍。
α射線量的測定方法如下。
.α射線量
α射線量的測定係使用氣流比例計數器的α射線測定裝置。測定樣品係於300mm×300mm的平面淺底容器鋪滿Cu球者。將該測定樣品放入α射線測定裝置內,以PR-10氣流放置24小時後,測定α射線量。
再者,使用於測定之PR-10氣體(氬90%-甲烷10%),係將PR-10氣體填充於氣瓶經過3週以上者。經過3週以上的氣瓶,為不使進入氣瓶的大氣中的氡產生α射線,遵照JEDEC(Joint Electron Device Engineering Council)所訂定的α射線測定方法之指針。
將製作之Cu球之元素分析結果、α射線量示於第
1表。
如第1表、第1圖及第2圖所示,使用純度為99.9%的Cu錠及99.995%以下的Cu線之Cu球,均表示真球度為0.990以上。另一方面,如第1表及第3圖所示,使用純度超過99.995%的Cu板的Cu球,真球度低過0.95。因此,於以下所示實施例及比較例,均係使用99.9%的Cu錠製造之Cu球製作Cu核球。
實施例1
關於以純度99.9%的Cu錠所製造的Cu球,以如下條件形成Sn焊料鍍敷披膜製作Cu核球。
Cu核球,係以約0.17庫倫的電量,使用以下的鍍敷液進行鍍敷處理,於直徑250μm的Cu球披覆膜厚(單側)為50μm的焊料鍍敷。以SEM照片觀察以焊料鍍敷披膜披覆的Cu核球的剖面,膜厚約為50μm。
處理後,於大氣中乾燥,得到Cu核球。
焊料鍍敷液,係如下製作。
於攪拌容器,對調製鍍敷液所需的水的1/3,放入54重量%的甲基磺酸水溶液的全容作為敷液。其次,放入錯化劑之硫醇化合物之一例之乙醯半胱胺酸確認溶解後,放入其他的錯化劑之芳香族胺基化合物之一例之2,2’-二硫代二苯胺。變成薄淡藍色的凝膠狀的液體迅速地放入甲基磺酸亞錫。其次對鍍敷液加入必要的2/3,最後放入介面活性劑之一例之α-萘酚聚氧乙烯醚(EO10莫耳)3g/L,完成鍍敷液的調製。製作鍍敷液中的甲基磺酸的濃度為2.64mol/L,錫離子濃度為0.337mol/L之鍍敷液。使用於本例之甲基磺酸亞錫,係以下述Sn板片材作為
原料調製者。
焊料鍍敷液之原料之Sn板片材的元素分析,及形成於Cu核球的表面的焊料鍍敷披膜的元素分析,關於U及Th係以高頻耦合電漿質譜分析(ICP-MS分析),關於其他的元素係以高頻耦合電漿發射光譜分析(ICP-AES分析)進行。Sn板片材的α射線量,係於300mm×300mm的平面淺底容器鋪Sn板片材以外與Cu球做同樣的測定。Cu核球的α射線量,亦與上述Cu球做同樣的測定。此外,關於Cu核球的真球度,亦以與Cu球相同的條件進行測定。將該等的測定結果示於第2表。
實施例2
關於以純度99.9%的銅錠所製造的Cu球,形成膜厚(單側)為50μm的Sn-Ag-Cu焊料鍍敷披膜製作Cu核球。
於實施例2,焊料鍍敷液,係如下製作。
於攪拌容器,對調製鍍敷液所需的水的1/3,放入54重量%的甲基磺酸水溶液的全容作為敷液。其次,邊攪拌放入所需量的氧化銀之全容確認完全沒有黑沉而成為透明後,迅速地放入氫氧化銅的全容完全溶解,放入錯化劑之硫醇化合物之一例之乙醯半胱胺酸確認溶解後,放入其他的錯化劑之芳香族胺基化合物之一例之2,2’-二硫代二苯胺。變成薄淡藍色的凝膠狀的液體迅速地放入甲基磺酸亞錫。液變成黃色透明。其次對鍍敷液加入必要的2/3,最後放入介面活性劑之一例之α-萘酚聚氧乙烯醚(EO10莫耳)3g/L,完成鍍敷液的調製。製作鍍敷液中的甲基磺酸的濃度為2.64mol/L,錫離子濃度為0.337mol/L、銅離子濃度為0.005mol/L、銀離子濃度為0.0237mol/L、之鍍
