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JPS6231828B2 - - Google Patents
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JPS6231828B2 - - Google Patents

Info

Publication number
JPS6231828B2
JPS6231828B2 JP55125783A JP12578380A JPS6231828B2 JP S6231828 B2 JPS6231828 B2 JP S6231828B2 JP 55125783 A JP55125783 A JP 55125783A JP 12578380 A JP12578380 A JP 12578380A JP S6231828 B2 JPS6231828 B2 JP S6231828B2
Authority
JP
Japan
Prior art keywords
layer
insulating layer
substrate
heat
conductor pattern
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP55125783A
Other languages
Japanese (ja)
Other versions
JPS5750455A (en
Inventor
Kenji Nagashima
Hiroshi Matsumoto
Hiroshi Oohira
Nobuo Iwase
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP55125783A priority Critical patent/JPS5750455A/en
Publication of JPS5750455A publication Critical patent/JPS5750455A/en
Publication of JPS6231828B2 publication Critical patent/JPS6231828B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10WGENERIC PACKAGES, INTERCONNECTIONS, CONNECTORS OR OTHER CONSTRUCTIONAL DETAILS OF DEVICES COVERED BY CLASS H10
    • H10W40/00Arrangements for thermal protection or thermal control
    • H10W40/20Arrangements for cooling
    • H10W40/25Arrangements for cooling characterised by their materials
    • H10W40/255Arrangements for cooling characterised by their materials having a laminate or multilayered structure, e.g. direct bond copper [DBC] ceramic substrates
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10WGENERIC PACKAGES, INTERCONNECTIONS, CONNECTORS OR OTHER CONSTRUCTIONAL DETAILS OF DEVICES COVERED BY CLASS H10
    • H10W90/00Package configurations
    • H10W90/701Package configurations characterised by the relative positions of pads or connectors relative to package parts
    • H10W90/731Package configurations characterised by the relative positions of pads or connectors relative to package parts of die-attach connectors
    • H10W90/734Package configurations characterised by the relative positions of pads or connectors relative to package parts of die-attach connectors between a chip and a stacked insulating package substrate, interposer or RDL

Landscapes

  • Cooling Or The Like Of Semiconductors Or Solid State Devices (AREA)

Description

【発明の詳細な説明】 この発明はパワー素子を組込んだ混成集積回路
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a hybrid integrated circuit incorporating power elements.

一般に、パワー素子例えばパワートランジスタ
は、基板上に他の素子例えば抵坑体、コンデン
サ、IC(集積回路)、小信号トランジスタ等と一
緒に組み込まれ、混成集積回路の回路機能が作り
上げられる。
Generally, a power element such as a power transistor is assembled on a substrate together with other elements such as a resistor, a capacitor, an IC (integrated circuit), a small signal transistor, etc., to create a circuit function of a hybrid integrated circuit.

ところで、このようなパワートランジスタを用
いた混成集積回路においては、大電力のため発熱
し、この発生した熱を外部に放熱させる放熱構造
が重要となる。従来、この放熱構造は例えば第1
図に示すようになつている。同図において、1は
パワートランジスタ、2はパワートランジスタ1
を固着させるための高温半田層、3はパワートラ
ンジスタ1で発生した熱を拡散させるためのCu
(銅)ブロツク層、4はCuブロツク層3を固着さ
せるための半田層、5はCu導体パターン、6は
エポキシ樹脂系接着剤からなる絶縁層、7はAl
(アルミニウム)基板、8は放熱板、9はAl基板
7を放熱板8に取り付けるためのねじである。す
なわち、この混成集積回路の放熱径路としては、
伝導、対流、輻射のうち伝導に注目すると、パワ
ートランジスタ1で発生した熱は、高温半田層
2、Cuブロツク層3、半田層4、Cu導体パター
ン5、絶縁層6、Al基板7、放熱板8と接続さ
れた順に伝導するように設計されている。
By the way, in a hybrid integrated circuit using such a power transistor, heat is generated due to the large amount of power, and a heat dissipation structure for dissipating the generated heat to the outside is important. Conventionally, this heat dissipation structure, for example,
It is as shown in the figure. In the same figure, 1 is a power transistor, 2 is a power transistor 1
3 is a Cu layer to diffuse the heat generated in the power transistor 1.
(copper) block layer, 4 is a solder layer for fixing the Cu block layer 3, 5 is a Cu conductor pattern, 6 is an insulating layer made of epoxy resin adhesive, 7 is Al
(aluminum) substrate, 8 is a heat sink, and 9 is a screw for attaching the Al substrate 7 to the heat sink 8. In other words, the heat dissipation path of this hybrid integrated circuit is as follows:
Focusing on conduction among conduction, convection, and radiation, the heat generated in the power transistor 1 is transferred to the high-temperature solder layer 2, the Cu block layer 3, the solder layer 4, the Cu conductor pattern 5, the insulating layer 6, the Al substrate 7, and the heat sink. 8 and are designed to conduct in the order in which they are connected.

