JPH0524647B2 - - Google Patents
Info
- Publication number
- JPH0524647B2 JPH0524647B2 JP12764489A JP12764489A JPH0524647B2 JP H0524647 B2 JPH0524647 B2 JP H0524647B2 JP 12764489 A JP12764489 A JP 12764489A JP 12764489 A JP12764489 A JP 12764489A JP H0524647 B2 JPH0524647 B2 JP H0524647B2
- Authority
- JP
- Japan
- Prior art keywords
- semiconductor ceramic
- diffusion
- grain boundary
- semiconductor
- substance
- 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 - Lifetime
Links
Landscapes
- Ceramic Capacitors (AREA)
Description
〔産業上の利用分野〕
本発明は、半導体磁器の表面に拡散物質を付着
させて該拡散物質を粒界層に熱拡散し、該粒界層
を再酸化する粒界絶縁型半導体磁器コンデンサの
製造方法に関する。
〔従来の技術〕
粒界絶縁型半導体磁器コンデンサは、半導体化
した磁器の結晶粒界を高抵抗化し、該結晶粒界を
誘電体として利用するものであり、その誘電特性
は結晶粒界近傍の数μm程度の絶縁体層の状態に
依存している。
一般に半導体磁器は、チタン酸ストロンチウム
又はチタン酸バリウムを主成分とし、原子価制御
元素と呼ばれるニオブ、タンタル、アンチモン又
は希土類元素等の元素のうち一種以上を含有せし
めた組成物を、所望の形状に成形して中性又は還
元性雰囲気中で焼成することにより得られる。
そして従来、このようにして得られた半導体磁
器の結晶粒界を絶縁体化する手段としては、大気
中で熱処理して粒界層を再酸化する方法、又は粒
界に拡散しやすく原子価を補償する粒界拡散物
質、例えば銅、ビスマス、鉛又はマンガン等の元
素のうち一種以上を半導体磁器表面に印刷等の手
段により付着せしめた後大気中で熱処理を行い、
前記粒界拡散物質を粒界層に拡散せしめると同時
に前記粒界層の再酸化を行う方法が一般的であ
る。
〔発明が解決しようとする課題〕
しかしながら上述した粒界絶縁体化工程におい
て、拡散物質を用いず大気中で熱処理して粒界層
を再酸化する方法では、得られたコンデンサの絶
縁抵抗値又は絶縁破壊電圧値が低いという欠点を
有していた。
一方、銅、ビスマス、鉛又はマンガン等の拡散
物質を用い熱拡散する方法では、上述した如く前
記拡散物質の粒界層への熱拡散と該粒界層の再酸
化とを同時に行うため、拡散物質を粒界層に十分
拡散させるには長時間の熱処理が必要であつた。
そしてこのことによつて、半導体磁器表面近傍の
結晶粒子の内部まで深く再酸化され、絶縁層の幅
が厚くなり、得られたコンデンサの静電容量の低
下又は誘電損失の上昇を招くといつた問題が生じ
ていた。また熱処理が十分行われないと、前記拡
散物質が均一に拡散せず、上述した拡散物質を用
いない方法と同様に、得られたコンデンサの絶縁
抵抗値又は絶縁破壊電圧値が低いという欠点があ
つた。これは特に、半導体磁器が厚肉形状である
場合又は複雑な形状を有している場合に顕著にみ
られた。
本発明は斯かる事情に鑑みてなされたものであ
り、粒界絶縁体化工程において、大気圧未満に減
圧した容器内で半導体磁器に拡散物質を熱拡散せ
しめた後、前記容器に酸素を含むガスを導入して
大気圧以上とすると共に冷却し結晶粒界の再酸化
を行うことにより、高静電容量値、高絶縁抵抗値
及び高絶縁破壊電圧値を有する小型大容量の粒界
絶縁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。
〔課題を解決するための手段〕
本発明に係る粒界絶縁型半導体磁器コンデンサ
の製造方法は、半導体磁器の表面に拡散物質を付
着させて該拡散物質を粒界層に熱拡散し、該粒界
層を再酸化する粒界絶縁型半導体磁器コンデンサ
の製造方法において、前記半導体磁器及び前記拡
散物質を大気圧未満に減圧した容器内に配し、加
熱する熱拡散過程と、前記容器内に酸素を含むガ
スを導入して大気圧以上の圧力とすると共に前記
容器内を冷却する再酸化過程とを含むことを特徴
とする。
〔作用〕
本発明の粒界絶縁型の半導体磁器コンデンサの
製造方法にあつては、半導体磁器及び拡散物質を
大気圧未満に減圧した容器内に配して加熱するこ
とより、前記拡散物質の蒸発が促進され、該拡散
物質の半導体磁器への付着量が増加する。そして
前記拡散物質の結晶粒界への拡散が促進され、こ
のときの半導体磁器の再酸化が防止される。
また、拡散物質の結晶粒界への拡散を行つた
後、前記容器に酸素を含むガスを導入すると共に
前記容器を冷却することより、前記拡散物質の結
晶粒界への過度の拡散が防止され、半導体磁器が
十分再酸化される。
〔実施例〕
以下、本発明の半導体磁器コンデンサの製造方
法をその実施例に基づき具体的に説明する。
まずチタン酸ストロンチウム系の半導体磁器の
製造方法について述べる。
炭酸ストロンチウム、酸化チタン及び五酸化ニ
オブを夫々モル比率にして100対100対0.2の割合
で秤量し、樹脂製ボールミルと樹脂製ボールとを
用いて24時間湿式混合を行つた後、蒸発乾燥して
1200℃で仮焼する。
得られた粉末にポリビニルアルコールを2.5%
添加して、再び樹脂製ボールミルと樹脂製ボール
とを用いて24時間湿式混合粉砕し、蒸発乾燥す
る。そして60メツシユの篩を通し、造粒して
2ton/cm2の圧力で10mmφ×1.5mmの円板状に成形
する。この成形体を1000℃で2時間加熱して有機
成分を除去し、H2,N2の混合気流(H2:N2=
1:9)中で1500℃で6時間焼成して、円板状チ
タン酸ストロンチウム系の半導体磁器を得る。
このようにして得た半導体磁器の性状は平均結
晶粒子径が50μmであり、ほぼ均一な粒成長を示
していた。また、この半導体磁器の比抵抗値は、
40mΩcmであり十分に低い値を示していた。
次に上述して得られた半導体磁器の結晶粒界を
絶縁体化する方法について述べる。
実施例 1
第1図は本発明方法を実施する装置の構成を示
す模式的断面図であり、図中1はその内部にて半
導体磁器を前記絶縁体化するための反応容器であ
る。この反応容器1は、例えばアルミナ製の円筒
形密封容器であり、軸長方向を水平方向として設
置されている。反応容器1外側にはヒータ6が周
設されており、前記反応容器1内の下側には断面
矩形のアルミナ製の支持台2が具設されている。
そして該支持台2上には、後述する拡散物質を付
着させた半導体磁器4aを載置すべく断面がコの
字型のアルミナ製の試料保持容器3が設けられて
いる。
一方、反応容器1の一側壁には温度センサ7の
挿入口7aが設けられており、前記温度センサ7
を反応容器1に挿入することよつて、前記試料保
持容器3に載置されている半導体磁器4a近傍の
温度が測定される。また反応容器1の他側壁の一
端側には、排気バルブ8aを介して図示しない真
空ポンプに接続する排気管8が固設され、他端側
には、ガス導入バルブ9aを介して図示しないコ
ンプレツサ又は酸素ボンベに接続するガス導入管
9が固設されている。
このような構成をなす装置を用い、以下の操作
にて半導体磁器の結晶粒界を絶縁体化させる。
まず、上述で得られた半導体磁器の表面の片面