敷液。
如此地製作鍍敷液之後,使用於實施例1使用之α射線量為0.203cph/cm2的Sn板片材,α射線量為<0.0010cph/cm2,純度為6N的Cu板材及α射線量為<0.0010cph/cm2,純度為5N之Ag薄片材之外,以與實施例1同樣地製作鍍敷液製作Cu核球,進行元素分析及α射線量、真球度的測定。將測定結果,示於第2表。
於本例錫離子亦係來自上述Sn板片材者,關於銀離子、銅離子,係分別來自上述Ag薄片材、Cu板材者。
比較例1
關於以純度99.9%的Cu錠所製造的Cu球,使用熔接法以如下條件形成Sn焊料披膜製作Cu核球。具體而言,於難以焊接的鋁板的既定的位置設置多數研缽狀的凹陷。此外,使用上述Sn板片材,藉由已知的噴霧法預先製作直徑為300μm的Sn球。於設於鋁基板的各凹陷,各放1個Cu球及Sn球,將助熔劑噴霧。之後,將鋁板於加熱爐中加熱為270℃使Sn球熔融。熔融Sn於Cu球的周圍沾濕,藉由表面張力披覆Cu球。如此地製作比較例1之Cu核球。焊料披膜的膜厚(單側)為50μm。關於製作的Cu核球,與實施例1同樣地,測定元素分析、α射線量及真球度。將測定結果示於第2表。
[第2表]
根據第2表,於實施例1,α射線量顯示未滿0.0010cph/cm2。實施例1之Cu核球,證明可藉由鍍敷法形成焊料鍍敷披膜可減低α射線量。
於實施例2,使焊料鍍敷披膜的組成為Sn-2.95Ag-0.29Cu時,α射線量顯示未滿0.0010cph/cm2。實施例2之Cu核球,與實施例1同樣地,證明可藉由鍍敷法形成焊料鍍敷披膜可減低α射線量。
此外於實施例1、實施例2所製作之Cu核球之α射線量,即使於製作後經過1年,並沒有看到α射線的上昇。另一方面,於比較例1,α射線量顯示0.183cph/cm2,顯示與Sn板片材同程度的α射線量。因此,比較例1的Cu核球,並沒有達至可迴避軟錯誤的程度的α射線量。
Claims (8)
- 一種Cu核球,包括:Cu球;及披覆於該Cu球的表面之焊料鍍敷披膜之Cu核球,其特徵在於:上述焊料鍍敷披膜,係Sn焊料鍍敷披膜或以Sn為主成分的無Pb焊料合金所構成之焊料鍍敷披膜,U的含量為5ppb以下,Th的含量為5ppb以下,該Cu球的純度為99.9%以上99.995%以下,Pb及/或Bi的含量的合計量為1ppm以上,真球度為0.95以上,然後,Cu核球的α射線量為0.0200cph/cm2以下。
- 根據申請專利範圍第1項之Cu核球,其中上述Cu核球的α射線量為0.0020cph/cm2以下。
- 根據申請專利範圍第1項之Cu核球,其中上述Cu核球的α射線量為0.0010cph/cm2以下。
- 根據申請專利範圍第1至3項中任一項之Cu核球,其中上述Cu球中的Pb及Bi的含量合計為1ppm以上。
- 根據申請專利範圍第1至4項中任一項之Cu核球,其直徑為1~1000μm。
- 根據申請專利範圍第1至5項中任一項之Cu核球,其中上述Cu球,在以上述焊料鍍敷披膜披覆之前預先以選自由Ni及Co之1元素以上所組成的鍍敷層披覆。
- 根據申請專利範圍第1至6項中任一項之Cu核球,其中上述Cu核球的真球度為0.95以上。
- 一種接點,使用申請專利範圍第1至7項中任一項之Cu核 球所形成。
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