JPH0153496B2 - - Google Patents

Info

Publication number
JPH0153496B2
JPH0153496B2 JP58089635A JP8963583A JPH0153496B2 JP H0153496 B2 JPH0153496 B2 JP H0153496B2 JP 58089635 A JP58089635 A JP 58089635A JP 8963583 A JP8963583 A JP 8963583A JP H0153496 B2 JPH0153496 B2 JP H0153496B2
Authority
JP
Japan
Prior art keywords
porcelain
semiconductor
hot isostatic
isostatic pressing
semiconductor ceramic
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
JP58089635A
Other languages
Japanese (ja)
Other versions
JPS59214214A (en
Inventor
Takehiko Yoneda
Hiromitsu Tagi
Masanori Fujimura
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP58089635A priority Critical patent/JPS59214214A/en
Publication of JPS59214214A publication Critical patent/JPS59214214A/en
Publication of JPH0153496B2 publication Critical patent/JPH0153496B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Ceramic Capacitors (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

産業上の利用分野 本発明は、セラミツクス内部の空孔が0のとき
の密度(理論密度)に対する実際の密度の比であ
る理論密度比が99%TD(Theoretical Density)
以上の場合の高密度セラミツクスを得ることが可
能な還元再酸化型半導体磁器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 従来の還元再酸化型半導体磁器コンデンサの製
造方法は、まず大気中焼成により誘電体磁器を作
り、それを1〜2気圧下の高温還元雰囲気処理に
より磁器全体を半導体化し、さらに再酸化処理に
より磁器の表面近傍のみを絶縁体化するという三
段熱処理を必要とする。この還元再酸化型半導体
磁器コンデンサは表面層約1〜40μmを利用する
ものであるから、この電気特性は内圧ポア(セラ
ミツクス内部に存在する空孔)に著しく左右され
る。従来の方式と、ポア分布(内在ポアの分布)
を悪くする因子(原料粒度、原料結晶相、異物有
機バインダ成分、成型圧等)が多く、理論密度比
94%TD〜98%TDが限界であり、99%TD以上は
不可能に近いものであつた。そのため、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(HIP)
し、半導体磁器と緻密なセラミツクスを同時に得
た後、再酸化処理する方法もあるが、還元性粉末
による半導体化の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(熱間静水圧プレスの参考文献:産業技術セン
ター発行、セラミツクス材料技術集成P684〜
P688)。 発明の目的 本発明は従来の欠点を除去し、最大ポア径3μ
m以下というポアレスセラミツクス、高い耐電圧
特性、低い誘電損失、高い品質安定性、さらに優
れた歩留りを与える還元再酸化型半導体磁器コン
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
囲気中にて熱処理して得た半導体磁器を熱間静水
圧プレスし、さらにこの半導体磁器表面を再酸化
処理するもので、高い耐電圧特性、低い誘電損
失、高い品質安定性さらに優れた歩留りを与える
還元再酸化型半導体磁器コンデンサを得ることが
できた。 実施例の説明 以下本発明の実施例を図面に基づいて説明す
る。 実施例 1 試料の調整工程では、半導体磁器組成として、
市販の工業用原料BaCO3粉末(純度99.9%以上)、
TiO2粉末(純度99.9%以上)、Nd2O3粉末(純度
99.9%以上)、及び市販の試薬特級MnO2の各粉末
を第1表の組成比になるように配合し、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、1150℃の温度で4時間仮焼成
した。この仮焼物を湿式粉砕し、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13mm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において1300℃の
温度で2時間焼成し、然る後に90%N2−10%H2
混合ガス中1100℃にて半導体磁器を得た。 第1表 半導体磁器組成(モル%) BaO Nd2O3 TiO2 MnO2 48.65 0.68 50.37 0.3 その後前記半導体磁器をAr中にて熱間静水圧
プレスする。この時の、熱間静水圧プレス条件と
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。 このようにして得られた還元再酸化型半導体磁
器を空気中において900℃の温度で加圧処理した。
この還元再酸化型半導体磁器の両面に銀電極を焼
付けてコンデンサ素子とし、その単位面積当りの
容量C(測定周波数1KHz)、誘電体損失tanδ(1K
Hz)、絶縁抵抗IR(測定時の印加電圧:直流50V)、
破壊電圧Vb、500g荷重を15秒間かけた際のビツ
カース硬度Hv(Kg/mm2)を測定した。その結果を
第2表に示す。ここで比較試料No.8は熱間静水圧
プレス処理しない試料で作る。 本発明によるNo.1〜No.5の試料を比較試料No.8
と比較すると、IRで約40%、Vbで約55%、Cで
約15%アツプし、tanδでは約40%ダウンするなど
の優れたコンデンサ特性が得られる。No.6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 has a theoretical density ratio of 99% TD (Theoretical Density), which is the ratio of the actual density to the density when there are no pores inside the ceramic (theoretical density).
The present invention relates to a method for manufacturing a reduction and reoxidation type semiconductor ceramic capacitor that can produce high-density ceramics in the above case. Structure of conventional example and its problems The conventional manufacturing method for reducing and reoxidizing semiconductor ceramic capacitors is to first make dielectric ceramic by firing in the air, and then process it in a high-temperature reducing atmosphere at 1 to 2 atmospheres to convert the entire ceramic into a semiconductor. It requires a three-step heat treatment to convert the porcelain into an insulator, and then re-oxidize the surface of the porcelain to make it an insulator. Since this reduction/reoxidation type semiconductor ceramic capacitor utilizes a surface layer of about 1 to 40 μm, its electrical characteristics are significantly influenced by internal pressure pores (vacancies existing inside the ceramic). Conventional method and pore distribution (distribution of intrinsic pores)
