JPH0460329B2 - - Google Patents
Info
- Publication number
- JPH0460329B2 JPH0460329B2 JP58089634A JP8963483A JPH0460329B2 JP H0460329 B2 JPH0460329 B2 JP H0460329B2 JP 58089634 A JP58089634 A JP 58089634A JP 8963483 A JP8963483 A JP 8963483A JP H0460329 B2 JPH0460329 B2 JP H0460329B2
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor
- hot isostatic
- isostatic pressing
- porcelain
- temperature
- 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
Links
Landscapes
- Ceramic Capacitors (AREA)
- Insulating Bodies (AREA)
Description
産業上の利用分野
本発明は、理論密度比99%TD以上の高密度セ
ラミツクス及び結晶粒界強度の高いセラミツクス
を同時に得ることが可能な半導体セラミツクコン
デンサの製造方法に関するものである。
従来例の構成とその問題点
粒界誘電体層型半導体コンデンサは、半導体化
結晶間の粒界領域を高抵抗化し、結晶粒界に誘電
体層を設けたものである。この粒界層型は結晶粒
界近傍の10-2〜数μmを利用するものであり、結
晶粒界の状態にてコンデンサ特性が左右される。
従来の方式だと結晶粒界の結合強度が弱く、結晶
粒界に誘電体層を設けた場合、誘電体層の厚みバ
ラツキや誘電体層の強度が弱く、耐電圧特性、誘
電損失等が悪いものであつた。
また、酸化性雰囲気中にて焼成した誘電体磁器
を還元性粉末中にて熱間静水圧プレスをし、半導
体磁器と緻密なセラミツクスを同時に得る方法も
あるが、半導体化の雰囲気コントロールが非常に
困難であり、品質の安定性及び製品歩留りが悪い
ものである。
また、半導体磁器の粒界に誘電体層を設けた後
に熱間静水圧プレスをすることもあるが、この方
式では熱間静水圧プレス条件の温度が常に拡散処
理温度以下でなければならないため、拡散温度が
(焼結温度−300℃)より低い場合、熱間静水圧プ
レス効果が出ないという欠点がある。
発明の目的
本発明は従来の欠点を除去し、理論密度比99%
TD以上の高密度セラミツクス及び結晶粒界強度
の高いセラミツクスを同時に得ることが可能であ
り、高い耐電圧特性、低い誘電損失、さらに優れ
た機械特性を与える半導体セラミツクコンデンサ
の製造方法を提供することを目的とするものであ
る。
発明の構成
上記目的を達成するために、本発明は還元性雰
囲気焼成にて半導体化した磁器を、熱間静水圧プ
レスし、然る後に前記半導体磁器の粒界に拡散剤
を熱拡散させ誘電体層を形成させるもので、高い
耐電圧特性、低い誘電損失、さらに優れた機械特
性を与える粒界誘電体層型半導体セラミツクコン
デンサを得ることができた。
実施例の説明
以下本発明について一実施例とともに説明す
る。試料の調整工程では、半導体磁気組成とし
て、市販の工業用原料SrCO3粉末(純度99.9%以
上)、TiO2粉末(純度99.9%以上)、及び市販の
試薬特級Nb2O5の各粉末を第1表の組成比になる
よう配合し、不純物混入防止のためウレタン内張
ポツトを用いて湿式混合し、乾燥した後1200℃の
温度で仮焼成した。
第 1 表
半導体磁器組成(モル%)
SrCO3 TiO2 Nb2O5
50.10 49.85 0.05
この仮焼成を湿式粉砕し、乾燥した後、ポリビ
ニルアルコール水溶液をバインダにして混合し、
32メツシユパスに整粒した。この整粒粉を直径13
mm、厚さ0.5mmの円板形に1t/cm2の加圧力で成形
し、これらの成形体を空気中1000℃で加熱処理し
た後に、90%N2−10%H2の混合ガス気流中にお
いて1400℃の温度で3時間焼成し半導体磁器を得
た。
その後、前記半導体磁器をArガス中にて熱間
静水圧プレスする。この時のプレス条件と磁器の
理論密度比、平均結晶粒径の関係を第1図、第2
図に示す。
次に拡散剤として、組成としてはBi2O3−Cu2
O系のペースト状のものを用い、該半導体磁器素
子表面にむらなく塗布した。以上のように拡散剤
を塗布した半導体磁器素子を大気下1100℃の温度
にて拡散処理を行つた。
このようにして得られた粒界誘電体層型半導体
磁器の円板形素子の両面にAg電極を焼付けてコ
ンデンサ素子とし、誘電率εa(測定周波数1KHz)
誘電体損失tanδ(1KHz)、昇圧破壊電圧Vb(V/
mm)及びビツカース硬度Hv(Kg/mm2,500g,15秒
荷重)を測定した。その結果を第2表に示す。こ
こで比較試料No.11は熱間静水圧プレス処理工程を
通さない従来の粒界誘電体層型セラミツクコンデ
ンサである。
第3図に熱間静水圧プレス前の半導体磁器の平
均結晶粒径と熱間静水圧プレス効果の関係を示
す。この図をみると、熱間静水圧プレス効果は結
晶粒径に左右され、50μmを超えると熱間静水圧
プレスがかかりにくくなる傾向にある。
本発明によるとNo.1〜No.7の試料を比較試料No.
