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JPS6031794B2 - Barium titanate semiconductor porcelain - Google Patents
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JPS6031794B2 - Barium titanate semiconductor porcelain - Google Patents

Barium titanate semiconductor porcelain

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Publication number
JPS6031794B2
JPS6031794B2 JP56212205A JP21220581A JPS6031794B2 JP S6031794 B2 JPS6031794 B2 JP S6031794B2 JP 56212205 A JP56212205 A JP 56212205A JP 21220581 A JP21220581 A JP 21220581A JP S6031794 B2 JPS6031794 B2 JP S6031794B2
Authority
JP
Japan
Prior art keywords
barium titanate
semiconductor
yttrium
present
amount
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
JP56212205A
Other languages
Japanese (ja)
Other versions
JPS58115075A (en
Inventor
修己 上垣外
晴夫 土井
辰視 日置
美治 広瀬
修之 山本
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.)
Toyota Central R&D Labs Inc
Original Assignee
Toyota Central R&D Labs Inc
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 Toyota Central R&D Labs Inc filed Critical Toyota Central R&D Labs Inc
Priority to JP56212205A priority Critical patent/JPS6031794B2/en
Priority to US06/373,817 priority patent/US4384989A/en
Priority to GB8212709A priority patent/GB2097778B/en
Priority to CA000402293A priority patent/CA1189770A/en
Publication of JPS58115075A publication Critical patent/JPS58115075A/en
Publication of JPS6031794B2 publication Critical patent/JPS6031794B2/en
Expired legal-status Critical Current

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  • Thermistors And Varistors (AREA)

Description

【発明の詳細な説明】 本発明は、正の抵抗温度特性を有するチタン酸/ゞIJ
ウム系半導体磁器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention provides titanic acid/IJ having positive resistance-temperature characteristics.
The present invention relates to aluminum-based semiconductor porcelain.

従来より、チタン酸バリウムは1び00・伽以上と高い
比抵抗を持つ絶縁体として知られており、このチタン酸
バリウム系材料にイットリウムなどの希土類元素、アン
チモン(Sb)、ニオブ(Nb)、ビスマス(Bi)ま
たはタンタル(Ta)などの少なくとも1種類以上の酸
化物を徴量添加し焼成するが、又は環元性雰囲気中で焼
成し半導体化したチタン酸バリウムの凝結体の粒界だけ
を酸化することにより、常温に於ける比抵抗10〜1ぴ
○・伽程度の低い半導体磁器が得られている。そして、
この様にして得られたチタン酸バリウム系半導体磁器は
、その抵抗温度特性に於いてチタン酸バリウムのキュリ
「点温度に相当する点を境に低温度側で低抵抗、高温度
側で高抵抗と急激にその電気比抵抗が立ち上がり可逆的
に起こるという特徴を持っている。そして、この様な正
の抵抗温度(PTC特性という)を利用して、温度制御
、電流制御等の為の材料として広く目的に応じ用いられ
てきた。
Conventionally, barium titanate has been known as an insulator with a high resistivity of 1.00.degree. At least one kind of oxide, such as bismuth (Bi) or tantalum (Ta), is added and fired, or only the grain boundaries of the barium titanate aggregates, which are converted into a semiconductor by firing in a cyclic atmosphere, are removed. By oxidizing, semiconductor porcelain with a low resistivity of 10 to 1 p.p.m. at room temperature is obtained. and,
The barium titanate-based semiconductor porcelain obtained in this way has a resistance-temperature characteristic of barium titanate that has low resistance at low temperatures and high resistance at high temperatures, with a point corresponding to the point temperature of barium titanate. It has the characteristic that the electric resistivity rises suddenly and reversibly.Using this positive resistance temperature (called PTC characteristic), it can be used as a material for temperature control, current control, etc. It has been used for a wide range of purposes.