ところで、パワートランジスタ1で発生した熱
が速く放熱板8に伝わるためには、上記各素子の
熱伝導率がよいことが必要となる。一般に、伝導
する熱量は次式(1)で与えられる。
Incidentally, in order for the heat generated in the power transistor 1 to be quickly transmitted to the heat sink 8, it is necessary that each of the above-mentioned elements have good thermal conductivity. Generally, the amount of heat conducted is given by the following equation (1).

Q=K・A・Δ/Δ …(1) ここで、Q:移動する熱量、K:熱伝導率、
A:熱の移動する部分の面積、ΔX:物質の厚
み、ΔT:物質の厚みΔXの両端での温度差であ
る。式(1)を変形すると、 ΔT=Δ/K・A・Q …(2) これはちようど電気回路のV=I・R(V:電
圧、I:電流、R:抵坑)に対応し、Δ/K・A(= Rth)を熱抵坑と呼ぶ。この値の大小によつて熱
伝導の良し悪しを見ることができる。すなわち、
厚みが薄い程、面積が大きい程、また熱伝導率が
大きい程熱抵坑(Rth)が小さくなる。ここで、
パワートランジスタ1で発生した熱が第2図に示
すように45゜の方向に拡がつて熱拡散すると仮定
すると、図に示すW1からW2までの間の熱抵坑は
次式(3)で与えられる。
Q=K・A・ΔT / ΔX …(1) Here, Q: amount of heat transferred, K: thermal conductivity,
A: Area of the part where heat moves, ΔX : Thickness of the material, ΔT : Temperature difference at both ends of the thickness ΔX of the material. Transforming equation (1), Δ T = Δ Correspondingly, ΔX /K·A (=Rth) is called thermal resistance. The quality of heat conduction can be determined by the magnitude of this value. That is,
The thinner the thickness, the larger the area, and the larger the thermal conductivity, the smaller the thermal resistance (Rth). here,
Assuming that the heat generated in the power transistor 1 spreads in the 45° direction as shown in Figure 2 and is thermally diffused, the thermal resistance between W 1 and W 2 shown in the figure is given by the following equation (3). is given by

Rth=1/K∫ 2W11/(2x+B)dx …(3) 式(3)により第1図に示した各素子の熱抵坑を計
算すると、 Rth(1)=0.172℃/W(パワートランジスタ:A=
3mm2、ΔX=130μm、K=0.84W/cm・℃)、 Rth(2)=0.071℃/W(高温半田層;ΔX=40μ
m、K=0.63W/cm・℃)、 Rth(3)=0.248℃/W(Cuブロツク層;A=13
mm2、ΔX=3mm、K=3.88W/cm・℃)、 Rth(4)=0.023℃/W(半田層;ΔX=100μm、K
=0.471W/cm・℃)、 Rth(5)=0.001℃/W(Cu導体パターン;ΔX
3.5μm、K=3.88W/cm・℃)、 Rth(6)=0.571℃/W(エポキシ樹脂の絶縁層;Δ
X=25μm、K=0.0035W/cm・℃)、 Rth(7)=0.076℃/W(Al基板;ΔX=2mm、K=
2.06W/cm・℃)、 全体のRth=1.162℃/Wとなる。
Rth=1/K∫ W 2W1 1/(2x+B) 2 dx...(3) Calculating the thermal resistance of each element shown in Figure 1 using equation (3), Rth(1)=0.172℃/W( Power transistor: A=
3mm 2 , Δ
m, K=0.63W/cm・℃), Rth(3)=0.248℃/W (Cu block layer; A=13
mm 2 , Δ
=0.471W/cm・℃), Rth(5)=0.001℃/W (Cu conductor pattern; ΔX =
3.5μm, K=3.88W/cm・℃), Rth(6)=0.571℃/W (epoxy resin insulation layer; Δ
X = 25μm, K = 0.0035W/cm・℃), Rth(7) = 0.076℃/W (Al substrate; ΔX = 2mm, K=
2.06W/cm・℃), total Rth=1.162℃/W.