The theoretical density ratio
The limit was 94% TD to 98% TD, and 99% TD or higher was nearly impossible. Therefore, the withstand voltage characteristics, dielectric loss, etc. were poor. In addition, dielectric porcelain fired in an oxidizing atmosphere is hot isostatically pressed (HIP) in reducing powder.
However, there is a method in which semiconducting porcelain and dense ceramics are obtained at the same time and then subjected to reoxidation treatment, but it is extremely difficult to control the semiconducting process using reducing powder, resulting in poor quality stability and product yield. (Hot isostatic press reference: Published by Industrial Technology Center, Ceramics Materials Technology Collection P684~
P688). Purpose of the invention The present invention eliminates the conventional drawbacks and provides a maximum pore diameter of 3 μm.
The object of the present invention is to provide a method for manufacturing a reduction and reoxidation type semiconductor ceramic capacitor that provides poreless ceramics with a diameter of less than m, high withstand voltage characteristics, low dielectric loss, high quality stability, and excellent yield. Structure of the Invention In order to achieve the above object, the present invention hot isostatically presses semiconductor porcelain obtained by heat treatment in a reducing atmosphere, and further subjects the surface of this semiconductor porcelain to reoxidation treatment, thereby achieving high durability. We were able to obtain a reduction-reoxidation type semiconductor ceramic capacitor that has excellent voltage characteristics, low dielectric loss, high quality stability, and excellent yield. DESCRIPTION OF EMBODIMENTS Hereinafter, embodiments of the present invention will be described based on the drawings. Example 1 In the sample preparation process, the semiconductor ceramic composition was as follows:
Commercially available industrial raw material BaCO 3 powder (purity 99.9% or more),
TiO 2 powder (purity 99.9% or more), Nd 2 O 3 powder (purity
99.9% or more) and commercially available reagent grade MnO 2 powder to the composition ratio shown in Table 1, wet-mixed using a urethane-lined pot to prevent contamination with impurities, and dried. Temporary firing was performed at a temperature of 4 hours. This calcined product was wet-pulverized, dried, mixed with an aqueous polyvinyl alcohol solution as a binder, and sized into 32 mesh passes. This sized powder was molded into a disk shape with a diameter of 13 mm and a thickness of 0.5 mm using a pressure of 1 t/cm 2 , and these molded bodies were fired in air at a temperature of 1300°C for 2 hours, and then 90% N2 −10% H2
Semiconductor porcelain was obtained at 1100°C in a mixed gas. Table 1 Semiconductor porcelain composition (mol %) BaO Nd 2 O 3 TiO 2 MnO 2 48.65 0.68 50.37 0.3 Thereafter, the semiconductor porcelain was hot isostatically pressed in Ar. At this time, the relationship between the hot isostatic pressing conditions, the theoretical density ratio of the porcelain, and the average grain size was determined as follows.
It is shown in Fig. 2. The thus obtained reduced and reoxidized semiconductor porcelain was subjected to pressure treatment in air at a temperature of 900°C.
Silver electrodes are baked on both sides of this reduction and reoxidation type semiconductor porcelain to make a capacitor element, and its capacitance per unit area C (measurement frequency 1KHz) and dielectric loss tanδ (1K
Hz), insulation resistance IR (applied voltage during measurement: 50V DC),
Breakdown voltage Vb and Vickers hardness Hv (Kg/mm 2 ) when a load of 500 g was applied for 15 seconds were measured. The results are shown in Table 2. Here, comparative sample No. 8 is made from a sample that is not subjected to hot isostatic pressing. Samples No. 1 to No. 5 according to the present invention were compared to sample No. 8.
Compared to the previous model, excellent capacitor characteristics can be obtained, such as an increase in IR of about 40%, a rise in Vb of about 55%, a rise in C of about 15%, and a decrease in tanδ of about 40%. Sample No. 6 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、1000℃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)を得ることが出来ない。ま