所が、この様な半導体磁器は、半導体化剤の添加量が僅
かに変化するだけでも比抵抗が急激に変化し実用に適せ
ないし、また再現性に乏しいといううらみがあった。ま
た、その製造に当っては、半導体化温度が高く、粒子成
長が大きく、粒子が粗大化し内部に気孔を取り込み易い
という欠点があった。更に、上記半導体磁器は、PTC
温度領域に於ける比抵抗変化中が大きく、かつ立上りが
急しゆんであることを必要とするスイッチング素子或い
は電流制御型発熱体等に使用する場合、添加剤としてM
n等が一般的に用いられている。
However, such semiconductor porcelain has the disadvantage that even a slight change in the amount of the semiconducting agent added causes a sudden change in resistivity, making it unsuitable for practical use and lacking in reproducibility. In addition, in its manufacture, there were drawbacks such as high semiconductor conversion temperature, large particle growth, coarse particles, and the tendency to incorporate pores into the particles. Furthermore, the semiconductor porcelain is PTC.
When used in switching elements or current-controlled heating elements that require a large change in resistivity in the temperature range and a rapid rise, M may be used as an additive.
n etc. are generally used.

しかし、これらの添加に当っては、極く徴量の変化が常
温に於ける比抵抗を大きく変化させる為に、千分の数パ
ーセントと言う様な微量の調整が必要であると言う問題
がある。本発明は、窒化チタニウム(TIN)、窒化ジ
ルコニウム(ZrN)または炭化珪素(SIC)の添加
が上記の欠点を取り除く効果のあることを偶然の機会に
見し、出したことに基づくものである。
However, when adding these, there is a problem in that very small changes in the characteristics can greatly change the resistivity at room temperature, so minute adjustments of a few thousandths of a percent are necessary. be. The present invention is based on the fortuitous discovery that the addition of titanium nitride (TIN), zirconium nitride (ZrN) or silicon carbide (SIC) is effective in eliminating the above-mentioned drawbacks.

即ち、本発明のチタン酸バリウム系半導体磁器は、チタ
ン酸バリウムとイットリウム、ランタン、セリウム、サ
マリウム、デイスプロシウム、アンチモンなどの3価の
金属元素およびニオブ、タンタル、ビスマスなどの5価
の金属元素などの徴量の半導体化剤とを含有するチタン
酸バリウム系半導体磁器に、窒化チタニウム(TIN)
、窒化ジルコニウム(ZてN)または炭化珪素(SIC
)のうち少なくとも1種類を0.1なし、し2.の重量
%含有させてなることを特徴とするものである。本発明
のチタン酸バリウム系半導体磁器は、半導体化剤として
のイットリウム等の成分割合が変化しても比抵抗が急激
に変化することがないので製造が容易である。
That is, the barium titanate-based semiconductor porcelain of the present invention contains barium titanate and trivalent metal elements such as yttrium, lanthanum, cerium, samarium, disprosium, and antimony, and pentavalent metal elements such as niobium, tantalum, and bismuth. Titanium nitride (TIN)
, zirconium nitride (ZTEN) or silicon carbide (SIC
) at least one of the following: 0.1 None, 2. It is characterized by containing % by weight of . The barium titanate-based semiconductor ceramic of the present invention is easy to manufacture because the resistivity does not change rapidly even if the proportion of components such as yttrium as a semiconductor agent changes.

又、本発明のチタン酸バリウム系半導体磁器は、従来の
ものに比較して低い温度で嘘結、半導体化するため結晶
粒子が小さく繊密である。更に、半導体化剤の広い添加
量の範囲でPTC領域に於ける抵抗変化が急しゆんかつ
変化中が大きいと言う特徴を有する。本発明のチタン酸
バリウム系半導体磁器を製造するには、従来のチタン酸
バリウム系半導体の原料粉末に、窒化チタニウム、窒化
ジルコニウム、炭化珪素粉末を混合し、大気中で焼成す
ることにより得られる。
Furthermore, the barium titanate semiconductor ceramic of the present invention undergoes solidification and becomes a semiconductor at a lower temperature than conventional ceramics, so its crystal grains are small and dense. Furthermore, the resistance change in the PTC region is rapid and large during the change within a wide range of addition amounts of the semiconductor agent. To manufacture the barium titanate-based semiconductor ceramic of the present invention, titanium nitride, zirconium nitride, and silicon carbide powder are mixed with conventional barium titanate-based semiconductor raw material powder, and the mixture is fired in the atmosphere.