これら熱抵坑のうち大きな割合を占めているの
は、高温半田層2、Cuブロツク層3及び絶縁層
6である。従つて、全体の熱抵坑を下げるために
は、これらの熱抵坑を下げればよいことがわか
る。しかし、これらのうち、高温半田層2は
TFT(熱疲労試験)等の特性上の問題からこれ
以上薄くすることは無理であり、またCuブロツ
ク層3の厚みを薄くすることは瞬間的に発生した
熱を吸収する役割を果たしている意味からも困難
である。残された絶縁層6は従来から使用されて
いる樹脂系絶縁層例えばエポキシ樹脂とすると、
前記のように0.571℃/Wと最も大きな熱抵坑を
有している。従つて、この絶縁層6の熱抵坑を下
げることが最も効果的である。従来、この樹脂系
の絶縁層6に無機質の粉(例えばAl2O3、SiO2
等)を混入させて熱伝導率を上げる方法もある
が、Al基板6との接着性の関係で、重量%で80
%が限度とされている。しかも、これら無機質の
粉は樹脂中で連続的に結合していなくて、分散さ
れているために熱伝導が樹脂層により阻止されて
しまい、せいぜい2倍程度の熱伝導率向上しか期
待できない。
The high temperature solder layer 2, the Cu block layer 3, and the insulating layer 6 account for a large proportion of these thermal resistances. Therefore, it can be seen that in order to lower the overall thermal resistance, it is necessary to lower these thermal resistances. However, among these, the high temperature solder layer 2
It is impossible to make it any thinner due to property problems such as TFT (thermal fatigue testing), and the thickness of the Cu block layer 3 is also made thinner because it plays the role of absorbing heat that is instantaneously generated. is also difficult. If the remaining insulating layer 6 is a conventionally used resin-based insulating layer, such as epoxy resin,
As mentioned above, it has the largest thermal resistance of 0.571°C/W. Therefore, it is most effective to lower the thermal resistance of this insulating layer 6. Conventionally, this resin-based insulating layer 6 has been coated with inorganic powder (for example, Al 2 O 3 , SiO 2
There is also a method of increasing thermal conductivity by mixing in aluminum (e.g.), but due to adhesiveness with the Al substrate 6, it is
% is the limit. Moreover, since these inorganic powders are not continuously bonded in the resin but are dispersed, heat conduction is blocked by the resin layer, and the thermal conductivity can only be expected to improve by about twice as much at most.

また、この樹脂系の絶縁層6をさらに薄くすれ
ば熱抵坑を下げることは可能であるが、ピンホー
ルが発生しやすく、耐電圧特性の面から厚さは25
μm程度が限度と思われる。また、この絶縁層6
はエポキシ系樹脂を使用しているために耐熱性が
低く、常用で100℃が限界である。他の基本的な
問題として、絶縁層6が25μmの厚さでは第3図
a,bに示すように、Al基板7とCu導体パター
ン5との間に約140pF/cm2の浮遊容量(C=εO
εSS/α、εO=8.855×10-12F/m、εS=4)が存 在する。すなわち混成集積回路を形成した場合、
各導体間にそれぞれの面積に比例して容量が寄生
的に存在することになり、回路そのものが発振し
やすくなつたり、歪率が大きくなる等の欠点を有
してしまう。
In addition, it is possible to lower the thermal resistance by making this resin-based insulating layer 6 even thinner, but pinholes are likely to occur, and the thickness is limited to 25 mm from the viewpoint of withstand voltage characteristics.
The limit seems to be around μm. Moreover, this insulating layer 6
Because it uses epoxy resin, it has low heat resistance, and the maximum temperature for regular use is 100℃. Another fundamental problem is that when the insulating layer 6 has a thickness of 25 μm, a stray capacitance of about 140 pF/cm 2 (C =ε O
ε S S/α, ε O =8.855×10 -12 F/m, ε S =4). In other words, when forming a hybrid integrated circuit,
A capacitance exists parasitically between each conductor in proportion to the area of each conductor, resulting in disadvantages such as the circuit itself becoming more likely to oscillate and the distortion rate increasing.

