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TW201637152A - Heat sink substrate - Google Patents

Heat sink substrate Download PDF

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TW201637152A
TW201637152A TW104144737A TW104144737A TW201637152A TW 201637152 A TW201637152 A TW 201637152A TW 104144737 A TW104144737 A TW 104144737A TW 104144737 A TW104144737 A TW 104144737A TW 201637152 A TW201637152 A TW 201637152A
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Taiwan
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layer
metal
thickness
heat dissipation
heat
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TW104144737A
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Chinese (zh)
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宇野智裕
小山田哲哉
橋野英兒
石川信二
澤野清志
津島榮樹
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新日鐵住金高新材料股份有限公司
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    • H10W40/10

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  • Laminated Bodies (AREA)

Abstract

一種交互積層Cu層及由金屬A構成之金屬A層而成的矩形散熱基板,其中前述Cu層及前述金屬A層合計積層5或9層,並且前述金屬A層之前述散熱基板長邊方向的平均結晶粒長度L與厚度方向的平均結晶粒長度t的比L/t係1.5至10,且長邊方向的前述平均結晶粒長度L與前述金屬A層之前述散熱基板寬度方向的平均結晶粒長度d的比L/d係1.2至7,藉由上述特徵可提供可提高長期可靠性之散熱基板。 A rectangular heat dissipation substrate formed by alternately stacking a Cu layer and a metal A layer made of a metal A, wherein the Cu layer and the metal A layer are a total of 5 or 9 layers, and the heat dissipation substrate of the metal layer A has a longitudinal direction The ratio L/t of the average crystal grain length L to the average crystal grain length t in the thickness direction is 1.5 to 10, and the average crystal grain length L in the longitudinal direction and the average crystal grain in the width direction of the heat dissipation substrate of the metal A layer. The ratio d of the length d is from 1.2 to 7, and the above features provide a heat-dissipating substrate which can improve long-term reliability.

Description

散熱基板 Heat sink substrate 技術領域 Technical field

本發明係有關於散熱基板,特別有關於適用於電 力模組之散熱基板。 The invention relates to a heat dissipating substrate, in particular to an electric device The heat sink substrate of the force module.

背景技術 Background technique

電動車、油電混合車及風力發電等使用電力模組作為電力控制用之零件。電力模組接合由陶瓷形成之絕緣基板及由金屬形成之散熱基板,同時透過接合材硬焊半導體裝置,特別是藉大電力動作之LSI、IC、功率電晶體等。藉大電力動作之半導體裝置在使用時產生熱。 Power modules such as electric vehicles, hybrid electric vehicles, and wind power generation are used as components for power control. The power module is bonded to an insulating substrate made of ceramics and a heat-dissipating substrate formed of metal, and the semiconductor device is brazed through the bonding material, in particular, an LSI, an IC, a power transistor, or the like that operates by a large power. A semiconductor device that operates with a large power generates heat when it is used.

散熱基板需要使由該等半導體裝置產生之熱更有效率地擴散、散熱。然而,如上所述,由於電力模組係由不同種材料構成之接合體,不僅在製造時,在使用時亦會因溫度變化產生內部應力。由於該內部應力,有散熱基板變形之問題。因此,散熱基板最好具有高機械強度及高熱傳導率。 The heat dissipation substrate needs to diffuse and dissipate heat generated by the semiconductor devices more efficiently. However, as described above, since the power module is a bonded body composed of different kinds of materials, internal stress is generated not only at the time of manufacture but also due to temperature change during use. Due to this internal stress, there is a problem that the heat dissipation substrate is deformed. Therefore, the heat dissipation substrate preferably has high mechanical strength and high thermal conductivity.

相對於此,例如,在專利文獻1中揭示依序積層Cu層、Mo層、Cu層之包覆材作為由3層構造構成之散熱基 板。藉由使該3層構造之包覆材中的Mo體積比在20%至99.6%之範圍內變化,可控制熱傳導率及熱膨脹係數,且獲得比Mo單體高之熱傳導率及比Cu單體小之熱膨脹係數。 On the other hand, for example, Patent Document 1 discloses a coating material in which a Cu layer, a Mo layer, and a Cu layer are sequentially laminated as a heat dissipation base composed of a three-layer structure. board. By changing the Mo volume ratio in the three-layered cladding material in the range of 20% to 99.6%, the thermal conductivity and the thermal expansion coefficient can be controlled, and the thermal conductivity and the specific Cu ratio higher than that of the Mo monomer can be obtained. Small thermal expansion coefficient.

此外,專利文獻2中揭示依序積層Cu層、Mo層、Cu層之3層構造包覆材的熱膨脹係數與Cu體積比的關係。在該構造之包覆材中,Mo層為1層時,為了例如使熱膨脹係數為12×10-6/K以下,熱傳導率低之Mo使用量必須為整體質量的20%以上。因此,該包覆材之厚度方向的熱傳導率為大約230W/(m.K)。 Further, Patent Document 2 discloses a relationship between a thermal expansion coefficient and a Cu volume ratio of a three-layer structure cladding material in which a Cu layer, a Mo layer, and a Cu layer are sequentially laminated. In the case of the cladding material of this structure, when the Mo layer is one layer, in order to have, for example, a thermal expansion coefficient of 12 × 10 -6 /K or less, the amount of Mo used having a low thermal conductivity must be 20% or more of the total mass. Therefore, the thermal conductivity of the cladding material in the thickness direction is about 230 W/(m.K).

另外,專利文獻3中揭示Cu層及Mo層交互積層5層以上之包覆材。在此情形中,藉由積層5層以上,可製得熱膨脹係數更小,且熱傳導率更高之包覆材。 Further, Patent Document 3 discloses a cladding material in which five or more layers of a Cu layer and a Mo layer are alternately laminated. In this case, by laminating 5 or more layers, a cladding material having a smaller thermal expansion coefficient and a higher thermal conductivity can be obtained.

先前技術文獻 Prior technical literature 專利文獻 Patent literature

專利文獻1:日本特開平2-102551號公報 Patent Document 1: Japanese Laid-Open Patent Publication No. 2-102551

專利文獻2:日本特開平6-268115號公報 Patent Document 2: Japanese Laid-Open Patent Publication No. Hei 6-268115

專利文獻3:日本特開2007-115731號公報 Patent Document 3: Japanese Laid-Open Patent Publication No. 2007-115731

發明概要 Summary of invention

然而,仍需要可因應對電力模組大電力化之要求的可靠性更高的散熱基板。特別受到注目的是積層Cu層與Mo層之層間、及安裝接合在散熱基板上之半導體裝置後等 的長期可靠性。由於藉由散熱基板接合熱膨脹係數不同之Si、SiC等之半導體裝置及陶瓷基板上的銅電極,在熱循環試驗時施加熱應力,因此有在散熱基板之層間產生裂縫及空孔等缺陷,且在半導體裝置中產生裂縫的問題。由於產生該等缺陷,有接合強度降低及熱傳導降低等之不良、半導體裝置故障的問題。 However, there is still a need for a more reliable heat dissipation substrate that can cope with the demand for power module power. Particularly noticeable is the lamination of the layers between the Cu layer and the Mo layer, and after mounting the semiconductor device bonded to the heat dissipation substrate. Long-term reliability. Since a semiconductor device such as Si or SiC having a different thermal expansion coefficient and a copper electrode on a ceramic substrate are bonded by a heat dissipation substrate, thermal stress is applied during a thermal cycle test, and thus defects such as cracks and voids are formed between the layers of the heat dissipation substrate. A problem of cracks occurring in a semiconductor device. Due to such defects, there is a problem that the bonding strength is lowered and the heat conduction is lowered, and the semiconductor device is defective.

因此本發明之目的在於提供可進一步提高長期可靠性之散熱基板。 Therefore, an object of the present invention is to provide a heat dissipation substrate which can further improve long-term reliability.

本發明之散熱基板係交互積層Cu層及由金屬A構成之金屬A層而成的矩形散熱基板,其特徵在於:前述Cu層及前述金屬A層合計積層5或9層,且前述金屬A層之前述散熱基板長邊方向的平均結晶粒長度L與厚度方向的平均結晶粒長度t的比(L/t)係1.5至10.0,並且長邊方向的前述平均結晶粒長度L與前述金屬A層之前述散熱基板寬度方向的平均結晶粒長度d的比(L/d)係1.2至7.0。 The heat dissipation substrate of the present invention is a rectangular heat dissipation substrate in which a Cu layer and a metal A layer made of a metal A are alternately laminated, wherein the Cu layer and the metal A layer are stacked in a stack of 5 or 9 layers, and the metal layer A The ratio (L/t) of the average crystal grain length L in the longitudinal direction of the heat dissipation substrate to the average crystal grain length t in the thickness direction is 1.5 to 10.0, and the average crystal grain length L in the longitudinal direction and the aforementioned metal A layer The ratio (L/d) of the average crystal grain length d in the width direction of the heat dissipation substrate is 1.2 to 7.0.

依據本發明,由於使散熱基板之結晶粒長度的平均縱橫比(L/t)、(L/d)大,可抑制在層間產生裂縫,並且可抑制在晶片間產生裂縫,因此可進一步提高長期可靠性。 According to the present invention, since the average aspect ratio (L/t) and (L/d) of the crystal grain length of the heat dissipating substrate are large, cracks can be suppressed from occurring between the layers, and cracks can be suppressed from occurring between the wafers, so that the long-term increase can be further improved. reliability.