チタン酸バリウムの代表的な原料としては炭酸バリウム
(BaC03)、酸化チタン(Ti02)が挙げられる
。チタン酸バリウムの原料は上記のものに限らないが、
不純物が多いと目的の半導体が得られない。
Typical raw materials for barium titanate include barium carbonate (BaC03) and titanium oxide (Ti02). The raw materials for barium titanate are not limited to those listed above, but
If there are too many impurities, the desired semiconductor cannot be obtained.

特に、鉄(Fe)、銅(Cu)、カリウム(K)、ナト
リウム(Na)、マグネシウム(Mg)、アルミニウム
(AI)等の不純物はチタン酸バリウムの半導体化に悪
影響があると言われている。半導体化剤としては、上記
した様にイットリウム等の3価の金属元素またはタンタ
ル等の5価の金属元素の一種又は二種以上を用いる。そ
の中でも、希±頚元素の酸化物が代表的なものである。
代表的な製造工程は、原料配合→湿式混合→脱水乾燥→
仮焼→粉砕→造粒→成形→本焼成である。
In particular, impurities such as iron (Fe), copper (Cu), potassium (K), sodium (Na), magnesium (Mg), and aluminum (AI) are said to have a negative effect on the semiconductor formation of barium titanate. . As the semiconductor agent, one or more of a trivalent metal element such as yttrium or a pentavalent metal element such as tantalum is used as described above. Among them, oxides of rare elements are representative.
The typical manufacturing process is raw material blending → wet mixing → dehydration drying →
The process is calcination → crushing → granulation → molding → main firing.

湿式混合、粉砕工程で不純物の混入を防止するためウレ
タンゴムで内張りしたステンレス製ポットおよびメノゥ
の宝石を使用するのも好ましい。仮暁は900℃ないし
1100午○程度で行う。
It is also preferable to use a stainless steel pot lined with urethane rubber and agate jewelry to prevent impurities from entering during the wet mixing and grinding steps. False dawn is carried out at around 900 degrees Celsius or 1100 o'clock in the morning.

この目的はチタン酸バリウム(舷Ti03)の合成と、
本焼成の際の焼成物の繊密化を図るためである。尚、本
発明に係る窒化チタニウム、窒化ジルコニウムまたは炭
化珪素の配合時期は、原料配合時でも、又、仮焼成の粉
砕工程で配合してもよい。以下、実験結果と共に本発明
のチタン酸バリウム系半導体磁器を説明する。実験例
1 本実験例は、従来のチタン酸バリウムーィットリゥム(
Ba,へYxTi03)半導体の焼成温度と室温比抵抗
の関係、および実施例に係る窒化チタニウム、窒化ジル
コニウム、炭化珪素を添加した場合の焼成温度と室温比
抵抗の関係を示すものである。
The purpose of this is to synthesize barium titanate (Board Ti03),
This is to make the fired product more delicate during the main firing. Incidentally, titanium nitride, zirconium nitride, or silicon carbide according to the present invention may be blended at the time of blending the raw materials, or may be blended during the pulverization step of pre-firing. The barium titanate semiconductor ceramic of the present invention will be explained below along with experimental results. Experimental example
1 This experimental example uses conventional barium yttrium titanate (
It shows the relationship between the firing temperature and room temperature resistivity of Ba, YxTi03) semiconductors, and the relationship between the firing temperature and room temperature resistivity when titanium nitride, zirconium nitride, and silicon carbide are added according to Examples.

従釆のチタン酸バリウムーィットリウム 母,へYxTi03)の半導体磁器組成のものと、それ
に窒化チタニウム(T州)、窒化ジルコニウム(ZrN
)、炭化珪素(SIC)を各々加えたものと4種類につ
いて半導体化温度を測定した。
The secondary barium titanate-yttrium matrix (YxTi03) has a semiconducting ceramic composition, as well as titanium nitride (T) and zirconium nitride (ZrN).
), silicon carbide (SIC) was added, and the semiconductor temperature was measured for four types.

尚、上記の×は0.003とした。Bろ.9的Yo.o
o3Ti03組成としては、炭酸バリウム、酸化イット
リウム、酸化チタンを、窒化チタニウム、窒化ジルコニ
ウム、炭化珪素として は微粉砕した夫々の粉末(くl
r)を各々用い、第1表に示す組成で配合した。
Note that the above x was set to 0.003. B. 9 Yo. o
The composition of o3Ti03 is barium carbonate, yttrium oxide, and titanium oxide, and titanium nitride, zirconium nitride, and silicon carbide are each finely pulverized powder.
r) were used, and the compositions shown in Table 1 were blended.