又は両面に、原子価補償のための結晶粒界拡散物
質即ち、酸化ビスマス(BiO3)、酸化銅
(Cu2O)、酸化鉛(PbO)をモル比にして4:
2:4の割合で混合した拡散物質ペーストを素体
1g当たり10mgの割合で塗布する。これを空気中、
350℃で2時間加熱して有機成分を燃焼除去し、
反応容器1内の試料保持容器3上に載置する。
次いで、排気バルブ8aを開放にして真空ポン
プにより反応容器1内を0.05MPaに減圧した後、
ヒータ6を用いて反応容器1内を1150℃に加熱
し、1時間この状態を保持する。その後、ガス導
入バルブ9aを開放にしてコンプレツサ又は酸素
ボンベから大気又は酸素ガスを導入して反応容器
1内を大気圧に戻し、自然放冷により室温まで冷
却すると粒界絶縁型半導体磁器コンデンサの素体
が得られる。そしてさらに、その両面にIn−Ga
合金を塗布して電極を形成すると、高静電容量
値、高絶縁抵抗値及び高絶縁破壊電圧値を有する
粒界絶縁型半導体磁器コンデンサが得られる。
なお、本実施例において拡散物質を付着させた
半導体磁器を大気圧未満の減圧下で熱拡散させた
のは、大気中又は大気圧以上の加圧下で前記半導
体磁器を熱拡散させると、前記拡散物質の結晶粒
界への拡散と同時に半導体磁器の再酸化反応が進
行し、その結果絶縁体層の幅が厚くなり、高い静
電容量値が得られないためである。
また前記熱拡散処理後、減圧状態の容器に大気
又は酸素ガスを導入し、大気圧以上とすると共に
前記容器を冷却するのは、大気又は酸素ガスを導
入した後更に加熱を続けると、半導体磁器の再酸
化と同時に拡散物質の拡散が必要以上に進行し、
高い静電容量が得られないためである。
また、前記容器内に大気圧以上の大気又は酸素
ガスを導入するのは、大気圧未満であると半導体
磁器が十分に再酸化されず得られた半導体磁器コ
ンデンサの絶縁抵抗値及び絶縁破壊電圧値が低く
なるためである。
実施例 2
次に本発明方法の他の実施例について説明す
る。
まず、上述と同様に拡散物質ペーストを塗布し
た後、有機成分を除去して得られた半導体磁器4
aを第1図の反応容器1内の試料保持容器3上に
載置する。次いで、真空ポンプを用いて反応容器
1内を0.07MPaに減圧し、1150℃で1時間加熱し
た後減圧した状態で加熱を停止し冷却を開始す
る。そして、反応容器1内の温度が1000℃になつ
たところでガス導入管9から大気を導入し、反応
容器1内を大気圧に戻すと共に冷却を継続して行
い、反応容器1内を室温にすると粒界絶縁型半導
体磁器コンデンサ素体が得られる。
このように熱拡散処理後、反応容器1内への大
気又は酸素ガスの導入温度を制御することによつ
て、つまり減圧した状態で所定の温度に冷却した
後大気又は酸素ガスを導入し、反応容器1内を大
気圧に戻すと共に冷却を継続して行うことによつ
て、半導体磁器4aの再酸化の進行を制御でき
る。
さらに、前記粒界絶縁型半導体磁器コンデンサ
素体の両面にIn−Ga合金を塗布して電極を形成
すると所望の静電容量値、絶縁抵抗値及び絶縁破
壊電圧値を有する粒界絶縁型半導体磁器コンデン
サが得られる。
実施例 3
次に本発明方法の第3の実施例について説明す
る。
まず、上述と同様に拡散物質ペーストを塗布し
た後、有機成分を除去して得られた半導体磁器4
aを第1図の反応容器1内の試料保持容器3上に
載置する。次いで、真空ポンプを用いて反応容器
1内を0.03MPaに減圧し、1150℃で1時間加熱し
た後減圧した状態で冷却を開始する。反応容器1
の温度が900℃になつたところで酸素ガスを導入
し、反応容器1内のガス圧力を0.2MPaとすると
共に反応容器1内の温度を900℃で30分間保持す
る。その後、自然放冷により反応容器1内を室温
まで冷却すると、粒界絶縁型半導体磁器コンデン
サ素体が得られる。
このように、熱拡散処理後、反応容器1内への
大気又は酸素ガスの導入時期を制御することによ
つて、つまり減圧した状態で所定温度に冷却した
反応容器1に、所定圧力まで大気又は酸素ガスを
導入し、前記温度で所定時間保持した後再び冷却
を行うことによつて、半導体磁器4aの再酸化の
進行を制御できる。
さらに、前記粒界絶縁型半導体磁器コンデンサ
素体の両面にIn−Ga合金を塗布して電極を形成
すると所望の静電容量値、絶縁抵抗値及び絶縁破
壊電圧値を有する粒界絶縁型半導体磁器コンデン
サが得られる。
実施例 4
さらに、本発明方法の第4の実施例について説
明する。
第2図は本発明方法を実施する他の装置の構成
を示す模式的断面図であり、図中1はその内部に
て半導体磁器を前記絶縁体化するための反応容器
である。この反応容器1は、例えばアルミナ製の
円筒形密封容器であり、軸長方向を水平方向とし
て設置されている。反応容器1外側にはヒータ6
が周設されており、前記反応容器1内の下側には
所定間隔にて断面矩形のアルミナ製の支持台2,
2が夫々具設されている。該支持台2,2上の一
方には拡散物質5を載置すべく断面がL字型のア
ルミナ製の試料保持容器3が設けられており、他
方には拡散物質5を付着させていない半導体磁器
4bを載置すべくやはり断面がL字型のアルミナ
製の試料保持容器3が設けられている。
一方、反応容器1の一側壁には温度センサ7,
7の挿入口7a,7aが夫々設けられており、前
記温度センサ7,7を反応容器1に挿入すること
よつて、前記試料保持容器3に載置されている半
導体磁器4b近傍の温度及び拡散物質5近傍の温
度が夫々測定される。また反応容器1の他側壁の
一端側には、排気バルブ8aを介して図示しない
真空ポンプに接続する排気管8が固設され、他端
側には、ガス導入バルブ9aを介して図示しない
コンプレツサ又は酸素ボンベに接続するガス導入
管9が固設されている。
このような構成をなす装置を用い、以下の操作
にて半導体磁器の結晶粒界を絶縁体化させる。
まず、拡散物質を付着させていない半導体磁器
4bを前記試料保持容器3に載置し、原子価補償
のための拡散物質即ち、酸化ビスマス(BiO3)、
酸化銅(Cu2O)、酸化鉛(PbO)をモル比にして
4:2:4の割合で混合した拡散物質を前記試料
保持容器3に載置する。そして、排気バルブ8a
を開放にして真空ポンプにより反応容器1内を
0.01MPaに減圧した後、ヒータ6を用いて拡散物
質5近傍の温度を1200℃に、半導体磁器4近傍の
温度を1150℃に加熱して1時間保持する。その
後、ガス導入バルブ9aを開放にしてコンプレツ
サにより大気を導入して反応容器1を大気圧に戻
し自然放冷により室温まで冷却すると、粒界絶縁
型半導体磁器コンデンサ素体が得られる。
このように、半導体磁器4bの加熱温度が拡散
物質5の加熱温度以下になるよう制御することに
よつて、拡散物質5の半導体磁器4bへの付着量
が増加し、拡散物質5の結晶粒界への拡散が十分
なされる。従つて、厚肉の又は複雑形状の半導体
磁器4bであつても、均一かつ薄い絶縁層を形成
できる。
さらに、前記粒界絶縁型半導体磁器コンデンサ
素体の両面にIn−Ga合金を塗布して電極を形成
すると高静電容量値、高絶縁抵抗値及び絶縁破壊
電圧値を有する粒界絶縁型半導体磁器コンデンサ
が得られる。
なお、半導体磁器4bの加熱温度が拡散物質5
の加熱温度以下になるよう制御するのは、半導体
磁器4bの加熱温度が拡散物質5の加熱温度以上
であると、半導体磁器4bへ拡散物質5が十分供
給されず、絶縁抵抗値又は絶縁破壊電圧値が低く
なるためである。
以上の如く得られた半導体磁器コンデンサの電
気特性即ち、見かけの誘電率εapp、誘電損失
tanδ、絶縁抵抗率ρ及び絶縁破壊電圧値を調べた
結果を第1表に示す。
前記見かけの誘電率εappは、1Vrms、1KHzの
交流電圧下で測定した静電容量C、素体厚みt、