た、第2図に示すように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
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1300℃)をオーバーすると急激に粒成
長し、第2表のNo.7の試料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、第4図に
示すように、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気圧未満では磁器の密度
の上昇が認められない。 第3図に熱間静水圧プレス前の半導体磁器平均
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。 実施例 2 資料の調整工程、組成、成形までは実施例1で
述べた通りである。この成形体を90%N2−10%
H2混合ガス中において1300℃の温度で2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中にて熱間静水圧プレスする。 このようにして得られた還元再酸化型半導体磁
器を空気中において900℃の温度で加熱処理した。
この還元再酸化型半導体磁器を実施例1と同様の
方法で特性等を調べた所、実施例1と非常に近い
特性が得られた。 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50〜60%となり、本発明の歩留りが
約90%であるのに対し、40%ダウンするなど欠点
がある。 また、上述した第4図の還元再酸化型半導体磁
器コンデンサ焼成温度を基準とした熱間静水圧プ
レス温度と理論密度比との関係をみると、熱間静
水圧プレスの限界は焼成温度T℃より300℃低い
温度がその下限値となつていることがわかる。 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以上高密度磁器が得られ
る。 (2) 磁器の半導体化コントロールが容易に雰囲気
で行なわれる。 (3) 製品歩留りが向上する。 (4) ポア分布が改良され、最大3μmのレベルに
なる。 (5) コンデンサ特性が向上し、安定化する。 このように、本発明の還元再酸化型半導体磁器
コンデンサの製造方法は非常に優れた特性を備え
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 1000℃, and the temperature effect decreases below 300 atm. ) cannot be obtained. In addition, as shown in Figure 2, the average grain size depends on the hot isostatic pressing temperature and does not depend much on the hot isostatic pressing pressure. ), grains grow rapidly and, as can be seen from the results of sample No. 7 in Table 2, the capacitor characteristics deteriorate. That is, if the firing temperature is T°C, then the hot isostatic pressing temperature is T-300°C, as shown in Figure 4.
If it is less than T.degree. C., no increase in porcelain density will be observed, and if it exceeds T.degree. C., grain growth will be promoted and foreign phase precipitation will occur, resulting in deterioration of capacitor characteristics. Further, when the hot isostatic pressing pressure is less than 300 atm, no increase in the density of the porcelain is observed. 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. Example 2 The material preparation process, composition, and molding were as described in Example 1. This molded body is 90%N 2 -10%
Semiconductor porcelain was obtained by firing in H 2 mixed gas at a temperature of 1300° C. for 2 hours. Thereafter, the semiconductor porcelain is hot isostatically pressed in Ar. The thus obtained reduced and reoxidized semiconductor porcelain was heat treated in air at a temperature of 900°C.
When the characteristics of this reduced and reoxidized semiconductor ceramic were examined in the same manner as in Example 1, characteristics very similar to those in Example 1 were obtained. 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. This method has drawbacks such as variation and product yield of about 50 to 60%, which is 40% lower than the yield of the present invention, which is about 90%. Furthermore, looking at the relationship between the hot isostatic pressing temperature and the theoretical density ratio based on the firing temperature of the reduction-reoxidation type semiconductor porcelain capacitor shown in Fig. 4 mentioned above, the limit of hot isostatic pressing is the firing temperature T°C. It can be seen that the lower limit is 300°C lower than that. Effects of the Invention According to the present invention, the following effects are brought about. (1) High-density porcelain with a theoretical density ratio of 99% TD or higher can be obtained. (2) Semiconductorization of porcelain can be easily controlled in the atmosphere. (3) Product yield is improved. (4) Pore distribution has been improved to a maximum level of 3 μm. (5) Capacitor characteristics are improved and stabilized. As described above, the method for manufacturing a reduction and reoxidation type semiconductor ceramic capacitor of the present invention has very excellent characteristics, is extremely stable even in industrial mass production, and has great industrial value.