10‧‧‧散熱基板 10‧‧‧heated substrate

12A,12B‧‧‧Cu層 12A, 12B‧‧‧Cu layer

14‧‧‧金屬A層 14‧‧‧Metal A layer

18‧‧‧結晶粒 18‧‧‧ crystal grain

d‧‧‧寬度方向之平均長度 d‧‧‧Average length in the width direction

L‧‧‧長邊方向之平均長度 L‧‧‧Average length in the long-side direction

t‧‧‧厚度方向之平均長度 t‧‧‧Average length in the thickness direction

X‧‧‧長邊方向 X‧‧‧Longside direction

Y‧‧‧寬度方向 Y‧‧‧Width direction

Z‧‧‧厚度方向 Z‧‧‧ Thickness direction

圖式之簡單說明 Simple description of the schema

圖1係顯示本實施形態之散熱基板結構的縱截面圖。 Fig. 1 is a longitudinal sectional view showing the structure of a heat dissipation substrate of the embodiment.

圖2顯示本實施形態之散熱基板結構的立體圖。 Fig. 2 is a perspective view showing the structure of the heat dissipation substrate of the embodiment.

圖3顯示本實施形態之散熱基板長邊方向金屬A層的截面示意圖。 Fig. 3 is a schematic cross-sectional view showing the metal layer A in the longitudinal direction of the heat dissipation substrate of the embodiment.

圖4顯示本實施形態之散熱基板寬度方向金屬A層的截面示意圖。 Fig. 4 is a schematic cross-sectional view showing the metal layer A in the width direction of the heat dissipation substrate of the embodiment.

用以實施發明之形態 Form for implementing the invention

以下,參照圖式詳細說明本發明之實施形態。 Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

1.實施形態 1. Implementation

(1)整體結構 (1) Overall structure

如圖1所示地,本實施形態之散熱基板10係交互積層5或9層之Cu層12A、12B及由金屬A構成之金屬A層14而成。在本圖之情形中,Cu層12A、12B及金屬A層14合計積層有5層。金屬A可使用低熱膨脹率材料之Mo或W。如圖2所示地,散熱基板10係以矩形板狀構成。在本圖中,長邊方向為X、寬度方向為Y、厚度方向為Z。散熱基板10,雖然未圖示,但例如在一側表面上使用晶粒附接材作為接合材接合半導體裝置(以下,亦稱為晶片),並在另一側表面上使用硬焊材接接合絕緣基板。 As shown in Fig. 1, the heat dissipation substrate 10 of the present embodiment is formed by alternately stacking 5 or 9 layers of Cu layers 12A and 12B and a metal A layer 14 made of metal A. In the case of this figure, the Cu layers 12A, 12B and the metal A layer 14 have a total of five layers. Metal A can use Mo or W of a low thermal expansion material. As shown in FIG. 2, the heat dissipation substrate 10 is formed in a rectangular plate shape. In the figure, the longitudinal direction is X, the width direction is Y, and the thickness direction is Z. The heat-dissipating substrate 10 is bonded to a semiconductor device (hereinafter, also referred to as a wafer) using a die attach material as a bonding material on one surface, for example, and is joined by a hard solder material on the other side surface. Insulating substrate.

(結晶粒徑) (crystal size)

金屬A層14,如圖3所示地,金屬A之結晶粒18之散熱基板10之長邊方向X的平均長度L比厚度方向Z的平均長度t大,即金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)大。因此,金屬A層14藉由加熱可同時抑制鄰接Cu層12A、12B 產生之熱膨脹及因冷卻產生之熱收縮。具體而言,金屬A層會因長邊方向X之平均長度大,而往長邊方向X彈性變形。依此,吾人推測金屬A層14會隨著Cu因加熱產生之熱膨脹而彈性變形,而可維持Cu層12A、12B與金屬A層14之間(以下亦稱為「層間」)的密接性。此外,金屬A層14藉由控制冷卻時之Cu層12A、12B的熱收縮,可維持Cu層12A、12B與金屬A層14之層間的密接性,並且抑制在層間產生裂縫。 As shown in FIG. 3, the metal A layer 14 has an average length L of the longitudinal direction X of the heat dissipation substrate 10 of the crystal grains 18 of the metal A larger than the average length t of the thickness direction Z, that is, the crystal grain 18 of the metal A layer 14. The average aspect ratio (L/t) of the long side/plate thickness is large. Therefore, the metal A layer 14 can simultaneously suppress the adjacent Cu layers 12A, 12B by heating. Thermal expansion and heat shrinkage due to cooling. Specifically, the metal A layer is elastically deformed in the longitudinal direction X due to the large average length of the longitudinal direction X. Accordingly, it is assumed that the metal A layer 14 is elastically deformed in accordance with thermal expansion of Cu due to heating, and the adhesion between the Cu layers 12A and 12B and the metal A layer 14 (hereinafter also referred to as "interlayer") can be maintained. Further, the metal A layer 14 can maintain the adhesion between the layers of the Cu layers 12A, 12B and the metal A layer 14 by controlling the heat shrinkage of the Cu layers 12A, 12B during cooling, and suppress the occurrence of cracks between the layers.

金屬A由於低熱膨脹率,抑制Cu層12A、12B之熱變形的效果高。另一方面,由於金屬A之熱膨脹率與Cu有很大差異,其熱膨脹率之差會成為在層間產生裂縫之原因。在本實施形態之情形中,藉由使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為1.5以上,可緩和層間及Cu層12A、12B內的熱應力。藉由使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為1.5以上,在使用高溫焊料作為晶粒附接材時之條件嚴格的熱循環中,可抑制層間之裂縫,因此可獲得高可靠性。在金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)小於1.5之情況下無法充分地抑制在Cu層12A、12B產生之加熱的熱膨脹及冷卻的熱收縮,因此無法抑制層間之裂縫成長。此外,若金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)超過10.0,則抑制層間之裂縫成長的效果飽和。金屬A層14之結晶粒18之長邊方向X的平均長度L及厚度方向的平均長度t係在包含長邊方向X及厚度方向Z之金屬A層14的截面中藉由電子束反向散射繞射法(EBSD:Electron Backscatter Diffraction)進行觀察, 並藉由分析軟體算出結晶粒18之厚度方向截面的平均大小的值。 The metal A has a high effect of suppressing thermal deformation of the Cu layers 12A and 12B due to a low coefficient of thermal expansion. On the other hand, since the thermal expansion coefficient of the metal A is greatly different from that of Cu, the difference in thermal expansion rate causes a crack between the layers. In the case of the present embodiment, by making the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 1.5 or more, the heat in the interlayer and the Cu layers 12A and 12B can be alleviated. stress. By setting the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 to 1.5 or more, in the case of using a high temperature solder as a die attaching material, the condition is strict thermal cycle. Cracks between the layers are suppressed, so high reliability can be obtained. When the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 is less than 1.5, the thermal expansion of the heating generated by the Cu layers 12A and 12B and the heat shrinkage of the cooling cannot be sufficiently suppressed. Therefore, it is impossible to suppress the crack growth between the layers. Further, when the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 exceeds 10.0, the effect of suppressing crack growth between the layers is saturated. The average length L of the longitudinal direction X of the crystal grains 18 of the metal A layer 14 and the average length t in the thickness direction are backscattered by electron beams in the cross section of the metal A layer 14 including the longitudinal direction X and the thickness direction Z. Observing by EBSD: Electron Backscatter Diffraction, The value of the average size of the cross section in the thickness direction of the crystal grains 18 was calculated by analyzing the software.

此外,如圖4所示地,金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為1.5至10.0,且金屬A層14之結晶粒18之散熱基板10之長邊方向X的平均長度L比寬度方向Y的平均長度d大,即金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)大,因此可抑制散熱基板10整體之熱變形,以減輕對搭載在散熱基板10上之晶片的破壞。這可考慮是因為藉由使長邊/寬度的平均縱橫比(L/d)大,可減少鄰接Cu層12A、12B產生之熱膨脹及熱收縮造成的變形,並且減少長邊方向X之金屬A層14的熱應變,因此可進一步提高強度、延展性。 Further, as shown in FIG. 4, the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 is 1.5 to 10.0, and the heat dissipation substrate 10 of the crystal grains 18 of the metal A layer 14 is provided. The average length L of the longitudinal direction X is larger than the average length d of the width direction Y, that is, the average aspect ratio (L/d) of the long side/width of the crystal grains 18 of the metal A layer 14 is large, so that the heat dissipation substrate 10 can be suppressed. The overall thermal deformation is to reduce the damage to the wafer mounted on the heat dissipation substrate 10. This is considered because by making the average aspect ratio (L/d) of the long side/width large, deformation due to thermal expansion and thermal contraction generated by the adjacent Cu layers 12A, 12B can be reduced, and metal A in the long-side direction X can be reduced. The thermal strain of the layer 14 can further increase the strength and ductility.

即,散熱基板10其藉由使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為1.5至10.0,且金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)為1.2至7.0,則金屬A層14可有效地抑制Cu層12A、12B之熱膨脹及熱收縮造成的熱變形。因此,散熱基板10可抑制在層間產生裂縫,並減少晶片受到之破壞,可進一步提高晶片與散熱基板10之接著性,因此可進一步提高長期可靠性。 That is, the heat dissipation substrate 10 has an average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 of 1.5 to 10.0, and the long side of the crystal grain 18 of the metal A layer 14/ The average aspect ratio (L/d) of the width is 1.2 to 7.0, and the metal A layer 14 can effectively suppress thermal deformation caused by thermal expansion and thermal contraction of the Cu layers 12A, 12B. Therefore, the heat dissipation substrate 10 can suppress cracks between the layers and reduce the damage of the wafer, and can further improve the adhesion between the wafer and the heat dissipation substrate 10, thereby further improving long-term reliability.