各々について、ウレタンラバ−で内張りし、メノー製玉
石をボールとしたボールミルで混合した。混合の後、1
100午○で2時間仮嬢を行なった。仮焼後、上記のボ
ールミルで十分に粉砕した。粉砕後、内径2仇舷の金型
に入れ、プレス圧600k9/塊で成形し、高さ3肌、
直径2Q舷の圧粉体を得た。次に、これらの圧粉体を1
240午0なし、し138000の第1表に示す如き各
温度にて1時間焼成した。
Each mixture was lined with urethane rubber and mixed in a ball mill using agate cobbles as balls. After mixing, 1
I acted as a temporary lady for 2 hours at 100pm. After calcining, it was thoroughly ground using the ball mill described above. After crushing, it is placed in a mold with an inner diameter of 2 mm and molded at a press pressure of 600k9/lump, with a height of 3 skins,
A green compact with a diameter of 2Q side was obtained. Next, these green compacts are
It was fired for 1 hour at each temperature shown in Table 1 of 240:00 and 138,000.

得られた焼成体の比抵抗を室温(20qo)で測定した
。焼成温度と比抵抗を第1表に合せて示す。第1表より
明らかの如く、窒化チタニウム、窒化ジルコニウム、炭
化珪素が配合されると、配合されない場合に比較し60
つ0なし、し80午○程度低い温度から半導体化および
暁鯖が可能であった。この理由については現在の所不明
であるが、窒化チタニウム、窒化ジルコニウム、炭化珪
素の添加剤が焼成時に発生する液相の組成に影響を及ぼ
すのではないかと考えられる。第1表 実験例 2 本実験例は、従来のチタン酸バリウムーィットリウム(
B1a,‐xYxTi03)半導体のイットリウム(Y
)量と室温比抵抗の関係、および本発明に係る窒化チタ
ニウム(TIN)、窒化ジルコニウム(ZrN)、炭化
珪素(SIC)を添加した場合のイットリウム(Y)量
と室温比抵抗の関係を示すものである。
The specific resistance of the obtained fired body was measured at room temperature (20 qo). The firing temperature and specific resistance are also shown in Table 1. As is clear from Table 1, when titanium nitride, zirconium nitride, and silicon carbide are blended, compared to the case where they are not blended, the
Semiconductorization and Akatsuki mackerel were possible at temperatures as low as 80 pm. The reason for this is currently unknown, but it is thought that the additives such as titanium nitride, zirconium nitride, and silicon carbide affect the composition of the liquid phase generated during firing. Table 1 Experimental Example 2 This experimental example is based on the conventional barium-yttrium titanate (
B1a, -xYxTi03) semiconductor yttrium (Y
) and the relationship between the amount of yttrium (Y) and the specific resistance at room temperature, and the relationship between the amount of yttrium (Y) and the specific resistance at room temperature when titanium nitride (TIN), zirconium nitride (ZrN), and silicon carbide (SIC) according to the present invention are added. It is.

母,〜YxTi03組成としては、炭酸バリウム、酸化
イットリウム、酸化チタンを原料として用い、イットリ
ウム(Y)量が0.1なし、し0.6原子%の範囲にて
配合した。
As for the composition of YxTi03, barium carbonate, yttrium oxide, and titanium oxide were used as raw materials, and the amount of yttrium (Y) was blended in a range of 0.1 to 0.6 at%.