11と比較すると、εaで約60%、Vbで約40%、Hv
で約30%アツプし、tanδで約60%ダウンするなど
の優れたコンデンサ特性が得られる。No.8〜No.10
の試料は発明外の比較例のものであり、本発明の
特性より劣るものである。
INDUSTRIAL APPLICATION FIELD The present invention relates to a method for manufacturing a semiconductor ceramic capacitor that can simultaneously produce high-density ceramics with a theoretical density ratio of 99% TD or higher and ceramics with high grain boundary strength. Structure of conventional example and its problems A grain boundary dielectric layer type semiconductor capacitor has a grain boundary region between semiconductor crystals with high resistance, and a dielectric layer is provided at the grain boundary. This grain boundary layer type utilizes the area of 10 -2 to several μm near the grain boundaries, and the capacitor characteristics are influenced by the state of the grain boundaries.
In the conventional method, the bonding strength of the grain boundaries is weak, and when a dielectric layer is provided at the grain boundaries, the thickness of the dielectric layer varies, the strength of the dielectric layer is weak, and the withstand voltage characteristics and dielectric loss are poor. It was hot. There is also a method of hot isostatically pressing dielectric porcelain fired in an oxidizing atmosphere in reducing powder to obtain semiconductor porcelain and dense ceramics at the same time, but it is difficult to control the atmosphere for semiconductor production. It is difficult, and the quality stability and product yield are poor. In addition, hot isostatic pressing is sometimes performed after providing a dielectric layer at the grain boundaries of semiconductor porcelain, but in this method, the temperature under hot isostatic pressing conditions must always be below the diffusion treatment temperature. If the diffusion temperature is lower than (sintering temperature - 300°C), there is a drawback that the hot isostatic pressing effect is not produced. Purpose of the invention The present invention eliminates the conventional drawbacks and achieves a theoretical density ratio of 99%.
It is an object of the present invention to provide a method for manufacturing a semiconductor ceramic capacitor that can simultaneously obtain high-density ceramics of TD or higher and ceramics with high grain boundary strength, and that provides high withstand voltage characteristics, low dielectric loss, and excellent mechanical properties. This is the purpose. Structure of the Invention In order to achieve the above object, the present invention hot isostatically presses porcelain made into a semiconductor by firing in a reducing atmosphere, and then thermally diffuses a diffusing agent into the grain boundaries of the semiconductor porcelain to create a dielectric material. By forming a dielectric layer, we were able to obtain a grain boundary dielectric layer type semiconductor ceramic capacitor that provides high withstand voltage characteristics, low dielectric loss, and excellent mechanical properties. DESCRIPTION OF EMBODIMENTS The present invention will be described below along with one embodiment. In the sample preparation process, commercially available industrial raw materials SrCO 3 powder (purity 99.9% or higher), TiO 2 powder (purity 99.9% or higher), and commercially available reagent grade Nb 2 O 5 powder were used as the semiconductor magnetic composition. The compositions were blended to have the composition ratios shown in Table 1, wet mixed using a urethane-lined pot to prevent contamination with impurities, dried, and then pre-fired at a temperature of 1200°C. Table 1 Semiconductor porcelain composition (mol%) SrCO 3 TiO 2 Nb 2 O 5 50.10 49.85 0.05 After wet-pulverizing this pre-fired material and drying it, a polyvinyl alcohol aqueous solution was used as a binder and mixed.