藉由使金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)為1.2以上,在溫差嚴格之熱循環條件下,可藉由減少散熱基板10之翹曲等抑制晶片產生裂縫,因此可獲得高可靠性。在金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)小於1.2之情況下無法充分地抑制加熱、冷卻 時之Cu層12A、12B的熱變形,因此無法抑制晶片產生裂縫。此外,若(L/d)超過7,則加工、切斷以製作散熱基板10時之產率降低,有生產性降低之問題。金屬A層14之結晶粒18之寬度方向Y的平均長度d及厚度方向Z之平均長度d係在包含長邊方向及厚度方向之金屬A層14的截面中藉由EBSD進行觀察,並藉由分析軟體算出結晶粒18之寬度方向截面的平均大小的值。 By making the average aspect ratio (L/d) of the long side/width of the crystal grains 18 of the metal A layer 14 1.2 or more, it is possible to reduce the warpage of the heat dissipation substrate 10, etc. under the thermal cycle conditions where the temperature difference is severe. The wafer is cracked, so high reliability can be obtained. When the average aspect ratio (L/d) of the long side/width of the crystal grains 18 of the metal A layer 14 is less than 1.2, heating and cooling cannot be sufficiently suppressed. At the time, the Cu layers 12A and 12B are thermally deformed, so that cracks in the wafer cannot be suppressed. In addition, when (L/d) exceeds 7, the yield when processing and cutting to produce the heat-dissipating substrate 10 is lowered, and there is a problem that productivity is lowered. The average length d of the width direction Y of the crystal grains 18 of the metal A layer 14 and the average length d of the thickness direction Z are observed by EBSD in the cross section of the metal A layer 14 including the longitudinal direction and the thickness direction, and by The analysis software calculates the value of the average size of the cross section of the crystal grains 18 in the width direction.

如上所述之金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為1.5至10.0,且金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)為1.2至7.0的效果可藉由重複進行500次比現行可靠性試驗之-40℃/175℃熱循環嚴格的-40℃/200℃熱循環試驗後觀察層間裂縫及重複進行500次-40℃/225℃熱循環試驗後觀察晶片裂縫,作為熱循環之試驗條件的一例來進行評價。 The average aspect ratio (L/t) of the long side/thickness of the crystal grain 18 of the metal A layer 14 as described above is 1.5 to 10.0, and the average aspect ratio of the long side/width of the crystal grain 18 of the metal A layer 14 is as follows. The effect of (L/d) of 1.2 to 7.0 can be observed by repeating 500 times of the -40 ° C / 175 ° C thermal cycle after the current reliability test - 40 ° C / 200 ° C thermal cycle test to observe the interlaminar cracks and repeat The wafer crack was observed after 500 cycles of -40 ° C / 225 ° C heat cycle test, and was evaluated as an example of the test conditions of the heat cycle.

較佳地,藉由使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為2.0以上,即使更長時間之熱循環亦可提高可靠性,且即使重複進行500次-40℃/225℃熱循環試驗後,亦可獲得抑制層間裂縫之效果。 Preferably, by making the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 2.0 or more, even a longer thermal cycle can improve reliability, and even if it is repeated After 500 cycles of -40 ° C / 225 ° C thermal cycle test, the effect of suppressing interlayer cracks can also be obtained.

更佳地,藉由使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為3.0以上,即使在假設SiC晶片等之高溫安裝之嚴格條件下的熱循環中亦可獲得高度抑制層間裂縫之效果。使用於如上所述之高溫安裝方面時的效果可藉由以重複進行1000次-40℃/225℃作為熱循環試驗條件的試驗來進行評價。 More preferably, by making the average aspect ratio (L/t) of the long side/thickness of the crystal grains 18 of the metal A layer 14 3.0 or more, the thermal cycle is performed under strict conditions such as assuming high temperature mounting of a SiC wafer or the like. The effect of highly inhibiting interlayer cracks can also be obtained. The effect when used in the high-temperature mounting aspect as described above can be evaluated by a test which repeats 1000 times -40 ° C / 225 ° C as a heat cycle test condition.

此外,較佳地,若金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)在2.0至7.0之範圍內,即使重複進行1000次-40℃/225℃之熱循環試驗後,亦可獲得高度抑制晶片產生裂縫之效果。 Further, preferably, if the average aspect ratio (L/d) of the long side/width of the crystal grains 18 of the metal A layer 14 is in the range of 2.0 to 7.0, even if 1000 times of heat of -40 ° C / 225 ° C is repeated. After the cycle test, the effect of highly inhibiting the cracking of the wafer can also be obtained.

(Cu層厚度) (Cu layer thickness)

若配置在表面之前述Cu層12B的厚度H1與配置在中央之前述Cu層12A的厚度H2的比(H1/H2)在0.2至0.9之範圍內,則在將晶片硬焊於散熱基板10上之安裝後的可靠性試驗中,可減少硬焊材內之空隙及晶片內之裂縫等的損傷。藉由令表面側之前述Cu層12B的厚度H1為薄,可減輕在加熱、冷卻過程中產生之Cu的伸長、收縮,以減輕施加在硬焊材及晶片上之應力。 If the ratio (H 1 /H 2 ) of the thickness H 1 of the Cu layer 12B disposed on the surface to the thickness H 2 of the Cu layer 12A disposed at the center is in the range of 0.2 to 0.9, the wafer is brazed to In the reliability test after mounting on the heat dissipation substrate 10, damage in the voids in the brazing material and cracks in the wafer can be reduced. By making the thickness H 1 of the aforementioned Cu layer 12B on the surface side thin, the elongation and contraction of Cu generated during heating and cooling can be alleviated to reduce the stress applied to the hard solder material and the wafer.

即,藉由使金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)為1.2以上,且進一步使Cu層之厚度H2的比(H1/H2)在0.2至0.9之範圍內,可在連接於散熱基板10之晶片的可靠性試驗中獲得高度抑制硬焊材之空隙或晶片產生之裂縫的效果。藉由H1/H2之適性化,可特別確認比裂縫小之以外力產生的空隙在硬焊材內減少。即使在作為具體例之重複進行500次-40℃/225℃的熱循環試驗後,亦可獲得抑制在硬焊材內產生空隙的效果。 That is, the average aspect ratio (L/d) of the long side/width of the crystal grains 18 of the metal A layer 14 is 1.2 or more, and the ratio (H 1 /H 2 ) of the thickness H 2 of the Cu layer is further made In the range of 0.2 to 0.9, it is possible to obtain an effect of highly suppressing the void of the hard-weld material or the crack generated by the wafer in the reliability test of the wafer connected to the heat-dissipating substrate 10. By the suitability of H 1 /H 2 , it is particularly confirmed that voids generated by forces other than cracks are reduced in the brazing material. Even after repeating the heat cycle test of -40 ° C / 225 ° C for 500 times as a specific example, the effect of suppressing generation of voids in the brazing material can be obtained.

散熱基板10藉由使配置於表面之前述Cu層12B的厚度H1及與前述Cu層12B連接之前述金屬A層14的厚度H3的比(H1/H3)為2.0至8.0,可抑制在晶片及未安裝在絕緣基板上之單體的高溫加熱中,因散熱基板10整體之熱變形 產生的翹曲。由於可抑制翹曲,結果,在為了藉硬焊材接合晶片及散熱基板10而在大約800℃之高溫下加熱的步驟中,可抑制在硬焊材與散熱基板10之間產生間隙,藉此可進一步提高密接性而提高可靠性。即使在作為具體例之對散熱基板10單體由常溫加熱至800℃並保持5分鐘後冷卻,可減少散熱基板單體之翹曲,結果因此獲得提高與晶片之密接性的效果。 The heat dissipation substrate 10 has a ratio (H 1 /H 3 ) of the thickness H 1 of the Cu layer 12B disposed on the surface and the thickness H 3 of the metal layer 14 connected to the Cu layer 12B of 2.0 to 8.0. The warpage caused by thermal deformation of the entire heat dissipation substrate 10 during high-temperature heating of the wafer and the monomer not mounted on the insulating substrate is suppressed. Since the warpage can be suppressed, as a result, in the step of heating at a high temperature of about 800 ° C in order to bond the wafer and the heat dissipation substrate 10 by the brazing material, it is possible to suppress generation of a gap between the hard solder material and the heat dissipation substrate 10, whereby The adhesion can be further improved to improve reliability. Even if the heat radiating substrate 10 is cooled by a normal temperature to 800 ° C and kept for 5 minutes as a specific example, the warpage of the heat radiating substrate can be reduced, and as a result, the effect of improving the adhesion to the wafer can be obtained.

藉由使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)為1.5以上,且使表面Cu層12B之厚度H1與中央Cu層12A之厚度H2的比(H1/H2)為0.2至0.9,進一步使表面Cu層12B之厚度H1及與前述Cu層12B連接之金屬A層14的厚度H3的比(H1/H3)為2.0至8.0,可進一步提高抑制散熱基板10之翹曲的效果。這是因為若比(H1/H3)為2.0以上,可提高熱傳導性而緩和熱應變之局部集中的緣故。此外,若比(H1/H3)超過8.0,則表面之Cu層12B熱膨脹之熱變形大,因此對晶片造成之破壞大。 A metal layer by crystal grains 14 of the longitudinal / thickness of 18 average aspect ratio (L / t) of 1.5 or more, and that the surface of the Cu layer thicknesses H 1 and 12B of the central thickness of the Cu layer 12A of the H 2 The ratio (H 1 /H 2 ) is 0.2 to 0.9, and the ratio (H 1 /H 3 ) of the thickness H 1 of the surface Cu layer 12B and the thickness H 3 of the metal A layer 14 connected to the Cu layer 12B is further 2.0. Up to 8.0, the effect of suppressing the warpage of the heat dissipation substrate 10 can be further improved. This is because if the ratio (H 1 /H 3 ) is 2.0 or more, the thermal conductivity can be improved and the local concentration of the thermal strain can be alleviated. Further, when the ratio (H 1 /H 3 ) exceeds 8.0, the thermal deformation of the Cu layer 12B on the surface is large, and the damage to the wafer is large.