この発明は上記実情に鑑みてなされたもので、
その目的は、回路全体の熱抵坑を効果的に下げる
ことができると共に耐熱性にも優れ、安定した動
作を行うことのできる混成集積回路を提供するこ
とにある。
This invention was made in view of the above circumstances.
The purpose is to provide a hybrid integrated circuit that can effectively lower the thermal resistance of the entire circuit, has excellent heat resistance, and can perform stable operation.

以下、図面を参照してこの発明の一実施例を説
明する。すなわち、この発明は前述の従来欠点を
除去する手段として、樹脂系絶縁層の代りに絶縁
性のセラミツクを金属基板上に連続的に堆積さ
せ、その上に回路を形成させようとするものであ
る。第4図において、11はパワートランジス
タ、12は高温半田層、13はCuブロツク層、
14は半田層、15はCu導体パターン、16は
金属酸化物、例えばAl2O3(アルミナ)の絶縁
層、17はAl基板、18は放熱板、19はねじ
である。
Hereinafter, one embodiment of the present invention will be described with reference to the drawings. That is, as a means to eliminate the above-mentioned conventional drawbacks, this invention attempts to continuously deposit insulating ceramic on a metal substrate instead of a resin-based insulating layer, and form a circuit thereon. . In FIG. 4, 11 is a power transistor, 12 is a high-temperature solder layer, 13 is a Cu block layer,
14 is a solder layer, 15 is a Cu conductor pattern, 16 is an insulating layer of metal oxide such as Al 2 O 3 (alumina), 17 is an Al substrate, 18 is a heat sink, and 19 is a screw.

上記Al2O3の絶縁層16の厚さを例えば100μ
mとした場合、前述の計算によると絶縁層16の
熱抵坑Rthは0.041℃/W(熱伝導率K=
0.260W/cm・℃)となり、従来の樹脂系絶縁層
(Rth=0.571℃/W)に比し約14分の1となる。
また耐熱性は1650℃と非常に高く、混成集積回路
の実用上なんら問題となることはない。さらに、
Al基板17とCu導体パターン15との間に存在
する浮遊容量は83pF/cm2となり、従来の樹脂系
絶縁層(140pF/cm2)と比較して大幅に減少で
き、回路の発振を防止し、歪率の改善をすること
が可能となる。
The thickness of the Al 2 O 3 insulating layer 16 is, for example, 100μ.
m, the thermal resistance Rth of the insulating layer 16 is 0.041°C/W (thermal conductivity K=
0.260W/cm・℃), which is approximately 1/14th of that of the conventional resin-based insulating layer (Rth=0.571℃/W).
Furthermore, its heat resistance is extremely high at 1,650°C, so it does not pose any practical problems for hybrid integrated circuits. moreover,
The stray capacitance that exists between the Al substrate 17 and the Cu conductor pattern 15 is 83 pF/cm 2 , which is significantly reduced compared to the conventional resin-based insulating layer (140 pF/cm 2 ), and prevents circuit oscillation. , it becomes possible to improve the distortion rate.

次に、上記混成集積回路の製造方法を説明す
る。まず、例えば厚さ2mmの純Al基板17の表
面を、Al2O3の粗い粉を吹き付けて10〜20μmに
荒す。しかる後、30分〜1時間以内にプラズマ溶
射装置(例えば第1メテコ社製のメテコ7M型)
を使つてAl2O3を100〜120μm堆積させ、絶縁層
16を形成させる。溶射はプラズマ溶射ガンと呼
ばれる電極間に不活性ガス、又は不活性ガスと水
素あるいはヘリウムとの混合ガスを流し、電気ア
ークを発生させガスを励起させ、1600℃まで調節
できる熱プラズマを生じさせる。この熱プラズマ
の発生した炎の中に平均粒度10μm程度のAl2O3
の粉を導入し、Al2O3を溶かした状態でAl基板1
7に付着させる。次に、Al2O3を100〜120μm堆
積したAl基板17上に、Cuペースト(例えばア
サヒ化学製のACP―030)を使つてスクリーン印
刷し、150℃で30分間焼成することによりCu導体
パターン15を形成する。そして、Cu入りの半
田層14を230℃のAl基板17上のCu導体パター
ン15上に付着させる。次に、例えば第5図に示
す回路図をAl基板17上に形成し、第4図に示
すように25cm×20cm×4cmのAl製無限大放熱板
18にシリコン・グリースを介してねじ19止め
する。
Next, a method of manufacturing the above hybrid integrated circuit will be explained. First, the surface of a pure Al substrate 17 with a thickness of 2 mm, for example, is roughened to 10 to 20 μm by spraying coarse powder of Al 2 O 3 . After that, within 30 minutes to 1 hour, use a plasma spraying device (for example, Metco 7M type manufactured by Daiichi Metco Co., Ltd.).
Al 2 O 3 is deposited to a thickness of 100 to 120 μm using a method to form an insulating layer 16 . Thermal spraying involves passing an inert gas, or a mixture of an inert gas and hydrogen or helium, between electrodes called a plasma spray gun, generating an electric arc and exciting the gas, creating a thermal plasma that can be adjusted up to 1600 degrees Celsius. In the flame generated by this thermal plasma, Al 2 O 3 with an average particle size of about 10 μm
Al substrate 1 was introduced with powder of Al 2 O 3 dissolved in it.
Attach it to 7. Next, on the Al substrate 17 on which Al 2 O 3 has been deposited to a thickness of 100 to 120 μm, a Cu paste (for example, ACP-030 manufactured by Asahi Chemical) is screen printed and baked at 150° C. for 30 minutes to form a Cu conductor pattern. form 15. Then, a solder layer 14 containing Cu is deposited on the Cu conductor pattern 15 on the Al substrate 17 at 230°C. Next, for example, the circuit diagram shown in FIG. 5 is formed on the Al substrate 17, and as shown in FIG. do.