電極面積S及び真空の誘電率ε0を式(1)に代入して
求めたものである。
εapp=Ct/ε0・S… (1)
前記誘電損失tanδ(%)は、1Vrms、1KHzの交
流電圧下で測定した結果であり、前記絶縁抵抗率
ρ(Ωcm)は、50Vの直流電圧を1分間印加した
後の抵抗値R、素体厚みt及び電極面積Sを式(2)
に代入して求めたものである。
ρ=R・S/t …(2)
また前記絶縁破壊電圧値(VDC/mm)は、直流
電圧を印加し測定した値を素子1mm厚当たりに換
算して求めたものである。
さらに、第1表では比較例として、本発明方法
の条件の範囲外で製造した粒界絶縁型半導体磁器
コンデンサの電気特性を示してある。即ち比較例
1は、拡散物質ペーストを塗布していない半導体
磁器を前記反応容器1に載置して0.05MPaに減圧
し、1150℃で1時間加熱した後大気を導入し自然
冷却して得た場合の半導体磁器コンデンサが、ま
た比較例2は拡散物質ペーストを塗布し有機成分
を除去した半導体磁器を、前記反応容器1内で減
圧せずに大気中で1150℃、1時間加熱し自然冷却
して得た場合の半導体磁器コンデンサが示してあ
る。
[Industrial Application Field] The present invention relates to a grain boundary insulated semiconductor ceramic capacitor in which a diffusion substance is attached to the surface of a semiconductor ceramic, the diffusion substance is thermally diffused into the grain boundary layer, and the grain boundary layer is reoxidized. Regarding the manufacturing method. [Prior art] Grain boundary insulated semiconductor ceramic capacitors are made by increasing the resistance of the crystal grain boundaries of semiconducting ceramic and using the crystal grain boundaries as a dielectric material. It depends on the state of the insulator layer, which is about several μm thick. Semiconductor porcelain is generally made of a composition whose main component is strontium titanate or barium titanate, and which contains one or more elements called valence control elements such as niobium, tantalum, antimony, or rare earth elements. It is obtained by molding and firing in a neutral or reducing atmosphere. Conventionally, methods for converting the grain boundaries of semiconductor ceramics obtained in this way into insulators include a method of re-oxidizing the grain boundary layer by heat treatment in the atmosphere, or a method of re-oxidizing the grain boundary layer, which is easily diffused into the grain boundaries. Grain boundary diffusion substances to be compensated, for example, one or more of elements such as copper, bismuth, lead, or manganese, are attached to the surface of the semiconductor porcelain by printing or other means, and then heat treatment is performed in the atmosphere,
A common method is to diffuse the grain boundary diffusion substance into the grain boundary layer and simultaneously re-oxidize the grain boundary layer. [Problems to be Solved by the Invention] However, in the grain boundary insulating step described above, in the method of reoxidizing the grain boundary layer by heat treatment in the atmosphere without using a diffusing substance, the insulation resistance value or It had the disadvantage of a low dielectric breakdown voltage value. On the other hand, in the thermal diffusion method using a diffusion substance such as copper, bismuth, lead, or manganese, the diffusion substance is thermally diffused into the grain boundary layer and the grain boundary layer is reoxidized at the same time, as described above. A long heat treatment was required to sufficiently diffuse the substance into the grain boundary layer.