(合金層) (alloy layer)

在Cu層12A、12B及金屬A層14之間形成有由Cu及金屬A構成之合金層。合金層係含有1至10at%之Cu及金屬A的區域。在此,合金層之濃度為1至10at%的原因是若在該濃度範圍內則合金之強度高,可期待提高Cu層12A、12B與金屬A層14之密接性的效果。 An alloy layer made of Cu and metal A is formed between the Cu layers 12A and 12B and the metal A layer 14. The alloy layer contains a region of 1 to 10 at% of Cu and metal A. Here, the reason why the concentration of the alloy layer is 1 to 10 at% is that the strength of the alloy is high in the concentration range, and the effect of improving the adhesion between the Cu layers 12A and 12B and the metal A layer 14 can be expected.

層間中央之Cu及金屬A濃度各為50at%的位置稱為接合界面。合金層與Cu層12A、12B或金屬A層14之邊界 為濃度變化小於1at%之位置。即,金屬A之濃度自接合界面朝向Cu層12A、12B減少,且金屬A濃度開始小於1at%之位置為合金層與Cu層12A、12B之邊界。同樣地,Cu之濃度自接合界面朝向金屬A層14減少,且Cu濃度開始小於1at%之位置為合金層與金屬A層14之邊界。即使由濃度化開始小於1at%之位置在Cu層12A、12B或金屬A層14側之濃度變化再成為1at%以上,亦不改變以前述位置作為合金層與Cu層12A、12B或金屬A層14之邊界。 The position where the concentration of Cu and metal A in the center of the interlayer is 50 at% each is called a joint interface. The boundary between the alloy layer and the Cu layer 12A, 12B or the metal A layer 14 It is a position where the concentration changes by less than 1 at%. That is, the concentration of the metal A decreases from the bonding interface toward the Cu layers 12A and 12B, and the position at which the metal A concentration starts to be less than 1 at% is the boundary between the alloy layer and the Cu layers 12A and 12B. Similarly, the concentration of Cu decreases from the bonding interface toward the metal A layer 14, and the position at which the Cu concentration starts to be less than 1 at% is the boundary between the alloy layer and the metal A layer 14. Even if the concentration change at the side of the Cu layer 12A, 12B or the metal A layer 14 is 1 at% or more from the position where the concentration starts less than 1 at%, the above position is not changed as the alloy layer and the Cu layer 12A, 12B or the metal A layer. The boundary of 14.

合金層由於低濃度且薄,組成分析最好是進行縱截面之穿透式電子顯微鏡(TEM:Transmission Electron Microscope)裝置之能量色散型X射線分析(EDS:Energy dispersive X-ray spectrometry)。該方法極適合在數nm級之微細區域中數at%之低濃度的組成分析。 Since the alloy layer is low in concentration and thin, the composition analysis is preferably an energy dispersive X-ray spectrometry (EDS) of a longitudinal section of a transmission electron microscope (TEM). This method is highly suitable for composition analysis of low concentrations of several at% in fine areas of several nm.

實際上,使用附屬於TEM裝置上之EDS裝置,接合界面居間地朝Cu層12A、12B及金屬A層14的厚度方向進行點分析。進行分析之範圍係在接合界面居間地朝Cu層12A、12B及金屬A層14的厚度方向,大約500至1000nm之範圍內。由於在自接合界面沿Cu層12A、12B及金屬A層14的厚度方向0至30nm之狹窄範圍內濃度急劇變化,點分析以2nm間隔詳細地進行分析,而由於在超過30nm之區域濃度變化小,點分析以10nm間隔進行。 Actually, the EDS device attached to the TEM device was used, and the bonding interface was subjected to dot analysis in the thickness direction of the Cu layers 12A and 12B and the metal A layer 14 in the middle. The analysis is performed in the range of the thickness of the Cu layers 12A, 12B and the metal A layer 14 in the thickness direction of the bonding interface, in the range of about 500 to 1000 nm. Since the concentration sharply changes in the narrow range of 0 to 30 nm in the thickness direction of the Cu layers 12A, 12B and the metal A layer 14 from the bonding interface, the dot analysis is analyzed in detail at intervals of 2 nm, and the concentration changes little in the region exceeding 30 nm. The point analysis was performed at intervals of 10 nm.

每一試料之測量數最好為3處以上。若測量數為3處以上,可確認再現性。在本實施形態之情形中,最好在4處之層間中,在2處以上之不同層間進行測量。 The number of measurements per sample is preferably three or more. If the number of measurements is three or more, the reproducibility can be confirmed. In the case of the present embodiment, it is preferable to measure between two different layers in the four layers.

在本實施形態之情形中,前述合金層之厚度總計為30至400nm。在此,「合金層之厚度總計」係在散熱基板10之多數層間中的一層間,以接合界面居間而形成在兩側的合金層總和。藉由使形成在Cu層12A、12B及金屬A層14間之含有Cu及金屬A的合金層,其含有濃度範圍各在1至10at%之Cu及金屬A的合金層的厚度總計在30至400nm之範圍內,可提高層間之密接性。藉此,可耐受隨著熱循環試驗等之溫度升降,起因於Cu與金屬A之熱膨脹差的剪應力,且可抑制在層間產生空孔,因此可提高長期可靠性。層間之空孔成為使接合強度降低之原因,有使長期可靠性降低之問題。若合金層之厚度小於30nm,則抑制空孔產生的效果減少。若合金層之厚度超過400nm,則合金層之熱阻大,因此熱傳導降低,此外,產生在層間形成合金層時因克根達(Kinrkendall)作用等產生空孔(以下亦稱為克根達空孔)的問題。在此克根達作用係在使2種不同金屬密接而加熱時,其界面移動之現象。如上所述之合金層的效果可藉作為熱循環試驗條件之重複進行500次-40℃/200℃之試驗來進行評價。 In the case of the present embodiment, the thickness of the alloy layer is 30 to 400 nm in total. Here, the "total thickness of the alloy layer" is formed between one of the plurality of layers of the heat dissipation substrate 10, and the total of the alloy layers on both sides is formed by the joint interface. By using an alloy layer containing Cu and metal A formed between the Cu layers 12A, 12B and the metal A layer 14, the thickness of the alloy layer containing Cu and metal A each having a concentration ranging from 1 to 10 at% is 30 to a total of 30 In the range of 400 nm, the adhesion between the layers can be improved. Thereby, it is possible to withstand the temperature rise and fall of the thermal cycle test or the like, the shear stress caused by the difference in thermal expansion between Cu and the metal A, and the occurrence of voids between the layers can be suppressed, so that long-term reliability can be improved. The voids between the layers are a cause of lowering the joint strength, and there is a problem that the long-term reliability is lowered. If the thickness of the alloy layer is less than 30 nm, the effect of suppressing the generation of voids is reduced. If the thickness of the alloy layer exceeds 400 nm, the thermal resistance of the alloy layer is large, so that heat conduction is lowered, and in addition, voids are generated due to the action of Kinknendall when forming an alloy layer between layers (hereinafter also referred to as Kogenda Hole) problem. Here, the KGunda action is a phenomenon in which the interface moves when two different metals are closely bonded and heated. The effect of the alloy layer as described above can be evaluated by repeating the test of 500 times - 40 ° C / 200 ° C as a thermal cycle test condition.

前述合金層宜形成在層間之80%以上的區域中。藉由在80%之區域中形成合金層,可進一步提高Cu層12A、12B及金屬A層14之密接性。 The alloy layer is preferably formed in a region of 80% or more between the layers. The adhesion between the Cu layers 12A, 12B and the metal A layer 14 can be further improved by forming an alloy layer in an area of 80%.

前述合金層中,前述Cu及前述金屬A之濃度各為1至3at%的低濃度層厚度宜為20至300nm。藉由使低濃度層之厚度在20至300nm的範圍內,即使在層間長時間或多次地 施加剪應力時亦可抑制空孔產生,因此可提高熱循環環境中之長期可靠性。關於該低濃度層之效果,確認在同等溫差長時間重複時可獲得比溫差大時高之效果。這考慮是低濃度層具有緩和殘留應力之作用的緣故。如上所述之低濃度層的效果可藉作為熱循環試驗條件之重複進行1000次-40℃/200℃之試驗來進行評價。 In the alloy layer, the thickness of the low concentration layer in which the concentration of Cu and the metal A is 1 to 3 at% each is preferably 20 to 300 nm. By making the thickness of the low concentration layer in the range of 20 to 300 nm, even for a long time or multiple times between layers The application of shear stress also suppresses the generation of voids, thereby improving long-term reliability in a thermal cycle environment. Regarding the effect of the low-concentration layer, it was confirmed that when the same temperature difference is repeated for a long time, an effect higher than when the temperature difference is large can be obtained. This is considered to be because the low concentration layer has the effect of relaxing the residual stress. The effect of the low-concentration layer as described above can be evaluated by repeating the test of 1000 times - 40 ° C / 200 ° C as a thermal cycle test condition.

雖然比低濃度層之濃度高之3至10%合金濃度的高濃度層具有提高接著性的效果,但該高濃度層在狹窄區域中濃度梯度大,因此只利用該高濃度層,難以提高熱循環環境中之長期可靠性。此外,為在廣大區域中形成高濃度層,會產生需要長時間高溫熱處理而使生產性降低等之問題。 Although the high-concentration layer having a concentration of 3 to 10% higher than the concentration of the low-concentration layer has an effect of improving adhesion, the concentration gradient of the high-concentration layer is large in a narrow region, and therefore it is difficult to increase heat only by using the high-concentration layer. Long-term reliability in a cyclic environment. Further, in order to form a high-concentration layer in a large area, there is a problem that a long-time high-temperature heat treatment is required to reduce productivity.