第6図は従来の樹脂系絶縁層6を用いた場合と
上記Al2O3絶縁層16を用いた場合の両者のCuブ
ロツク層上の温度と出力電力との関係を示すもの
である。同図において、○イは樹脂系絶縁層6の場
合、○ロはAl2O3絶縁層16の場合である。これに
よると明らかに、Al2O3絶縁層16の方が樹脂系
絶縁層6より熱伝導のよいことがわかる(Cuブ
ロツク層上の温度で約10℃の差がある)。
FIG. 6 shows the relationship between the temperature on the Cu block layer and the output power when the conventional resin-based insulating layer 6 is used and when the Al 2 O 3 insulating layer 16 is used. In the same figure, ○A is the case of the resin-based insulating layer 6, and ○B is the case of the Al 2 O 3 insulating layer 16. This clearly shows that the Al 2 O 3 insulating layer 16 has better thermal conductivity than the resin-based insulating layer 6 (there is a difference of about 10° C. in temperature on the Cu block layer).

尚、上記実施例においては、絶縁層16として
金属酸化物のAl2O3(K=0.260W/cm・℃、εS
=9.4F/m)を用いて説明したが、他の金属酸
化物、例えばMgO・SiO2(ステアタイト;K=
0.025、εS=6.3)、2MgO・SiO2(フオルステラ
イト;K=0.034、εS=6.2)、ZrO2・SiO2(ジル
コン;K=0.050、εS=8.8)、MgO(マグネシ
ア;K=0.363、εS=5.6)、BeO(ベリリア;K
=1.173、εS=6.4)、TiO2(酸化チタン;K=
0.121、εS=8.6)等でもよい。また、金属酸化
物に限らず、金属窒化物、例えばAlN(窒化アル
ミニウム;K=0.60、εS=8.9)、BN(窒化ボロ
ン;K=0.287、εS=4.2)であつてもよい。
In the above embodiment, the insulating layer 16 is made of metal oxide Al 2 O 3 (K=0.260W/cm・℃, ε S
= 9.4F/m), but other metal oxides, such as MgO・SiO 2 (Steatite; K=
0.025, ε S = 6.3), 2MgO・SiO 2 (forsterite; K = 0.034, ε S = 6.2), ZrO 2・SiO 2 (zircon; K = 0.050, ε S = 8.8), MgO (magnesia; K = 0.363, ε S = 5.6), BeO (beryria; K
= 1.173, ε S = 6.4), TiO 2 (titanium oxide; K =
0.121, ε S = 8.6), etc. Furthermore, the material is not limited to metal oxides, but may also be metal nitrides, such as AlN (aluminum nitride; K=0.60, ε S =8.9) and BN (boron nitride; K=0.287, ε S =4.2).