As a result, the crystal grains near the surface of the semiconductor ceramic are reoxidized deeply, and the width of the insulating layer becomes thicker, leading to a decrease in capacitance or an increase in dielectric loss of the resulting capacitor. A problem had arisen. Furthermore, if the heat treatment is not performed sufficiently, the diffusion substance will not be uniformly diffused, resulting in the drawback that the resulting capacitor will have a low insulation resistance value or dielectric breakdown voltage value, similar to the above-mentioned method that does not use a diffusion substance. Ta. This was particularly noticeable when the semiconductor porcelain had a thick shape or a complicated shape. The present invention has been made in view of such circumstances, and in the step of forming a grain boundary insulator, after thermally diffusing a diffusion substance into semiconductor ceramics in a container whose pressure is reduced to less than atmospheric pressure, the container contains oxygen. By introducing gas to raise the pressure to above atmospheric pressure and cooling to reoxidize the grain boundaries, a small, large-capacity, grain-boundary insulated type with high capacitance, high insulation resistance, and high dielectric breakdown voltage is created. The object of the present invention is to provide a method for manufacturing a semiconductor ceramic capacitor. [Means for Solving the Problems] A method for manufacturing a grain boundary insulated semiconductor ceramic capacitor according to the present invention involves attaching a diffusing substance to the surface of semiconductor ceramic, thermally diffusing the diffusing substance into the grain boundary layer, and dispersing the grain. A method for manufacturing a grain boundary insulated semiconductor ceramic capacitor in which the boundary layer is reoxidized includes a thermal diffusion process in which the semiconductor ceramic and the diffusion material are placed in a container whose pressure is reduced to below atmospheric pressure, and heated, and oxygen is added to the container. The method is characterized in that it includes a reoxidation process in which a gas containing gas is introduced to bring the pressure above atmospheric pressure and the inside of the container is cooled. [Function] In the method of manufacturing a grain boundary insulated semiconductor ceramic capacitor of the present invention, the semiconductor ceramic and the diffusion material are placed in a container whose pressure is reduced to below atmospheric pressure and heated, thereby causing the evaporation of the diffusion material. is promoted, and the amount of the diffusion substance adhering to the semiconductor ceramic increases. Diffusion of the diffusion substance to the grain boundaries is promoted, and re-oxidation of the semiconductor ceramic is prevented at this time. Furthermore, after the diffusion substance has diffused into the grain boundaries, by introducing a gas containing oxygen into the container and cooling the container, excessive diffusion of the diffusion substance into the grain boundaries can be prevented. , the semiconductor porcelain is fully reoxidized. [Example] Hereinafter, the method for manufacturing a semiconductor ceramic capacitor of the present invention will be specifically explained based on the example. First, a method for manufacturing strontium titanate-based semiconductor porcelain will be described. Strontium carbonate, titanium oxide, and niobium pentoxide were weighed in a molar ratio of 100:100:0.2, wet mixed for 24 hours using a resin ball mill and a resin ball, and then evaporated and dried.