積層之前述Cu層12A、12B及前述金屬A層14之厚度總計宜為0.5至2mm。若厚度總計在上述範圍內,則可控制整體之熱傳導、熱膨脹,且在實用上之熱循環環境或TCT(溫度循環測試:Temperature Cycle Testing)試驗等中可安定地發揮性能。 The thickness of the aforementioned Cu layers 12A, 12B and the aforementioned metal A layer 14 is preferably 0.5 to 2 mm in total. When the total thickness is within the above range, the overall heat conduction and thermal expansion can be controlled, and the performance can be stably achieved in a practical thermal cycle environment or a TCT (Temperature Cycle Testing) test or the like.

(2)製造方法 (2) Manufacturing method

接著,本實施形態之散熱基板10可藉由交互重疊Cu板及金屬A板並實施熱壓加工來製造。以下,依序說明形成具有所希望大小之結晶粒18的金屬A層14的方法、及形成合金層的方法。 Next, the heat dissipation substrate 10 of the present embodiment can be manufactured by superimposing a Cu plate and a metal A plate on each other and performing hot press processing. Hereinafter, a method of forming the metal A layer 14 having the crystal grains 18 of a desired size and a method of forming the alloy layer will be described in order.

(金屬A層) (metal layer A)

控制金屬A層14之金屬A之長邊方向X的平均結晶粒長 度L、及厚度方向之平均結晶粒長度t、以及寬度方向之平均結晶粒長度d的方法包括:在金屬A板單體之製造步驟中控制的方法、及在接合Cu板與金屬A板之步驟中控制的方法。藉由製造接合前之金屬A板單體時之輥軋及熱處理,控制長度L、t、d,並在切斷接合Cu板與金屬A板之原板的步驟中,管理長度L、d是有效的。L、d係藉由散熱基板10之面內的方向來決定,因此可藉將原板切斷成小片時之方向來調整。以下,說明控制接合前之金屬A板單體長度L、t的方法。 Controlling the average crystal grain length of the long side direction X of the metal A of the metal A layer 14 The method of the L, the average crystal grain length t in the thickness direction, and the average crystal grain length d in the width direction includes a method of controlling in the manufacturing step of the metal A plate unit, and bonding the Cu plate and the metal A plate. The method of control in the step. The length L, t, and d are controlled by the rolling and heat treatment in the production of the metal A plate unit before joining, and the length L and d are effective in the step of cutting the original plate of the bonded Cu plate and the metal A plate. of. Since L and d are determined by the direction in the plane of the heat dissipation substrate 10, they can be adjusted by cutting the original plate into small pieces. Hereinafter, a method of controlling the metal L-plate lengths L and t before joining will be described.

為使金屬A層14之結晶粒18之長邊/板厚的平均縱橫比(L/t)在1.5至10.0之範圍內,增加金屬A板之輥軋加工度,同時使在加工途中實施之中間熱處理溫度比再結晶溫度低是有效的。為了在1.5至10.0之範圍中提高長邊/板厚的平均縱橫比(L/t),宜實施2次以上之中間熱處理,且使中間熱處理溫度比再結晶溫度低。相對於此,藉由降低輥軋之加工度及使中間熱處理溫度比再結晶溫度高,長邊/板厚的平均縱橫比(L/t)可小於1.5。因此藉由在實施中間熱處理後,在進行試料之冷卻前進行輥軋,可輕易地控制長度L、t。 In order to make the average aspect ratio (L/t) of the long side/thickness of the crystal grain 18 of the metal A layer 14 in the range of 1.5 to 10.0, the rolling workability of the metal A plate is increased, and at the same time, it is carried out during processing. The intermediate heat treatment temperature is lower than the recrystallization temperature. In order to increase the average aspect ratio (L/t) of the long side/plate thickness in the range of 1.5 to 10.0, it is preferred to carry out the intermediate heat treatment twice or more, and the intermediate heat treatment temperature is lower than the recrystallization temperature. On the other hand, by reducing the degree of processing of the rolling and making the intermediate heat treatment temperature higher than the recrystallization temperature, the average aspect ratio (L/t) of the long side/thickness can be less than 1.5. Therefore, the lengths L and t can be easily controlled by performing rolling after performing the intermediate heat treatment before cooling the sample.

為了使金屬A層14之結晶粒18之長邊/寬度的平均縱橫比(L/d)在1.2至7.0之範圍內,控制輥軋由金屬A構成之板材時的通過1次軋縮率、輥軋速度並使輥軋方向之結晶粒18大幅成長,且進一步以使輥軋方向與散熱板之長邊方向平行的方式切斷是有效的。即,藉由使軋縮率在30至80%之範圍內,並控制輥軋速度在0.3至10m/分之範圍內,使結 晶粒18之成長與輥軋方向一致,可在1.2至7.0之範圍內輕易地調整(L/d)。相對於此,藉由減少輥軋之軋縮率,或以使輥軋方向為散熱板之寬度方向的方式切斷,(L/d)可小於1.2。此外,藉由使輥軋之軋縮率上升、增加通過數、使中間熱處理溫度降低,(L/d)可超過7.0。 In order to make the average aspect ratio (L/d) of the long side/width of the crystal grains 18 of the metal A layer 14 in the range of 1.2 to 7.0, it is controlled to pass the primary reduction ratio when rolling the sheet composed of the metal A, The rolling speed is such that the crystal grains 18 in the rolling direction are greatly grown, and it is effective to cut the rolling direction so as to be parallel to the longitudinal direction of the heat dissipation plate. That is, by making the rolling reduction in the range of 30 to 80% and controlling the rolling speed in the range of 0.3 to 10 m/min, the knot is made The growth of the crystal grains 18 coincides with the rolling direction and can be easily adjusted (L/d) in the range of 1.2 to 7.0. On the other hand, (L/d) may be less than 1.2 by reducing the rolling reduction ratio of the rolling or cutting the rolling direction so as to be the width direction of the heat dissipation plate. Further, (L/d) may exceed 7.0 by increasing the rolling reduction ratio of the rolling, increasing the number of passes, and lowering the intermediate heat treatment temperature.

以下以使用Mo作為金屬A時,由5mm厚之Mo板輥軋薄至預定厚度之製造步驟為例說明中間熱處理,作為具體製造條件之一例,即藉由使1道次之輥軋時的軋縮率在30至70%之範圍內,並在輥軋速度在0.5至3m/分之範圍內製作,可調整長邊/寬度之平均縱橫比(L/d)。就熱處理而言,可分為在厚度1至1.5mm之範圍內進行1次之熱處理(第一中間熱處理)、及在厚度0.1至0.3mm之範圍內進行1次以上之熱處理(第二中間熱處理)。調整長邊/板厚之平均縱橫比(L/t)至1.5至4之範圍內,且調整(L/d)至1.2至7.0之範圍內的有效熱處理條件係實施1次第一中間熱處理、2次以上第二中間熱處理,並令其溫度範圍為700至1200℃。使長邊/板厚之平均縱橫比(L/t)在4至10.0之範圍內的有效熱處理條件係在第一中間熱處理為600至800℃以上,且第二中間熱處理為500至800℃之溫度範圍內實施2次以上。藉由以輥軋方向與散熱基板10之長邊方向平行方式切斷原板而小片化,可製得預定大小之散熱基板10。 Hereinafter, in the case where Mo is used as the metal A, the intermediate heat treatment is exemplified as a manufacturing step in which a 5 mm thick Mo plate is rolled to a predetermined thickness, and as an example of specific production conditions, that is, rolling is performed by rolling one pass. The shrinkage ratio is in the range of 30 to 70%, and the rolling speed is in the range of 0.5 to 3 m/min, and the average aspect ratio (L/d) of the long side/width can be adjusted. In terms of heat treatment, it may be divided into a heat treatment once in the range of 1 to 1.5 mm in thickness (first intermediate heat treatment), and a heat treatment in which the thickness is 0.1 to 0.3 mm or more (second intermediate heat treatment) ). Adjusting the average aspect ratio (L/t) of the long side/plate thickness to the range of 1.5 to 4, and adjusting the effective heat treatment conditions in the range of (L/d) to 1.2 to 7.0 is performed once the first intermediate heat treatment, 2 or more second intermediate heat treatments, and the temperature range is 700 to 1200 °C. The effective heat treatment conditions for the average aspect ratio (L/t) of the long side/plate thickness in the range of 4 to 10.0 are in the first intermediate heat treatment of 600 to 800 ° C or more, and the second intermediate heat treatment is 500 to 800 ° C. It is carried out twice or more in the temperature range. The original plate is cut into small pieces in a direction in which the rolling direction is parallel to the longitudinal direction of the heat-dissipating substrate 10, whereby a heat-dissipating substrate 10 having a predetermined size can be obtained.

製造條件不限於上述記載,藉由使溫度、長度L、t、熱處理溫度等條件適性化,可獲得所希望之平均縱橫比(L/t)或(L/d)。 The production conditions are not limited to those described above, and a desired average aspect ratio (L/t) or (L/d) can be obtained by adapting conditions such as temperature, length L, t, and heat treatment temperature.

(合金層) (alloy layer)

作為本實施形態之在層間形成合金層的方法,控制在交互重疊Cu板及金屬A板並實施熱壓加工時之溫度歷程、壓力歷程等,在層間形成合金層的方法量產性高,且工業上亦簡便。此外,作為其他方法,亦可在接合前在金屬A層14側鍍敷薄Cu後實施熱處理,事先形成Cu及金屬A之合金層的一部分。 As a method of forming an alloy layer between layers in the present embodiment, a method of forming an alloy layer between layers by controlling a temperature history and a pressure history when a Cu plate and a metal A plate are overlapped and performing hot press processing is controlled, and mass production is high. Industrial is also simple. Further, as another method, a thin Cu may be plated on the metal A layer 14 side before bonding, and then heat treatment may be performed to form a part of the alloy layer of Cu and metal A in advance.