The grain size was adjusted to 32 meters. This sized powder has a diameter of 13
mm and 0.5 mm thick under a pressure of 1 t/cm 2 , and after heat-treating these molded bodies in air at 1000°C, a mixed gas stream of 90% N 2 -10% H 2 was applied. Semiconductor porcelain was obtained by firing for 3 hours at a temperature of 1400°C. Thereafter, the semiconductor porcelain is hot isostatically pressed in Ar gas. The relationship between the pressing conditions at this time, the theoretical density ratio of the porcelain, and the average grain size is shown in Figures 1 and 2.
As shown in the figure. Next, as a diffusing agent, the composition is Bi 2 O 3 −Cu 2
An O-based paste was used and evenly applied to the surface of the semiconductor ceramic element. The semiconductor ceramic element coated with the diffusing agent as described above was subjected to a diffusion treatment at a temperature of 1100° C. in the atmosphere. Ag electrodes were baked on both sides of the disk-shaped element of the grain boundary dielectric layer type semiconductor porcelain obtained in this way to form a capacitor element, and the dielectric constant ε a (measurement frequency 1 KHz)
Dielectric loss tanδ (1KHz), boost breakdown voltage V b (V/
mm) and Bitkers hardness Hv (Kg/mm 2 , 500g, 15 seconds load) were measured. The results are shown in Table 2. Here, comparative sample No. 11 is a conventional grain boundary dielectric layer type ceramic capacitor that is not subjected to the hot isostatic pressing process. FIG. 3 shows the relationship between the average crystal grain size of semiconductor porcelain before hot isostatic pressing and the hot isostatic pressing effect. Looking at this figure, the effect of hot isostatic pressing depends on the crystal grain size, and when the grain size exceeds 50 μm, hot isostatic pressing tends to be difficult to apply. According to the present invention, samples No. 1 to No. 7 are compared to comparative sample No.
11, about 60% for ε a , about 40% for Vb, Hv
Excellent capacitor characteristics can be obtained with approximately 30% increase in tan δ and approximately 60% decrease in tan δ. No.8~No.10
The sample is a comparative example outside the invention and has characteristics inferior to those of the present invention.
【表】【table】
【表】
熱間静水圧プレス条件においては、第1図に示
すように1100℃未満では圧力効果が急激に減少
し、300気圧未満では温度効果が減少し、ともに
高密度(99%TD以上)を得ることが出来ない。
従つて拡散処理後熱間静水圧プレスする従来例で
は、拡散処理温度が1100℃未満では熱間静水圧プ
レス効果が出て来ない。また第2図に示すよう
に、半導体磁器の平均結晶粒径は熱間静水圧プレ
ス温度に依存し、熱間静水圧プレス圧力にはあま
り依存せず、熱間静水圧プレス温度が焼成温度
(図では1400℃)をオーバーすると急激に粒成長
し、第2表のNo.10の結果からもわかるように、コ
ンデンサ特性が劣化する。
すなわち、焼成温度をT℃とすると、熱間静水
圧プレス温度が(T−300)℃未満では磁器密度
の上昇が認められず、T℃を超えると粒成長が促
進されるとともに異相析出等が起こり、コンデン
サ特性が劣化する。また熱間静水圧プレス圧力が
300気圧未満では磁器密度の上昇は認められない。
また、従来例の酸化性雰囲気中にて焼成した誘
電体磁器を還元性粉末中にて熱間静水圧プレスす
る方式は、還元性粉末の種類、量及び熱間静水圧
プレス温度によりコンデンサ特性がばらつき、製
品歩留りが約30〜40%となり、本発明品の歩留り
が約70%であるのに対し、40〜60%ダウンするな
どの欠点がある。
発明の効果
以上本発明によれば、次のような効果がもたら
される。
(1) 理論密度比99%TD以上の高密度セラミツク
スが得られる。
(2) コンデンサ特性が向上し、安定化する。
(3) 製品歩留りが向上する。
(4) 結晶粒界に析出したポアがなくなり、結晶粒
界強度等が強化できる。
このように、本発明の半導体セラミツクコンデ
ンサの製造方法は非常に優れた性能を備えてお
り、工業的量産化においても著しく安定であり、
産業的価値の大なるものである。[Table] Under hot isostatic pressing conditions, as shown in Figure 1, the pressure effect decreases rapidly below 1100℃, and the temperature effect decreases below 300 atm, both of which result in high density (over 99% TD). I can't get it.