Calculate at 1200℃. Add 2.5% polyvinyl alcohol to the resulting powder
The mixture is then wet mixed and ground again for 24 hours using a resin ball mill and resin balls, and then evaporated and dried. Then, it is passed through a 60 mesh sieve and granulated.
Form into a disc shape of 10mmφ x 1.5mm using a pressure of 2ton/ cm2 . This molded body was heated at 1000°C for 2 hours to remove organic components, and a mixed gas flow of H 2 and N 2 (H 2 :N 2 =
1:9) for 6 hours at 1500°C to obtain a disk-shaped strontium titanate semiconductor ceramic. The semiconductor porcelain thus obtained had an average crystal grain size of 50 μm and exhibited almost uniform grain growth. In addition, the specific resistance value of this semiconductor porcelain is
It was 40 mΩcm, which was a sufficiently low value. Next, a method for converting the crystal grain boundaries of the semiconductor ceramic obtained above into an insulator will be described. Example 1 FIG. 1 is a schematic sectional view showing the configuration of an apparatus for carrying out the method of the present invention, and numeral 1 in the figure is a reaction vessel for converting the semiconductor ceramic into the insulator. The reaction vessel 1 is, for example, a cylindrical sealed vessel made of alumina, and is installed with its axial direction in the horizontal direction. A heater 6 is provided around the outside of the reaction container 1, and a support base 2 made of alumina and having a rectangular cross section is provided on the lower side inside the reaction container 1.
A sample holding container 3 made of alumina and having a U-shaped cross section is provided on the support base 2 in order to place a semiconductor ceramic 4a to which a diffusion substance, which will be described later, is attached. On the other hand, an insertion port 7a for a temperature sensor 7 is provided on one side wall of the reaction vessel 1.
By inserting the sample into the reaction container 1, the temperature near the semiconductor ceramic 4a placed in the sample holding container 3 is measured. Further, an exhaust pipe 8 connected to a vacuum pump (not shown) via an exhaust valve 8a is fixed at one end of the other side wall of the reaction vessel 1, and a compressor (not shown) is connected to the other end via a gas introduction valve 9a. Alternatively, a gas introduction pipe 9 connected to an oxygen cylinder is fixedly installed. Using a device having such a configuration, the grain boundaries of the semiconductor ceramic are made into an insulator by the following operations. First, on one or both surfaces of the semiconductor ceramic obtained above, grain boundary diffusion substances for valence compensation, such as bismuth oxide (BiO 3 ), copper oxide (Cu 2 O), and lead oxide (PbO), are applied. The molar ratio is 4:
Diffusion material paste mixed in a ratio of 2:4 is used as an element.
Apply at a rate of 10mg per gram. In the air,
Heat at 350℃ for 2 hours to burn off organic components,
Place it on the sample holding container 3 inside the reaction container 1. Next, after opening the exhaust valve 8a and reducing the pressure inside the reaction container 1 to 0.05 MPa using a vacuum pump,
The inside of the reaction vessel 1 is heated to 1150° C. using the heater 6, and this state is maintained for 1 hour. Thereafter, the gas introduction valve 9a is opened to introduce atmospheric air or oxygen gas from a compressor or an oxygen cylinder to return the inside of the reaction vessel 1 to atmospheric pressure, and when it is naturally cooled to room temperature, the grain boundary insulated semiconductor ceramic capacitor is formed. You get a body. Furthermore, In-Ga on both sides.