為了在層間形成以1至10at%之濃度範圍含有Cu及金屬A,且厚度總計在30nm至400nm之範圍內的合金層,必須使溫度歷程及壓力歷程之2條件適當化。其中一加工條件宜為在低溫區域提高升溫速度,並在高溫區域降低升溫速度。例如以大約500℃為界利用2階段控制是有效的。具體而言,藉由令到500℃之第1升溫速度為30至80℃/分,且令在500℃以上到最終加熱溫度之第2升溫速度為20至80℃/分,可形成所希望之合金層。在此之最終加熱溫度在850至1050℃之溫度範圍內,且在該溫度區域保持20至50分。 In order to form an alloy layer containing Cu and metal A in a concentration range of 1 to 10 at% and a total thickness in the range of 30 nm to 400 nm between layers, it is necessary to appropriately condition the temperature history and the pressure history. One of the processing conditions is preferably to increase the rate of temperature rise in the low temperature region and to decrease the rate of temperature rise in the high temperature region. For example, it is effective to utilize 2-stage control at a boundary of about 500 °C. Specifically, the first temperature increase rate to 500 ° C is 30 to 80 ° C / min, and the second temperature increase rate at 500 ° C or higher to the final heating temperature is 20 to 80 ° C / min. Alloy layer. The final heating temperature here is in the temperature range of 850 to 1050 ° C and is maintained in this temperature range for 20 to 50 minutes.

在此改變升溫速度之變化溫度宜在400至600℃之範圍內。這是因為400至600℃之溫度範圍接近Cu之再結晶溫度,且藉進行再結晶而軟質化,因此促進加壓時在界面之變形及擴散等的緣故。此外,除了上述2階段控制以外,亦可使用3階段控制,但量產管理較繁雜。 Here, the temperature at which the temperature rise rate is changed is preferably in the range of 400 to 600 °C. This is because the temperature range of 400 to 600 ° C is close to the recrystallization temperature of Cu, and is softened by recrystallization, thereby promoting deformation and diffusion at the interface during pressurization. In addition, in addition to the above two-stage control, three-stage control can also be used, but mass production management is complicated.

在此,若到500℃之第1升溫速度過慢,則合金層形成粒狀而有品質上之問題。此外,若第1升溫速度過快,恐怕會因Cu與金屬A之擴散速度不同而產生克根達空 孔。若500℃以上之第2升溫速度過慢,則合金層之厚度不均一。此外,若第2升溫速度過快,在爐內產生溫度不均而成為合金層濃度分布因場所而不均一的原因。不限於上述之溫度條件,藉由認識如此做之課題而使溫度歷程適性化,可工業地形成所希望之適當合金層。 Here, if the first temperature increase rate to 500 ° C is too slow, the alloy layer is formed into a granular shape and has a problem in quality. In addition, if the first heating rate is too fast, I am afraid that K-Dakong will be generated due to the difference in the diffusion speed of Cu and metal A. hole. When the second temperature increase rate of 500 ° C or more is too slow, the thickness of the alloy layer is not uniform. Further, when the second temperature increase rate is too fast, temperature unevenness occurs in the furnace, and the alloy layer concentration distribution is not uniform due to the location. Without being limited to the above-described temperature conditions, it is possible to industrially form a desired alloy layer as desired by recognizing the temperature history.

另外,第2升溫速度宜比第1升溫速度慢10℃/分以上。若第2升溫速度與第1升溫速度之差小於10℃/分,恐怕難以控制低濃度合金層之成長及其厚度。 Further, the second temperature increase rate is preferably 10 ° C/min or more slower than the first temperature increase rate. When the difference between the second temperature increase rate and the first temperature increase rate is less than 10 ° C / min, it may be difficult to control the growth of the low-concentration alloy layer and the thickness thereof.

最好與上述溫度歷程連動地調整壓力歷程,而在低溫區域提高加壓壓力,並在高溫區域降低加壓壓力。例如以大約500℃為界利用2階段控制是有效的。為在低溫區域獲得金屬接合,考慮促進加壓時之界面變形,並在高溫區域藉由Cu之軟質化而過剩地進行界面變形,以便具有抑制合金層不連續的效果。低溫區域之加壓壓力宜在高溫區域之加壓壓力的1.2至2倍的範圍內。具體而言,令到500℃之加壓壓力在36至260kgf/cm2的範圍內,並令500℃以上之加壓壓力在30至130kgf/cm2的範圍內,藉此比較容易形成所希望之合金層。在此,若加壓壓力小於下限值,則金屬接合不充分而使金屬層不連續。若加壓壓力超過上限值,則在脆性之金屬A層14中產生裂縫等,難以安定地形成合金層,而若在高溫區域超過上限值,則有Cu層12A、12B之厚度不均一等的問題。 It is preferable to adjust the pressure history in conjunction with the above temperature history, and to increase the pressurizing pressure in the low temperature region and to lower the pressurizing pressure in the high temperature region. For example, it is effective to utilize 2-stage control at a boundary of about 500 °C. In order to obtain metal joining in a low temperature region, it is conceivable to promote interfacial deformation during pressurization, and excessively interfacial deformation is performed by softening Cu in a high temperature region, so as to have an effect of suppressing discontinuity of the alloy layer. The pressing pressure in the low temperature region is preferably in the range of 1.2 to 2 times the pressing pressure in the high temperature region. Specifically, the pressurization pressure to 500 ° C is in the range of 36 to 260 kgf / cm 2 , and the pressurization pressure of 500 ° C or more is in the range of 30 to 130 kgf / cm 2 , whereby it is easy to form a desired Alloy layer. Here, when the pressurization pressure is less than the lower limit value, the metal joining is insufficient and the metal layer is discontinuous. When the pressure exceeds the upper limit, cracks or the like are formed in the brittle metal layer A, and it is difficult to form the alloy layer stably. If the high temperature region exceeds the upper limit, the thickness of the Cu layers 12A and 12B is not uniform. Etc.

此外,藉由上述溫度歷程及加壓歷程,可在層間之80%形成合金層。另一方面,為使低濃度層之厚度安 定,且減少合金層內之空孔、龜裂等,使冷卻時之溫度變化、加壓壓力階段地適當化是有效的。最好在高溫區域降低冷卻速度,並在低溫區域提高冷卻速度。此外,最好亦階段地降低加壓壓力。藉此,可在高溫區域減少冷卻速度而緩和熱膨脹差造成之應變,以抑制在薄合金層中產生龜裂。此外,藉由增加低溫區域之冷卻速度,可提高作業效率。另外,若在高溫下急速地減少加壓壓力,恐怕低濃度層會因熱應力之作用而變形,且低濃度層之厚度不均一會變大。 Further, the alloy layer can be formed at 80% between the layers by the above temperature history and pressurization history. On the other hand, in order to make the thickness of the low concentration layer It is effective to reduce pores, cracks, and the like in the alloy layer, and to appropriately change the temperature at the time of cooling and the pressurization pressure. It is preferable to lower the cooling rate in a high temperature region and increase the cooling rate in a low temperature region. In addition, it is preferred to also reduce the pressurization pressure in stages. Thereby, the cooling rate can be reduced in the high temperature region to alleviate the strain caused by the difference in thermal expansion to suppress the occurrence of cracks in the thin alloy layer. In addition, work efficiency can be improved by increasing the cooling rate in the low temperature region. Further, if the pressurization pressure is rapidly reduced at a high temperature, the low-concentration layer may be deformed by the action of thermal stress, and the thickness of the low-concentration layer may become uneven.

作為冷卻時之溫度變化、加壓壓力的具體例,在由加熱溫度850至1050℃冷卻之情形中,到700℃之冷卻速度為10至30℃/分且加壓壓力在60至200kgf/cm2之範圍內,而700℃以下之冷卻速度為40至80℃/分且加壓壓力在在30至130kgf/cm2之範圍內對量產亦有用。宜至少具有冷卻速度為10℃/分,加壓壓力為30kgf/cm2之差。在此使變化溫度為大約700℃,在提高層間密接性方面是有效的。雖然詳情尚不明,但考慮是以該溫度附近為界形成在界面之低濃度層的強度、延展性、內部之擴散舉動等變化的關係。 As a specific example of the temperature change and the pressurizing pressure at the time of cooling, in the case of cooling by the heating temperature of 850 to 1050 ° C, the cooling rate to 700 ° C is 10 to 30 ° C / min and the pressurizing pressure is 60 to 200 kgf / cm. Within the range of 2 , the cooling rate below 700 ° C is 40 to 80 ° C / min and the pressurizing pressure is also useful for mass production in the range of 30 to 130 kgf / cm 2 . It is preferred to have at least a cooling rate of 10 ° C / min and a pressurization pressure of 30 kgf / cm 2 . Here, the change temperature is about 700 ° C, which is effective in improving interlayer adhesion. Although the details are not known, it is considered that the relationship between the strength, the ductility, and the internal diffusion behavior of the low concentration layer formed at the interface is defined by the vicinity of the temperature.

關於各原料,由熱傳導性之觀點來看,Cu之純度宜為99.3%以上,且可使用無氧銅、精銅等。作為金屬A之Mo及W可使用純度99.3%以上之市售原料。此外,在散熱基板10要求高強度之用途等中,亦可使用含有5%以下添加元素之Cu及Mo或W等。 With respect to each raw material, the purity of Cu is preferably 99.3% or more from the viewpoint of thermal conductivity, and oxygen-free copper, refined copper, or the like can be used. As the Mo and W of the metal A, a commercially available raw material having a purity of 99.3% or more can be used. Further, in the use of the heat-dissipating substrate 10 requiring high strength, Cu, Mo, W or the like containing 5% or less of an additive element may be used.