Therefore, in the conventional example of hot isostatic pressing after diffusion treatment, the hot isostatic pressing effect cannot be obtained if the diffusion treatment temperature is less than 1100°C. In addition, as shown in Figure 2, the average grain size of semiconductor porcelain depends on the hot isostatic pressing temperature, but does not depend much on the hot isostatic pressing pressure, and the hot isostatic pressing temperature is the firing temperature ( When the temperature exceeds 1400°C (in the figure), grain growth occurs rapidly, and as can be seen from the results in No. 10 in Table 2, the capacitor characteristics deteriorate. In other words, when the firing temperature is T°C, no increase in porcelain density is observed when the hot isostatic pressing temperature is below (T-300)°C, and when it exceeds T°C, grain growth is promoted and foreign phase precipitation occurs. This causes deterioration of capacitor characteristics. In addition, the hot isostatic press pressure
No increase in porcelain density is observed below 300 atm. In addition, in the conventional method of hot isostatic pressing dielectric porcelain fired in an oxidizing atmosphere into reducing powder, capacitor characteristics vary depending on the type and amount of reducing powder and the hot isostatic pressing temperature. There are disadvantages such as variation and product yield of about 30 to 40%, which is 40 to 60% lower than the yield of the product of the present invention, which is about 70%. Effects of the Invention According to the present invention, the following effects are brought about. (1) High-density ceramics with a theoretical density ratio of 99% TD or higher can be obtained. (2) Capacitor characteristics are improved and stabilized. (3) Product yield is improved. (4) Pores precipitated at grain boundaries are eliminated, and grain boundary strength can be strengthened. As described above, the method for manufacturing semiconductor ceramic capacitors of the present invention has extremely excellent performance and is extremely stable even in industrial mass production.
It has great industrial value.
第1図は本発明の一実施例を説明するための熱
間静水圧プレス(HIP)条件と理論密度比の関係
を示す図、第2図及び第3図は本発明の一実施例
を説明するための熱間静水圧プレス条件と平均結
晶粒子径の関係を示す図である。
Figure 1 is a diagram showing the relationship between hot isostatic pressing (HIP) conditions and theoretical density ratio to explain an embodiment of the present invention, and Figures 2 and 3 are diagrams to explain an embodiment of the present invention. FIG. 3 is a diagram showing the relationship between hot isostatic pressing conditions and average crystal grain size for achieving the desired results.
Claims (1)
T℃にて焼成して半導体磁器を作り、この半導体
磁器を(T−300)℃〜T℃,300気圧以上の気圧
下で熱間静水圧プレスした後、前記半導体磁器の
粒界に拡散剤を熱拡散させることを特徴とする半
導体セラミツクコンデンサの製造方法。 2 還元性雰囲気中T℃にて焼成した半導体磁器
の平均結晶粒径が50μm以下であることを特徴と
する特許請求の範囲第1項記載の半導体セラミツ
クコンデンサの製造方法。[Claims] 1. Semiconductor porcelain is produced by shaping the raw material into any desired shape and firing it at T°C in a reducing atmosphere, and then heating the semiconductor porcelain at (T-300)°C to T°C at a temperature of 300 atmospheres or more. A method for manufacturing a semiconductor ceramic capacitor, which comprises hot isostatic pressing under atmospheric pressure and then thermally diffusing a diffusing agent into the grain boundaries of the semiconductor ceramic. 2. The method for manufacturing a semiconductor ceramic capacitor according to claim 1, wherein the average crystal grain size of the semiconductor ceramic fired at T° C. in a reducing atmosphere is 50 μm or less.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58089634A JPS59214213A (en) | 1983-05-20 | 1983-05-20 | Method of producing semiconductor ceramic capacitor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58089634A JPS59214213A (en) | 1983-05-20 | 1983-05-20 | Method of producing semiconductor ceramic capacitor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59214213A JPS59214213A (en) | 1984-12-04 |
| JPH0460329B2 true JPH0460329B2 (en) | 1992-09-25 |
Family
ID=13976194
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58089634A Granted JPS59214213A (en) | 1983-05-20 | 1983-05-20 | Method of producing semiconductor ceramic capacitor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59214213A (en) |
-
1983
- 1983-05-20 JP JP58089634A patent/JPS59214213A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59214213A (en) | 1984-12-04 |
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