When an electrode is formed by applying the alloy, a grain boundary insulated semiconductor ceramic capacitor having a high capacitance value, high insulation resistance value, and high dielectric breakdown voltage value is obtained. Note that in this example, the semiconductor porcelain to which the diffusive substance was attached was thermally diffused under reduced pressure below atmospheric pressure. This is because the reoxidation reaction of the semiconductor ceramic progresses simultaneously with the diffusion of the substance to the grain boundaries, and as a result, the width of the insulator layer becomes thicker, making it impossible to obtain a high capacitance value. After the thermal diffusion treatment, air or oxygen gas is introduced into the container in a reduced pressure state to raise the pressure to above atmospheric pressure and the container is cooled. At the same time as the reoxidation of
This is because high capacitance cannot be obtained. In addition, it is important to introduce the atmosphere or oxygen gas at a pressure higher than atmospheric pressure into the container because if the pressure is lower than atmospheric pressure, the semiconductor ceramic will not be sufficiently reoxidized, resulting in the insulation resistance value and dielectric breakdown voltage value of the semiconductor ceramic capacitor. This is because the Example 2 Next, another example of the method of the present invention will be described. First, the semiconductor porcelain 4 obtained by applying the diffusion substance paste and removing the organic components in the same manner as described above.
A is placed on the sample holding container 3 in the reaction container 1 shown in FIG. Next, the pressure inside the reaction vessel 1 was reduced to 0.07 MPa using a vacuum pump, and after heating at 1150° C. for 1 hour, heating was stopped and cooling was started while the pressure was reduced. Then, when the temperature inside the reaction vessel 1 reaches 1000°C, air is introduced from the gas introduction pipe 9, and the inside of the reaction vessel 1 is returned to atmospheric pressure, and cooling is continued to bring the inside of the reaction vessel 1 to room temperature. A grain boundary insulated semiconductor ceramic capacitor body is obtained. After the thermal diffusion treatment, by controlling the temperature at which the atmosphere or oxygen gas is introduced into the reaction vessel 1, that is, after cooling it to a predetermined temperature under reduced pressure, the atmosphere or oxygen gas is introduced and the reaction is carried out. By returning the inside of the container 1 to atmospheric pressure and continuing cooling, the progress of reoxidation of the semiconductor ceramic 4a can be controlled. Further, when an In-Ga alloy is applied to both sides of the grain boundary insulated semiconductor ceramic capacitor body to form electrodes, a grain boundary insulated semiconductor ceramic capacitor having desired capacitance, insulation resistance, and dielectric breakdown voltage values can be obtained. A capacitor is obtained. Example 3 Next, a third example of the method of the present invention will be described. First, the semiconductor porcelain 4 obtained by applying the diffusion substance paste and removing the organic components in the same manner as described above.
A is placed on the sample holding container 3 in the reaction container 1 shown in FIG. Next, the pressure inside the reaction vessel 1 was reduced to 0.03 MPa using a vacuum pump, and after heating at 1150° C. for 1 hour, cooling was started under reduced pressure. Reaction vessel 1
When the temperature reaches 900°C, oxygen gas is introduced, the gas pressure inside the reaction vessel 1 is set to 0.2 MPa, and the temperature inside the reaction vessel 1 is maintained at 900°C for 30 minutes. Thereafter, the inside of the reaction vessel 1 is cooled down to room temperature by natural cooling to obtain a grain boundary insulated semiconductor ceramic capacitor body. In this way, by controlling the timing of introducing the atmosphere or oxygen gas into the reaction vessel 1 after the thermal diffusion treatment, in other words, the atmosphere or oxygen gas is introduced into the reaction vessel 1 which has been cooled to a predetermined temperature in a reduced pressure state to a predetermined pressure. The progress of reoxidation of the semiconductor ceramic 4a can be controlled by introducing oxygen gas, maintaining the temperature for a predetermined time, and then cooling it again. Further, when an In-Ga alloy is applied to both sides of the grain boundary insulated semiconductor ceramic capacitor body to form electrodes, a grain boundary insulated semiconductor ceramic capacitor having desired capacitance, insulation resistance, and dielectric breakdown voltage values can be obtained. A capacitor is obtained. Example 4 Furthermore, a fourth example of the method of the present invention will be described. FIG. 2 is a schematic cross-sectional view showing the structure of another apparatus for carrying out the method of the present invention, in which reference numeral 1 denotes a reaction vessel for converting the semiconductor ceramic into the insulator. The reaction vessel 1 is, for example, a cylindrical sealed vessel made of alumina, and is installed with its axial direction in the horizontal direction. A heater 6 is installed outside the reaction vessel 1.
are provided around the periphery, and on the lower side of the reaction vessel 1, support stands 2 made of alumina and having a rectangular cross section are arranged at predetermined intervals.
2 are provided respectively. A sample holding container 3 made of alumina and having an L-shaped cross section is provided on one side of the support stands 2, 2 to place the diffusion substance 5, and the other side is provided with a semiconductor sample holding container 3 on which the diffusion substance 5 is not attached. A sample holding container 3 made of alumina and also having an L-shaped cross section is provided in order to place the porcelain 4b thereon. On the other hand, a temperature sensor 7 is mounted on one side wall of the reaction vessel 1.
By inserting the temperature sensors 7, 7 into the reaction container 1, the temperature and diffusion near the semiconductor ceramic 4b placed in the sample holding container 3 can be measured. The temperature near each substance 5 is measured. Further, an exhaust pipe 8 connected to a vacuum pump (not shown) via an exhaust valve 8a is fixed at one end of the other side wall of the reaction vessel 1, and a compressor (not shown) is connected to the other end via a gas introduction valve 9a. Alternatively, a gas introduction pipe 9 connected to an oxygen cylinder is fixedly installed. Using a device having such a configuration, the grain boundaries of the semiconductor ceramic are made into an insulator by the following operations. First, the semiconductor ceramic 4b to which no diffusion substance is attached is placed on the sample holding container 3, and a diffusion substance for valence compensation, that is, bismuth oxide (BiO 3 ), is placed on the sample holding container 3.