窒化チタニウム、窒化ジルコニウムおよび炭化珪素はそ
れぞれ1.肌t%ずつ添加した。これら各々を用いて、
実験例1に示した方法と同様の方法にて夫々の半導体磁
器を得た。尚、その際の焼成は、1380q0にて行な
った。これにより得られた焼成体のイットリウム(Y)
量と室温比抵抗の関係を第1図に、添加剤が窒化チタニ
ウムの場合は曲線1、窒化ジルコニウムの場合には曲線
2、炭化珪素の場合は曲線3、無添加の場合には曲線4
の各曲線で示した。第1図により明らかの如く、本発明
に係る窒化チタニウム、窒化ジルコニウム、炭化珪素が
添加された場合にはイットリウム(Y)量の範囲に渡っ
て低い比抵抗が得られているに対し、無添加の場合には
イットリウム(Y)量が0.3原子%近傍の極く狭い範
囲でのみしか低い比抵抗が得られないのである。
Titanium nitride, zirconium nitride and silicon carbide are each 1. Each skin t% was added. Using each of these,
Each semiconductor ceramic was obtained in the same manner as shown in Experimental Example 1. Incidentally, the firing at that time was performed at 1380q0. Yttrium (Y) of the fired body thus obtained
Figure 1 shows the relationship between the amount and room temperature specific resistance. Curve 1 is when the additive is titanium nitride, Curve 2 is when it is zirconium nitride, Curve 3 is when it is silicon carbide, and Curve 4 is when there is no additive.
It is shown by each curve. As is clear from FIG. 1, when titanium nitride, zirconium nitride, and silicon carbide according to the present invention are added, low resistivity is obtained over a range of yttrium (Y) amounts, whereas when no additives are used, In this case, a low resistivity can be obtained only in an extremely narrow range in which the amount of yttrium (Y) is around 0.3 atomic %.

従って、本発明に係る窒化チタニウム、窒化ジルコニウ
ム、炭化珪素は、半導体化剤の有効添加量範囲を大きく
拡げていることが分る。
Therefore, it can be seen that the titanium nitride, zirconium nitride, and silicon carbide according to the present invention greatly expand the effective addition amount range of the semiconductor agent.

実験例 3 本実験例は、従来のチタン酸バリウムーイツトリウム(
BaMYxTj03)半導体に本発明に係る窒化チタニ
ウム(TIN)、窒化ジルコニウム(ZrN)、炭化珪
素(SIC)を添加した場合の、添加量と室温比抵抗と
の関係を示するものである。
Experimental Example 3 In this experimental example, the conventional barium-yttrium titanate (
This figure shows the relationship between the amount of addition and the specific resistance at room temperature when titanium nitride (TIN), zirconium nitride (ZrN), and silicon carbide (SIC) according to the present invention are added to a BaMYxTj03) semiconductor.

0.3原子%イットリウム(Y)をドープしたチタン酸
バリウム半導体を用い、実験例1と同様の方法にて各々
の半導体磁器を得た。
Each semiconductor ceramic was obtained in the same manner as in Experimental Example 1 using a barium titanate semiconductor doped with 0.3 at % yttrium (Y).

その際、焼成は1300『0にて1時間行なった。得ら
れた焼成体の本発明に係る添加剤の量と室温比抵抗との
関係を第2表に示す。第1表の比較例に示した様に、本
発明に係る添加剤を配合しないでイットリウム(Y)を
0.3原子%添加したチタン酸バリウムの焼成温度13
00ooに於ける焼成物の室温(20o0)での比抵抗
は著しく高い値(IQQ・抑)である。
At that time, firing was performed at 1300° for 1 hour. Table 2 shows the relationship between the amount of the additive according to the present invention and the room temperature resistivity of the obtained fired body. As shown in the comparative example in Table 1, the firing temperature of barium titanate to which 0.3 at.% of yttrium (Y) was added without adding the additive according to the present invention was 13.
The specific resistance of the fired product at room temperature (20o0) at 00oo is an extremely high value (IQQ/inhibition).

そして、焼成温度が1360oo程度になると始めて比
抵抗が200・即程度となる。しかし、第2表に示する
如く、窒化チタニウム、窒化ジルコニウム、炭化珪素の
少なくとも1種以上を添加した場合には、添加量0.1
wt%に於いて既に低い比抵抗と成り、更に添加量を多
くしても、2wt%程度迄は、抵抗値は殆ど変わらない
。この様に本発明に係る添加剤の幅広い添加量範囲に於
いて、無添加の場合と比較しかなり低温でイットリウム
(Y)をドープしたチタン酸バリウムの半導体化が可能
であった。しかし、添加量が3.小れ%以上になると比
抵抗の値が大きくなる。従って、本発明に係る添加剤の
添加量は0.1なし、し2.肌t%の範囲がよい。
Then, only when the firing temperature reaches about 1360 oo, the specific resistance becomes about 200. However, as shown in Table 2, when at least one of titanium nitride, zirconium nitride, and silicon carbide is added, the amount of addition is 0.1
The specific resistance is already low at wt%, and even if the amount added is further increased, the resistance value hardly changes up to about 2wt%. As described above, within a wide range of addition amounts of the additive according to the present invention, it was possible to convert barium titanate doped with yttrium (Y) into a semiconductor at a considerably lower temperature than when no additive is added. However, the amount added is 3. If it becomes less than %, the value of specific resistance increases. Therefore, the amount of additives added according to the present invention is 0.1% and 2%. The skin t% range is good.