2.實施例 2. Examples

(1)試料 (1) Sample

依照在上述「製造方法」中說明之步驟,製作5層及9層構造之散熱基板作為試料。首先,準備預定厚度之Cu板及Mo板或W板。接著,進行提高在接合界面之密接性的洗淨處理。為對Mo板及W板去除氧化膜,藉大約50℃之熱水進行洗淨,接著藉稀硫酸等對Cu板進行酸洗處理。洗淨後實施水洗、乾燥。最後交互積層Cu板及Mo板或W,並藉由熱壓加工接合,製成實施例及比較例之散熱基板(原板)。藉放電加工由該原板切出試料,使試料大小為長邊方向長度20mm,且寬度方向長度10mm。製成之試料規格顯示於表1中。 According to the procedure described in the above "Manufacturing Method", a heat-dissipating substrate having a 5-layer structure and a 9-layer structure was prepared as a sample. First, a Cu plate and a Mo plate or a W plate of a predetermined thickness are prepared. Next, a washing treatment for improving the adhesion at the joint interface is performed. In order to remove the oxide film on the Mo plate and the W plate, the aluminum plate is washed with hot water of about 50 ° C, and then the Cu plate is pickled by dilute sulfuric acid or the like. After washing, it is washed with water and dried. Finally, the Cu board and the Mo board or W were laminated and joined by hot press working to form the heat dissipating substrate (original board) of the examples and the comparative examples. The sample was cut out from the original plate by electric discharge machining so that the sample size was 20 mm in the longitudinal direction and 10 mm in the width direction. The prepared sample specifications are shown in Table 1.

(2)評價 (2) Evaluation

對實施例及比較例之散熱基板,在厚度方向之Mo層及W層的截面藉EBSD(Zeiss公司製,Ultra55)裝置觀察Mo及W之長度L、t,並藉由分析軟體算出平均粒徑。此外,使用TEM(日本電子(股)製,JEM-2100F)裝置、EDS裝置(日本電子(股)製,JED-2300T)進行接合界面之濃度分析。濃度分析係接合界面居間地沿垂線方向在Cu層及Mo層兩側合計大約200至500nm的範圍內進行。關於進行濃度分析之間隔,基本上是以10nm間隔進行。此外,為使合金層之邊界明確,就相當於低濃度區域之大約1至10at%的濃度區域而言,以2nm間隔詳細地進行分析。每一試料之測量係以3線以上實施EDS線分析。最好在Cu層及Mo層之多數層間中之2處以 上的不同層間測量。 For the heat dissipation substrates of the examples and the comparative examples, the lengths of the Mo layer and the W layer in the thickness direction were observed by EBSD (Ultra 55 manufactured by Zeiss), and the lengths L and t of Mo and W were observed, and the average particle diameter was calculated by analyzing the software. . Further, concentration analysis of the joint interface was performed using a TEM (JEM-2100F, manufactured by JEOL Ltd.) and an EDS device (manufactured by JEOL Ltd., JED-2300T). The concentration analysis is performed in a manner in which the bonding interface is interposed in the vertical direction in the range of about 200 to 500 nm on both sides of the Cu layer and the Mo layer. The interval for performing the concentration analysis was basically performed at intervals of 10 nm. Further, in order to make the boundary of the alloy layer clear, the concentration region corresponding to about 1 to 10 at% of the low concentration region was analyzed in detail at intervals of 2 nm. The measurement of each sample was performed by EDS line analysis with more than 3 lines. Preferably, at two of the majority of the Cu layer and the Mo layer Different layers are measured on top.

長期可靠性之評價係實施TCT試驗。使用之試料係在散熱基板之單側藉Ag硬焊接合Si晶片,而在相反側藉Ni合金硬焊料接合氧化鋁DCB(直接銅接合:Direct Copper Bond)基板之Cu電極的試料。TCT試驗使用加熱溫度不同之2種試驗條件。TCT試驗條件係TCT試驗條件(2)比TCT試驗條件(1)嚴格之熱循環條件。溫度範圍在試驗條件(1)係-40至+200℃,而在試驗條件(2)係-40至+225℃ The evaluation of long-term reliability is the implementation of the TCT test. The sample used was a sample in which a Cu electrode of an alumina DCB (Direct Copper Bond) substrate was bonded by a Ni alloy hard solder on one side of the heat dissipation substrate by Ag hard soldering of the Si wafer. The TCT test uses two test conditions with different heating temperatures. The TCT test conditions are the thermal cycling conditions under which the TCT test conditions (2) are stricter than the TCT test conditions (1). The temperature range is from -40 to +200 °C in the test conditions (1), and -40 to +225 °C in the test conditions (2).

TCT試驗係在試驗條件(1)(-40至+200℃之範圍)下進行500次或1000次溫度升降,且在試驗條件(2)(-40至+225℃之範圍)下進行500次或1000次溫度升降。該TCT試驗後,進行散熱基板之截面觀察並進行評價。試料數為各2個。為進行截面觀察,進行散熱基板之截面切斷及機械研磨。散熱基板之截面觀察係選定多數層間中之3處不同層間,藉SEM觀察各大約2mm之層間的空孔及裂縫。以大小區別,分類為空孔大小小於10μm(主要呈點狀),裂縫10μm以上之龜裂(主要呈線狀)。 The TCT test is carried out 500 times or 1000 times in the test condition (1) (range of -40 to +200 ° C), and is carried out 500 times under the test condition (2) (-40 to +225 ° C range). Or 1000 temperature rises and falls. After the TCT test, the cross section of the heat-dissipating substrate was observed and evaluated. The number of samples is two each. For cross-sectional observation, cross-section cutting and mechanical polishing of the heat-dissipating substrate are performed. The cross-sectional observation of the heat-dissipating substrate was carried out by selecting three different layers among the plurality of layers, and observing the voids and cracks between the layers of about 2 mm by SEM. According to the size difference, the pore size is less than 10 μm (mainly in the shape of a dot), and the crack is more than 10 μm (mainly linear).

散熱基板之層間空孔觀察係調查個數,若該個數在每1mm為5個以下則TCT試驗之長期可靠性良好,因此在表2中記為○記號,若在6至20個之範圍內則判斷為實用上沒有問題但品質上希望改善而在表2中記為△記號,若為21個以上則有可靠性降低之問題,因此在表2中記為×記號。 The number of holes in the interlayer observation of the heat-dissipating substrate is investigated. If the number is 5 or less per 1 mm, the long-term reliability of the TCT test is good. Therefore, it is marked as ○ in Table 2, and in the range of 6 to 20. In the meantime, it is judged that there is no problem in practical use, but the quality is expected to be improved, and it is indicated by Δ mark in Table 2, and if it is 21 or more, there is a problem that reliability is lowered. Therefore, it is indicated as × mark in Table 2.

散熱基板之層間裂縫觀察係調查個數,若該個 數在每1mm為5個以下則TCT試驗之長期可靠性良好,因此在表2中記為○記號,若在6至15個之範圍內則判斷為實用上沒有問題但品質上希望改善而在表2中記為△記號,若為16個以上則有可靠性降低之問題,因此在表2中記為×記號。 The number of interlayer cracks in the heat-dissipating substrate is investigated, if the number When the number is 5 or less per 1 mm, the long-term reliability of the TCT test is good. Therefore, it is indicated as ○ mark in Table 2, and if it is in the range of 6 to 15, it is judged that there is no problem in practical use, but the quality is expected to be improved. In Table 2, the symbol is denoted by Δ. If it is 16 or more, the reliability is lowered. Therefore, it is indicated by × in Table 2.

散熱基板之硬焊的空隙觀察係藉由截面觀察調查5μm以上之空隙個數,若該個數在每1mm為10個以下則TCT試驗之長期可靠性良好,因此在表2中記為○記號,若在11至20個之範圍內則判斷為實用上沒有問題但品質上希望改善而在表2中記為△記號,若為21個以上則有可靠性降低之問題,因此在表2中記為×記號。 When the number of voids of 5 μm or more is investigated by cross-section observation, the long-term reliability of the TCT test is good when the number is 10 or less per 1 mm, so it is marked as ○ mark in Table 2. If it is in the range of 11 to 20, it is judged that there is no problem in practical use, but the quality is expected to be improved, and it is indicated as Δ mark in Table 2, and if it is 21 or more, the reliability is lowered, so in Table 2, Recorded as × mark.

此外,以未安裝之散熱基板作為試料,評價因高溫加熱後之散熱基板的熱變形產生的翹曲。試料數為各2個。高溫加熱條件係由常溫加熱至800℃,接著在800℃保持5分鐘後,在大氣中冷卻(試驗條件(3))。翹曲之評價係使用雷射顯微鏡(Lasertec(股)公司製,H1200),測量沿對角線方向由中心至末端之長度E、及中央部與端部之高度差G,並以G/E作為翹曲比。若翹曲比小於0.03%則熱變形小而為良好,因此在表2中記為○記號,若在0.03至0.1%之範圍內則判斷為實用上沒有問題但品質上希望改善而在表2中記為△記號,若超過0.1%則有因翹曲而密接性降低之問題,因此在表2中記為×記號。 Further, the heat-dissipating substrate which was not mounted was used as a sample, and the warpage caused by the thermal deformation of the heat-dissipating substrate after the high-temperature heating was evaluated. The number of samples is two each. The high-temperature heating condition was heated from room temperature to 800 ° C, and then kept at 800 ° C for 5 minutes, and then cooled in the atmosphere (test condition (3)). The warpage was evaluated by using a laser microscope (manufactured by Lasertec Co., Ltd., H1200) to measure the length E from the center to the end in the diagonal direction, and the height difference G between the center portion and the end portion, and G/E. As the warpage ratio. When the warpage ratio is less than 0.03%, the thermal deformation is small and is good. Therefore, it is marked as ○ mark in Table 2, and if it is in the range of 0.03 to 0.1%, it is judged that there is no practical problem, but the quality is expected to be improved. In the case of the Δ mark, if it exceeds 0.1%, there is a problem that the adhesion is lowered due to warpage, and therefore, it is denoted by X mark in Table 2.