A diffusion substance made by mixing copper oxide (Cu 2 O) and lead oxide (PbO) in a molar ratio of 4:2:4 is placed in the sample holding container 3 . And exhaust valve 8a
is opened and the inside of reaction vessel 1 is pumped using a vacuum pump.
After reducing the pressure to 0.01 MPa, the temperature near the diffusion material 5 is heated to 1200° C. and the temperature near the semiconductor ceramic 4 is heated to 1150° C. using the heater 6, and maintained for one hour. Thereafter, the gas introduction valve 9a is opened to introduce atmospheric air using a compressor, and the reaction vessel 1 is returned to atmospheric pressure and cooled to room temperature by natural cooling, thereby obtaining a grain boundary insulated semiconductor ceramic capacitor body. In this way, by controlling the heating temperature of the semiconductor ceramic 4b to be equal to or lower than the heating temperature of the diffusion material 5, the amount of the diffusion material 5 attached to the semiconductor ceramic 4b is increased, and the crystal grain boundaries of the diffusion material 5 are sufficient diffusion. Therefore, even if the semiconductor ceramic 4b is thick or has a complicated shape, a uniform and thin insulating layer can be formed. Furthermore, when an In-Ga alloy is applied to both sides of the grain boundary insulated semiconductor ceramic capacitor body to form electrodes, a grain boundary insulated semiconductor porcelain having high capacitance, high insulation resistance, and dielectric breakdown voltage can be produced. A capacitor is obtained. Note that the heating temperature of the semiconductor porcelain 4b is higher than that of the diffusion substance 5.
The reason why the heating temperature is controlled to be below the heating temperature is that if the heating temperature of the semiconductor porcelain 4b is higher than the heating temperature of the diffusion material 5, the diffusion material 5 will not be sufficiently supplied to the semiconductor porcelain 4b, and the insulation resistance value or dielectric breakdown voltage will decrease. This is because the value becomes lower. The electrical properties of the semiconductor ceramic capacitor obtained as described above, namely, the apparent permittivity ε app and the dielectric loss
Table 1 shows the results of examining tan δ, insulation resistivity ρ, and dielectric breakdown voltage values. The apparent permittivity ε app is the capacitance C measured under an AC voltage of 1 Vrms and 1 KHz, the thickness t of the element body,
It was obtained by substituting the electrode area S and the vacuum permittivity ε 0 into equation (1). ε app = Ct/ε 0・S... (1) The above dielectric loss tan δ (%) is the result of measurement under an AC voltage of 1 Vrms, 1 KHz, and the above insulation resistivity ρ (Ωcm) is the result of measurement under a DC voltage of 50 V. After applying for 1 minute, the resistance value R, the element thickness t, and the electrode area S are expressed by formula (2).
It was obtained by substituting . ρ=R·S/t (2) The dielectric breakdown voltage value (V DC /mm) is calculated by converting the value measured by applying a DC voltage per 1 mm thickness of the element. Further, Table 1 shows, as a comparative example, the electrical characteristics of a grain boundary insulated semiconductor ceramic capacitor manufactured outside the conditions of the method of the present invention. That is, Comparative Example 1 was obtained by placing semiconductor porcelain to which no diffusive substance paste was applied, placing it in the reaction vessel 1, reducing the pressure to 0.05 MPa, heating it at 1150°C for 1 hour, and then introducing air to naturally cool it. In Comparative Example 2, a semiconductor ceramic capacitor coated with a diffusion substance paste and from which organic components were removed was heated in the atmosphere at 1150°C for 1 hour without reducing the pressure in the reaction vessel 1, and then cooled naturally. A semiconductor porcelain capacitor obtained by
以上詳述した如く、本発明の粒界絶縁型半導体
磁器コンデンサの製造方法では、半導体磁器の粒
界層の絶縁化工程において、前記半導体磁器及び
前記拡散物質を大気圧未満に減圧した容器内に配
し、加熱して前記拡散物質を結晶粒界に熱拡散す
る過程を有するので、前記拡散物質の半導体磁器
への付着量が増加し拡散が十分がなされる。この
ことにより、静電容量値の低下が防止できまた、
厚肉又は複雑形状の半導体磁器であつても、均一
かつ薄い絶縁体層が形成できる。
そして前記過程後、前記容器内に酸素を含むガ
スを導入して大気圧以上の圧力とすると共に、前
記容器内を冷却して前記粒界層の再酸化を行うの
で、半導体磁器表面近傍の結晶粒子の過度の再酸
化が防止される。従つて、高静電容量値、高絶縁
抵抗値及び高絶縁破壊電圧値を有する小型大容量
の粒界絶縁型半導体磁器コンデンサが得られる等
本発明は優れた効果を奏する。
As detailed above, in the method for manufacturing a grain boundary insulated semiconductor ceramic capacitor of the present invention, in the step of insulating the grain boundary layer of the semiconductor ceramic, the semiconductor ceramic and the diffusion material are placed in a container whose pressure is reduced to below atmospheric pressure. Since the method includes a process of thermally diffusing the diffusion substance to the grain boundaries by disposing the semiconductor ceramic and heating it, the amount of the diffusion substance attached to the semiconductor ceramic increases and sufficient diffusion is achieved. This prevents the capacitance value from decreasing, and
A uniform and thin insulating layer can be formed even on thick or complex-shaped semiconductor porcelain. After the above process, a gas containing oxygen is introduced into the container to make the pressure higher than atmospheric pressure, and the inside of the container is cooled to reoxidize the grain boundary layer, so that the crystals near the surface of the semiconductor ceramic are cooled. Excessive re-oxidation of the particles is prevented. Therefore, the present invention exhibits excellent effects such as obtaining a small, large-capacity, grain-boundary insulated semiconductor ceramic capacitor having a high capacitance value, high insulation resistance value, and high dielectric breakdown voltage value.