また本発明に係る添加剤を夫々0.5M%ずつ2種類混
合させた場合について、上誌と同様の方法にて半導体磁
器を得、得られた焼成体の本発明に係る添加剤の添加量
と室温比抵抗との関係を調べた。
In addition, in the case where two types of additives according to the present invention are mixed at 0.5 M% each, semiconductor porcelain is obtained by the same method as above, and the amount of additives according to the present invention in the obtained fired body is The relationship between this and room temperature resistivity was investigated.

その関係を第2表に示す。第2表より明らかの如く、本
発明に係る添加剤を2種類混合し配合させた場合に於い
ても、同様の効果を有することが分る。第2表 実験例 4 本実験例は、従来のチタン酸バリウムーィットリゥム(
BaMYxTi03)半導体に本発明に係る窒化チタニ
ウム(TIN)、窒化ジルコニウム(ZrN)、炭化珪
素(SIC)を添加した場合の、添加量と比抵抗変化中
との関係を示するものである。
The relationship is shown in Table 2. As is clear from Table 2, it can be seen that similar effects are obtained even when two types of additives according to the present invention are mixed and blended. Table 2 Experimental Example 4 This experimental example uses conventional barium yttrium titanate (
This figure shows the relationship between the amount of addition and the change in specific resistance when titanium nitride (TIN), zirconium nitride (ZrN), and silicon carbide (SIC) according to the present invention are added to a BaMYxTi03) semiconductor.

ここで、比抵抗変化中とは、半導体磁器の温度対比抵抗
の関係に於ける比抵抗の最大値(pmax)と最小値(
pmin)の比とする。
Here, the term "currently changing resistivity" means the maximum value (pmax) and minimum value (pmax) of resistivity in the relationship between temperature and resistance of semiconductor ceramics.
pmin).

0.3原子%イットリウム(Y)をドーブしたチタン酸
バリウム半導体を用い、これに本発明に係る添加剤を種
々の割合で添加し、実験例1と同様の方法にて各々の半
導体磁器を得た。
Using a barium titanate semiconductor doped with 0.3 atom% yttrium (Y), the additives according to the present invention were added in various proportions, and each semiconductor ceramic was obtained in the same manner as in Experimental Example 1. Ta.

その際、焼成温度は1380qoとした。得られた焼成
体の本発明に係る添加剤の量と比抵抗変化中との関係を
第2図に、添加剤が窒化チタニウムの場合は曲線5、室
化ジルコニウムの場合は曲線6、炭化珪素の場合は曲線
7の各曲線で、また無添加の場合は′点8でそれぞれ示
した。第2図より明らかの如く、本発明に係る添加剤を
添加した場合には、0.1〜2.肌t%の添加量の広し
・範囲で比抵抗変化中が1ぴないし1びであり、無添加
の場合の値の1び程度(図中4)を大幅に改善すること
が分る。
At that time, the firing temperature was 1380 qo. The relationship between the amount of the additive according to the present invention and the change in resistivity of the obtained fired body is shown in FIG. In the case of , each curve is shown as curve 7, and in the case of no additive, it is shown as point 8. As is clear from FIG. 2, when the additive according to the present invention is added, 0.1 to 2. It can be seen that the change in resistivity is 1 to 1 degree over a wide range of the addition amount of skin t%, and the value is significantly improved by about 1 degree (4 in the figure) when no additive is added.

実験例 5 本実験例は、従来のチタン酸バリウム−イットリウム(
Ba,TYxTi03)半導体に本発明に係る窒化チタ
ニウム(TIN)、室化ジルコニウム(ZrN)、炭化
珪素(SIC)を添加した場合の、添加量とPTC領域
に於ける抵抗変化率との関係を示するものである。
Experimental Example 5 In this experimental example, the conventional barium titanate-yttrium (
Figure 2 shows the relationship between the amount of addition and the rate of change in resistance in the PTC region when titanium nitride (TIN), zirconium chamber (ZrN), and silicon carbide (SIC) according to the present invention are added to a Ba, TYxTi03) semiconductor. It is something to do.