以上のようにこの発明によれば、金属基板上に
絶縁性のセラミツクを溶射法により連続的に堆積
し、このセラミツク上に回路を形成させる構成と
したので、熱抵坑を著しく低下させることができ
ると共に耐熱性にも優れる。従つて、Cuブロツ
ク層の大きさを小さくでき、また素子の使用温度
範囲を高くすることができるために、混成集積回
路の大きさを従来のものより小型にすることが可
能となる。また、導体と基板間の浮遊容量が減少
するので、回路の安定性や歪率の改良に効果的で
あり、実用上極めて有効である。
As described above, according to the present invention, an insulating ceramic is continuously deposited on a metal substrate by a thermal spraying method, and a circuit is formed on this ceramic, so that thermal resistance can be significantly reduced. It also has excellent heat resistance. Therefore, the size of the Cu block layer can be reduced, and the operating temperature range of the device can be increased, so that the size of the hybrid integrated circuit can be made smaller than that of conventional circuits. Furthermore, since stray capacitance between the conductor and the substrate is reduced, it is effective in improving circuit stability and distortion rate, and is extremely effective in practice.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は従来の混成集積回路の構成を示す断面
図、第2図はパワートランジスタで発生した熱の
拡散状態を説明するための図、第3図a,bは上
記回路における浮遊容量の形成状態を説明するた
めのもので、aは絶縁層部の断面図、bは等価回
路図、第4図はこの発明の一実施例に係る混成集
積回路の構成を示す断面図、第5図は上記回路の
具体的な電気回路図、第6図は出力電力とCuブ
ロツク層の温度との関係を、第1図及び第4図に
それぞれ示した回路を比較して示す図である。 11…パワートランジスタ、12…高温半田
層、13…Cuブロツク層、14…半田層、15
…Cu導体パターン、16…絶縁層(Al2O3)、1
7…Al基板、18…放熱板。
Figure 1 is a cross-sectional view showing the configuration of a conventional hybrid integrated circuit, Figure 2 is a diagram illustrating the state of diffusion of heat generated in a power transistor, and Figures 3a and b are the formation of stray capacitance in the above circuit. 4 is a cross-sectional view showing the configuration of a hybrid integrated circuit according to an embodiment of the present invention, and FIG. 5 is a cross-sectional view of the insulating layer portion, b is an equivalent circuit diagram, and FIG. A specific electrical circuit diagram of the above circuit, FIG. 6, is a diagram showing the relationship between the output power and the temperature of the Cu block layer by comparing the circuits shown in FIGS. 1 and 4, respectively. DESCRIPTION OF SYMBOLS 11...Power transistor, 12...High temperature solder layer, 13...Cu block layer, 14...Solder layer, 15
...Cu conductor pattern, 16...Insulating layer (Al 2 O 3 ), 1
7...Al substrate, 18...heat sink.

Claims (1)

【特許請求の範囲】 1 金属基板と、 この金属基板上にプラズマ容射法により堆積形
成される絶縁性のセラミツク層と、 このセラミツク層上に形成される銅導体パター
ンと、 この銅導体パターン上に半田層を介して固着さ
れる銅ブロツク層と、 この銅ブロツク層上に半田層を介して固着され
る半導体素子とを具備したことを特徴とする混成
集積回路。
[Scope of Claims] 1. A metal substrate, an insulating ceramic layer deposited on the metal substrate by plasma spraying, a copper conductor pattern formed on the ceramic layer, and a copper conductor pattern formed on the copper conductor pattern. 1. A hybrid integrated circuit comprising: a copper block layer fixed to a semiconductor device through a solder layer; and a semiconductor element fixed onto the copper block layer via a solder layer.
JP55125783A 1980-09-10 1980-09-10 Hybrid integrated circuit Granted JPS5750455A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55125783A JPS5750455A (en) 1980-09-10 1980-09-10 Hybrid integrated circuit

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55125783A JPS5750455A (en) 1980-09-10 1980-09-10 Hybrid integrated circuit

Publications (2)

Publication Number Publication Date
JPS5750455A JPS5750455A (en) 1982-03-24
JPS6231828B2 true JPS6231828B2 (en) 1987-07-10

Family

ID=14918734

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55125783A Granted JPS5750455A (en) 1980-09-10 1980-09-10 Hybrid integrated circuit

Country Status (1)

Country Link
JP (1) JPS5750455A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63193547A (en) * 1987-02-06 1988-08-10 Showa Denko Kk Circuit board
JP5546889B2 (en) * 2010-02-09 2014-07-09 日本電産エレシス株式会社 Electronic component unit and manufacturing method thereof

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0015053A1 (en) * 1979-01-27 1980-09-03 LUCAS INDUSTRIES public limited company A method of manufacturing a semi-conductor power device assembly and an assembly thereby produced

Also Published As

Publication number Publication date
JPS5750455A (en) 1982-03-24

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