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

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
を示す特性図、第2図、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
結晶粒径の関係を示す図、第4図は本発明の一実
施例を説明するための還元再酸化型半導体磁器コ
ンデンサ焼成温度を基準とした熱間静水圧温度と
理論密度比の関係を示す図である。
Fig. 1 is a characteristic diagram showing the relationship between hot isostatic pressing (HIP) conditions and theoretical density ratio to explain an embodiment of the present invention, and Figs. 2 and 3 show an embodiment of the present invention. A diagram showing the relationship between hot isostatic pressing conditions and average grain size for explanation, and FIG. 4 is a diagram showing the relationship between hot isostatic pressing conditions and average crystal grain size. FIG. 3 is a diagram showing the relationship between hydrostatic pressure temperature and theoretical density ratio.

Claims (1)

【特許請求の範囲】 1 還元性雰囲気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、
前記半導体磁器表面を再酸化することを特徴とす
る還元再酸化型半導体磁器コンデンサの製造方
法。 2 還元性雰囲気下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項記載の還元再酸化型半
導体磁器コンデンサの製造方法。 3 大気中T℃にて焼成し誘電体磁器を作り、こ
の誘電体磁器を還元性雰囲気下にて熱処理して半
導体化した後、この半導体磁器を(T−300)℃
〜T℃、300以上の気圧下で熱間静水圧プレスし、
さらに前記半導体磁器表面を再酸化処理すること
を特徴とする還元再酸化型半導体磁器コンデンサ
の製造方法。 4 大気中T℃にて焼成した誘電体磁器の平均結
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3項記載の還元再酸化型半導体磁器
コンデンサの製造方法。
[Claims] 1. Semiconductor porcelain is produced by firing in a reducing atmosphere T°C, and this semiconductor porcelain is heated at (T-300)°C to T°C,
After hot isostatic pressing under pressure of over 300 atmospheres,
A method for manufacturing a reduction and reoxidation type semiconductor ceramic capacitor, comprising reoxidizing the surface of the semiconductor ceramic. 2. The method for manufacturing a reduced and reoxidized 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. 3 Firing in the air at T°C to produce dielectric porcelain, heat-treating this dielectric porcelain in a reducing atmosphere to convert it into a semiconductor, and then converting this semiconductor porcelain to (T-300)°C.
Hot isostatic pressing at ~T°C and pressure of 300 or more,
A method for manufacturing a reduction and reoxidation type semiconductor ceramic capacitor, further comprising subjecting the semiconductor ceramic surface to a reoxidation treatment. 4. The method for manufacturing a reduction and reoxidation type semiconductor ceramic capacitor according to claim 3, wherein the average crystal grain size of the dielectric ceramic fired at T° C. in the atmosphere is 50 μm or less.
JP58089635A 1983-05-20 1983-05-20 Method of producing semiconductor ceramic capacitor Granted JPS59214214A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58089635A JPS59214214A (en) 1983-05-20 1983-05-20 Method of producing semiconductor ceramic capacitor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58089635A JPS59214214A (en) 1983-05-20 1983-05-20 Method of producing semiconductor ceramic capacitor

Publications (2)

Publication Number Publication Date
JPS59214214A JPS59214214A (en) 1984-12-04
JPH0153496B2 true JPH0153496B2 (en) 1989-11-14

Family

ID=13976224

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58089635A Granted JPS59214214A (en) 1983-05-20 1983-05-20 Method of producing semiconductor ceramic capacitor

Country Status (1)

Country Link
JP (1) JPS59214214A (en)

Also Published As

Publication number Publication date
JPS59214214A (en) 1984-12-04

Similar Documents

Publication Publication Date Title
US4477401A (en) Method of manufacturing a dielectric
US4785375A (en) Temperature stable dielectric composition at high and low frequencies
JPH0715856B2 (en) Multilayer ceramic capacitor and manufacturing method thereof
JPH0153495B2 (en)
JPS6053408B2 (en) Reduced semiconductor ceramic composition
JPH0153493B2 (en)
JPH0460329B2 (en)
KR940011059B1 (en) Semiconductor condenser
JPS6128209B2 (en)
JPH06102573B2 (en) Composition for reduction / reoxidation type semiconductor ceramic capacitor
JP3562085B2 (en) Dielectric ceramic composition, capacitor using the same, and method for producing dielectric ceramic composition
KR100310275B1 (en) Process for Preparing PFN Dielectric Ceramics with High Dielectric Constant and Low Dielectric Loss
JPH0159728B2 (en)
JPS59214214A (en) Method of producing semiconductor ceramic capacitor
JPS6115529B2 (en)
JPS6120504B2 (en)
KR950014718B1 (en) Dielectric ceramic composition for electromagnetic interference filter and manufacturing method thereof
JPS6128208B2 (en)
JPS6357931B2 (en)
JP2734888B2 (en) Method for producing semiconductor porcelain composition
JPS6235256B2 (en)
JPH0153494B2 (en)
JPH05326320A (en) Thin film chip capacitor
JPS633442B2 (en)
JPS6332744B2 (en)