(3)結果 (3) Results

由表1、2可知,實施例1至24由於金屬A層之結晶粒長 邊/板厚的平均縱橫比(L/t)為1.5至10.0,且金屬A層之結晶粒長邊/寬度的平均縱橫比(L/d)為1.2至7.0,TCT試驗條件(1)(循環條件500次)之安裝後的層間裂縫觀察結果為良好且TCT試驗條件(2)(循環條件500次)之安裝後的晶片裂縫觀察結果為良好。相對於此,比較例1至9由於金屬A層之結晶粒長邊/板厚的平均縱橫比(L/t),或金屬A層之結晶粒長邊/寬度的平均縱橫比(L/d)小於上述範圍之下限或超過上限,所以TCT試驗條件(1)(循環條件500次)之安裝後的層間裂縫觀察結果為×,且TCT試驗條件(2)(循環條件500次)之安裝後的晶片裂縫觀察結果為×。 As can be seen from Tables 1 and 2, Examples 1 to 24 have crystal grain lengths due to the metal A layer. The average aspect ratio (L/t) of the edge/plate thickness is 1.5 to 10.0, and the average aspect ratio (L/d) of the crystal grain length/width of the metal A layer is 1.2 to 7.0, and the TCT test condition (1) ( The result of the interlaminar crack observation after the installation of the cycle condition of 500 times was good, and the result of the wafer crack observation after the mounting of the TCT test condition (2) (circular condition 500 times) was good. On the other hand, in Comparative Examples 1 to 9, the average aspect ratio (L/t) of the crystal grain long side/sheet thickness of the metal A layer, or the average aspect ratio (L/d) of the crystal grain long side/width of the metal A layer. ) is less than the lower limit of the above range or exceeds the upper limit, so the observation result of the interlaminar crack after the installation of the TCT test condition (1) (circular condition 500 times) is ×, and after the installation of the TCT test condition (2) (circular condition 500 times) The wafer crack observation result is ×.

此外,實施例1、2、5、6、8、9、11、12、14至23由於前述(L/d)為2.0以上,TCT試驗條件(2)(循環條件1000次)之安裝後的晶片裂縫觀察結果為良好。 Further, in Examples 1, 2, 5, 6, 8, 9, 11, 12, and 14 to 23, since the above (L/d) was 2.0 or more, the TCT test condition (2) (circulation condition 1000 times) was installed. The wafer crack observation was good.

實施例1、2、4至12、14至24由於金屬A層之結晶粒長邊/板厚的平均縱橫比(L/t)為2.0以上,TCT試驗條件(2)(循環條件500次)之安裝後的層間裂縫觀察結果為良好。 In Examples 1, 2, 4 to 12, and 14 to 24, the average aspect ratio (L/t) of the crystal grain long side/thickness of the metal A layer was 2.0 or more, and the TCT test condition (2) (circulation condition 500 times) The interlaminar crack observation after the installation was good.

實施例1、2、5、6、8至12、15至17、19至23由於金屬A層之結晶粒長邊/板厚的平均縱橫比(L/t)為3.0以上,TCT試驗條件(2)(循環條件1000次)之安裝後的層間裂縫觀察結果為良好。 Examples 1, 2, 5, 6, 8 to 12, 15 to 17, 19 to 23 have an average aspect ratio (L/t) of crystal grain length/sheet thickness of the metal A layer of 3.0 or more, and TCT test conditions ( 2) The results of observation of interlaminar cracks after installation (1000 cycles) were good.

實施例1至8、10、11、19至21、24由於表面之Cu層厚度H1與中央之Cu層厚度H2的比(H1/H2)為0.2至0.9,TCT試驗條件(2)(循環條件500次)之安裝後的硬焊材內的 空隙觀察結果為良好。 8,10,11,19 Examples 1 to 21 and 24 due to the surface of the Cu layer and the thickness H 1 of the central Cu layer thickness ratio H 2 (H 1 / H 2) from 0.2 to 0.9, TCT test conditions (2 The results of the void observation in the hard-weld material after the installation (500 cycles) were good.

實施例1、2、4至8、10至14、16、19至24由於表面之Cu層厚度H1及與前述Cu層連接之金屬A層厚度H3的比(H1/H3)為2.0至8.0,試驗條件(3)(800℃之高溫加熱)之單體翹曲評價結果為良好。 Examples 1, 2, 4 to 8, 10 to 14, 16, 19 to 24 have a ratio (H 1 /H 3 ) of the Cu layer thickness H 1 of the surface and the metal layer thickness H 3 connected to the Cu layer. From 2.0 to 8.0, the monomer warpage evaluation result of the test condition (3) (high temperature heating at 800 ° C) was good.

實施例1至4、6至10、12至24由於合金層之厚度總計為30至400nm,TCT試驗條件(1)(循環條件500次)之安裝後的層間空孔觀察結果為良好。 In Examples 1 to 4, 6 to 10, and 12 to 24, since the thickness of the alloy layer was 30 to 400 nm in total, the observation of the interlaminar pores after the installation of the TCT test condition (1) (cycle condition 500 times) was good.

實施例2至4、7至10、12至20、22至24由於低濃度層厚度為20至300nm,TCT試驗條件(1)(循環條件1000次)之安裝後的層間空孔觀察結果為良好。 Examples 2 to 4, 7 to 10, 12 to 20, and 22 to 24 have a low concentration layer thickness of 20 to 300 nm, and the TCT test condition (1) (circulation condition 1000 times) is good after the installation of the interlayer voids. .

3.變形例 3. Modifications

本發明不限於上述實施形態,可在本發明宗旨之範圍內進行適當變更。 The present invention is not limited to the above embodiment, and can be appropriately modified within the scope of the gist of the invention.

10‧‧‧散熱基板 10‧‧‧heated substrate

12A,12B‧‧‧Cu層 12A, 12B‧‧‧Cu layer

14‧‧‧金屬A層 14‧‧‧Metal A layer

Claims (8)

一種散熱基板,係交互積層Cu層及由金屬A構成之金屬A層而成的矩形散熱基板,其特徵在於:前述Cu層及前述金屬A層合計積層5或9層;前述金屬A層之前述散熱基板長邊方向的平均結晶粒長度L與厚度方向的平均結晶粒長度t的比(L/t)係1.5至10.0;且長邊方向的前述平均結晶粒長度L與前述金屬A層之前述散熱基板寬度方向的平均結晶粒長度d的比(L/d)係1.2至7.0。 A heat dissipating substrate is a rectangular heat dissipating substrate formed by alternately laminating a Cu layer and a metal A layer made of a metal A, wherein the Cu layer and the metal A layer are a total of 5 or 9 layers; and the metal A layer is The ratio (L/t) of the average crystal grain length L in the longitudinal direction of the heat dissipation substrate to the average crystal grain length t in the thickness direction is 1.5 to 10.0; and the average crystal grain length L in the longitudinal direction and the aforementioned metal layer A are The ratio (L/d) of the average crystal grain length d in the width direction of the heat dissipation substrate is 1.2 to 7.0. 如請求項1之散熱基板,其中配置於表面之前述Cu層厚度H1及與前述Cu層連接之前述金屬A層厚度H3的比(H1/H3)為2.0至8.0。 The heat dissipation substrate of a request, wherein the configuration on the surface of the Cu layer thicknesses H 1 and H the thickness of the metal layer A is connected to the ratio of the Cu-layer (H 1 / H 3) 3 is 2.0 to 8.0. 如請求項1或2之散熱基板,其中配置於表面之前述Cu層厚度H1與配置於中央之前述Cu層厚度H2的比(H1/H2)為0.1至0.9。 The requested item of the heat-dissipating substrate 1 or 2, wherein the Cu-layer is disposed on the surface of the thickness H 1 and is arranged at the center of the thickness of the Cu layer of H 2 (H 1 / H 2) from 0.1 to 0.9. 如請求項1或2之散熱基板,其在前述Cu層與前述金屬A層的層間,形成有由Cu及前述金屬A構成之合金層;並且前述合金層含有1至10at%之前述Cu或前述金屬A,且厚度總計為30至400nm。 The heat dissipation substrate according to claim 1 or 2, wherein an alloy layer composed of Cu and the metal A is formed between the Cu layer and the layer of the metal A layer; and the alloy layer contains 1 to 10 at% of the foregoing Cu or the foregoing Metal A, and the total thickness is 30 to 400 nm. 如請求項4之散熱基板,其中前述合金層形成在前述層間之80%以上的區域。 The heat dissipation substrate of claim 4, wherein the alloy layer is formed in a region of 80% or more of the layer. 如請求項4之散熱基板,其中前述合金層中,前述Cu或前述金屬A之濃度為1至3at%的低濃度層厚度係20至300nm。 The heat-dissipating substrate according to claim 4, wherein in the alloy layer, the concentration of the Cu or the metal A is 1 to 3 at%, and the low-concentration layer has a thickness of 20 to 300 nm. 如請求項1或2之散熱基板,其中經積層之前述Cu層及前述金屬A層的厚度總計為0.5至2mm。 The heat-dissipating substrate of claim 1 or 2, wherein the thickness of the laminated Cu layer and the metal A layer is 0.5 to 2 mm in total. 如請求項1或2之散熱基板,其中前述金屬A係Mo或W。 The heat dissipation substrate of claim 1 or 2, wherein the aforementioned metal A is Mo or W.
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