ここで、抵抗変化率(△p/△T)は次の様に定義する
Here, the resistance change rate (Δp/ΔT) is defined as follows.

△p/△T=(pmax−pmin)/(Tpmax−
Tpm【n)Tpmax:比抵抗最大を示す温度 Tpmin:比抵抗最小を示す温度 試料としての半導体磁器は、試験例4で得られた焼成体
を用いる。
△p/△T=(pmax-pmin)/(Tpmax-
Tpm[n) Tpmax: Temperature at which the specific resistance is maximum Tpmin: Temperature at which the specific resistance is the minimum The fired body obtained in Test Example 4 is used as the semiconductor ceramic sample.

その本発明に係る添加剤の量とPTC領域に於ける抵抗
変化率との関係を第3図に、添加剤が窒化チタニウムの
場合は曲線9、窒化ジルコニウムの場合は曲線10、炭
化珪素の場合は曲線11の各曲線で、無添加の場合は点
I2でそれぞれ示した。第3図より明らかの如く、本発
明に係る添加剤の添加により、その添加量が0.1なし
、し2.肌t%の広い範囲に於いて、△p/△Tの値を
大きく改善することが分る。
The relationship between the amount of the additive and the rate of change in resistance in the PTC region according to the present invention is shown in Figure 3, where curve 9 is used as the additive when titanium nitride is used, curve 10 is used when the additive is used as zirconium nitride, and curve 10 is used when the additive is used as the additive in the PTC region. is each curve of curve 11, and the case of no additive is shown as point I2. As is clear from FIG. 3, the addition of the additive according to the present invention reduces the amount of addition from 0.1 to 2. It can be seen that the value of Δp/ΔT is greatly improved over a wide range of skin t%.

これは、即ち、抵抗変化の立ち上がりが急しゆんである
ことに他ならない。実験例 6本実験例は、従来のチタ
ン酸バリウムーランタン(BaMLaxTi03)半導
体、チタン酸バリウム−セリウム(欧.‐xCexTi
03)半導体、チタン酸バリウムーアンチモン(Ba,
‐xS広Ti03)半導体に本発明に係る添加剤を添加
した場合の、添加剤と室温比抵抗との関係を示するもの
である。
This is nothing but the fact that the rise of the resistance change is slowing down rapidly. Experimental Example 6 This experimental example uses a conventional barium-lanthanum titanate (BaMLaxTi03) semiconductor, barium-cerium titanate (EU.-xCexTi)
03) Semiconductor, barium titanate-antimony (Ba,
-xS wide Ti03) It shows the relationship between the additive and room temperature resistivity when the additive according to the present invention is added to a semiconductor.

チタン酸バリウムに、ランタン(La)、セリウム(C
e)、アンチモン(Sb)を各々0.6原子%ドープし
た。
Barium titanate, lanthanum (La), cerium (C)
e), antimony (Sb) was doped at 0.6 atomic %.

この場合の比抵抗は、それぞれ1『(い)、1ぴ(Ce
)、IQ(Sb)○・伽であった。これらの各化学組成
のチタン酸バリウムに、窒化チタニウム(TIN)、窒
化ジルコニウム(ZrN)、炭化珪素(SIC)をそれ
ぞれ0.5wt%配合し、実験例1と同様の方法にて各
々の半導体磁器を得た。その際、焼成は1300℃にて
1時間行なった。得られた焼成体の本発明に係る添加剤
と室温比抵抗の関係を第3表に示す。第3表より明らか
の如く、本発明に係る添加剤を0.5wt%配合すると
、イットリウム(Y)を半導体化剤としてドープした場
合と同様に、半導化剤の添加量の幅を増大させる働きが
あることが分る。
In this case, the specific resistances are 1' (i) and 1 pi (Ce), respectively.
), and IQ (Sb) was ○. 0.5 wt% of each of titanium nitride (TIN), zirconium nitride (ZrN), and silicon carbide (SIC) was added to barium titanate having each of these chemical compositions, and each semiconductor ceramic was prepared in the same manner as in Experimental Example 1. I got it. At that time, firing was performed at 1300° C. for 1 hour. Table 3 shows the relationship between the additives according to the present invention and the room temperature specific resistance of the obtained fired bodies. As is clear from Table 3, when 0.5 wt% of the additive according to the present invention is added, the range of the amount of the semiconducting agent added increases, similar to when doping yttrium (Y) as the semiconducting agent. I know it's working.