第1図は本発明方法を実施する装置の構成を示
す模式的断面図、第2図は本発明方法を実施する
他の装置の構成を示す模式的断面図である。
1…反応容器、2…支持台、3…試料保持容
器、4a…半導体磁器、4b…半導体磁器、5…
拡散物質、6…ヒータ、7…温度センサ。
FIG. 1 is a schematic cross-sectional view showing the configuration of an apparatus for implementing the method of the present invention, and FIG. 2 is a schematic cross-sectional view showing the configuration of another apparatus for implementing the method of the present invention. DESCRIPTION OF SYMBOLS 1... Reaction container, 2... Support stand, 3... Sample holding container, 4a... Semiconductor porcelain, 4b... Semiconductor porcelain, 5...
Diffusion substance, 6... Heater, 7... Temperature sensor.
Claims (1)
拡散物質を粒界層に熱拡散し、該粒界層を再酸化
する粒界絶縁型半導体磁器コンデンサの製造方法
において、 前記半導体磁器及び前記拡散物質を大気圧未満
に減圧した容器内に配し、加熱する熱拡散過程
と、 前記容器内に酸素を含むガスを導入して大気圧
以上の圧力とすると共に前記容器内を冷却する再
酸化過程と を含むことを特徴とする粒界絶縁型半導体磁器コ
ンデンサの製造方法。[Scope of Claims] 1. A method for manufacturing a grain boundary insulated semiconductor ceramic capacitor in which a diffusion substance is attached to the surface of semiconductor ceramic, the diffusion substance is thermally diffused into the grain boundary layer, and the grain boundary layer is reoxidized, A thermal diffusion process in which the semiconductor porcelain and the diffusion material are placed in a container whose pressure is reduced to below atmospheric pressure and heated; A method for manufacturing a grain boundary insulated semiconductor ceramic capacitor, the method comprising: a reoxidation process of cooling the capacitor.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12764489A JPH02305418A (en) | 1989-05-19 | 1989-05-19 | Manufacture of grain boundary insulated type semiconductor porcelain capacitor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12764489A JPH02305418A (en) | 1989-05-19 | 1989-05-19 | Manufacture of grain boundary insulated type semiconductor porcelain capacitor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02305418A JPH02305418A (en) | 1990-12-19 |
| JPH0524647B2 true JPH0524647B2 (en) | 1993-04-08 |
Family
ID=14965191
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12764489A Granted JPH02305418A (en) | 1989-05-19 | 1989-05-19 | Manufacture of grain boundary insulated type semiconductor porcelain capacitor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH02305418A (en) |
-
1989
- 1989-05-19 JP JP12764489A patent/JPH02305418A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPH02305418A (en) | 1990-12-19 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| JPH0524646B2 (en) | ||
| CN110304916B (en) | Anti-reduction BaTiO3Base medium ceramic and preparation method thereof | |
| JPH0524647B2 (en) | ||
| JP2971689B2 (en) | Grain boundary type semiconductor porcelain capacitor | |
| JP3124896B2 (en) | Manufacturing method of semiconductor porcelain | |
| JP2970405B2 (en) | Grain boundary insulating semiconductor porcelain composition and method for producing the same | |
| JPS6128209B2 (en) | ||
| JPH0521266A (en) | Method of manufacturing grain boundary insulated semiconductor porcelain matter | |
| JP2665643B2 (en) | Manufacturing method of grain boundary layer type ceramics | |
| JP2506286B2 (en) | Method for manufacturing grain boundary insulated semiconductor porcelain | |
| JP2734888B2 (en) | Method for producing semiconductor porcelain composition | |
| JP2687138B2 (en) | Grain boundary insulation method for strontium titanate-based semiconductor ceramics | |
| JPS6242363B2 (en) | ||
| CN119683991A (en) | Pond dielectric zinc oxide ceramic and preparation method and application thereof | |
| JPS63285920A (en) | Manufacture of grain boundary insulation type semiconductor ceramic capacitor | |
| JP2838249B2 (en) | Manufacturing method of grain boundary insulated semiconductor porcelain | |
| JPS6128208B2 (en) | ||
| JPH0734415B2 (en) | Grain boundary insulation type semiconductor porcelain composition | |
| JPH07120597B2 (en) | Method for forming grain boundary layer of semiconductor porcelain | |
| JPH02194510A (en) | Manufacturing method of semiconductor ceramic capacitor | |
| JPS6242365B2 (en) | ||
| JP2936876B2 (en) | Semiconductor porcelain composition and method for producing the same | |
| JPH07267729A (en) | Production of grain boundary insulated semiconductor porcelain | |
| JPS6032344B2 (en) | Grain boundary insulated semiconductor porcelain capacitor material | |
| JPS6217368B2 (en) |