尚、これらの半導体化チタン酸バリウムのPTC効果は
pmax/pminが1ぴ〜1ぴであり、いずれも優れ
たPTC特性を示した。第3表
The PTC effect of these barium titanate semiconductors had a pmax/pmin of 1 to 1 p, and all exhibited excellent PTC characteristics. Table 3

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

図は、本発明の実験例を示し、第1図は第2実験例の於
けるイットリウム量と室温比抵抗の関係を示す線図、第
2図は本発明に係る添加剤の添加量と比抵抗変化中との
関係を示す線図、第3図は本発明に係る添加剤の添加量
とPTC領域に於ける抵抗変化率との関係を示す線図で
ある。 努)図 第2図 第3図
The figures show experimental examples of the present invention, Figure 1 is a diagram showing the relationship between the amount of yttrium and room temperature specific resistance in the second experimental example, and Figure 2 is a diagram showing the amount and ratio of additives according to the present invention. FIG. 3 is a diagram showing the relationship between the amount of additive and the rate of change in resistance in the PTC region according to the present invention. Figure 2 Figure 3

Claims (1)

【特許請求の範囲】 1 チタン酸バリウムと微量の半導体化剤とからなるチ
タン酸バリウム系半導体に、窒化チタニウム、窒化ジル
コニウム又は炭化珪素のうち少なくとも一種類を0.1
ないし2.0重量%添加してなることを特徴とするチタ
ン酸バリウム系半導体磁器。 2 前記半導体化剤は、イツトリウム、ランタン、セリ
ウム、サマリウム、デイスプロシウム、アンチモンなど
の3価の金属元素およびニオブ、タンタル、ビスマスな
どの5価の金属元素であることを特徴とする特許請求の
範囲第1項のチタン酸バリウム系半導体磁器。
[Claims] 1. At least one of titanium nitride, zirconium nitride, or silicon carbide is added to a barium titanate-based semiconductor consisting of barium titanate and a trace amount of a semiconductor agent in an amount of 0.1
A barium titanate-based semiconductor porcelain characterized by containing at least 2.0% by weight of barium titanate. 2. The semiconductor forming agent is a trivalent metal element such as yttrium, lanthanum, cerium, samarium, disprosium, and antimony, and a pentavalent metal element such as niobium, tantalum, and bismuth. Barium titanate-based semiconductor porcelain of scope 1.
JP56212205A 1981-05-06 1981-12-25 Barium titanate semiconductor porcelain Expired JPS6031794B2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP56212205A JPS6031794B2 (en) 1981-12-25 1981-12-25 Barium titanate semiconductor porcelain
US06/373,817 US4384989A (en) 1981-05-06 1982-04-30 Semiconductive barium titanate
GB8212709A GB2097778B (en) 1981-05-06 1982-04-30 Barium titanate composition
CA000402293A CA1189770A (en) 1981-05-06 1982-05-05 Semiconductive barium titanate

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56212205A JPS6031794B2 (en) 1981-12-25 1981-12-25 Barium titanate semiconductor porcelain

Publications (2)

Publication Number Publication Date
JPS58115075A JPS58115075A (en) 1983-07-08
JPS6031794B2 true JPS6031794B2 (en) 1985-07-24

Family

ID=16618657

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56212205A Expired JPS6031794B2 (en) 1981-05-06 1981-12-25 Barium titanate semiconductor porcelain

Country Status (1)

Country Link
JP (1) JPS6031794B2 (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
RU2007119938A (en) * 2004-12-09 2009-01-20 Хрд Корп. (Us) CATALYST AND METHOD FOR CONVERTING PARAFFIN HYDROCARBONS WITH A LOW MOLECULAR WEIGHT IN ALKENES

Also Published As

Publication number Publication date
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