JPS6312324B2 - - Google Patents

Info

Publication number
JPS6312324B2
JPS6312324B2 JP56015968A JP1596881A JPS6312324B2 JP S6312324 B2 JPS6312324 B2 JP S6312324B2 JP 56015968 A JP56015968 A JP 56015968A JP 1596881 A JP1596881 A JP 1596881A JP S6312324 B2 JPS6312324 B2 JP S6312324B2
Authority
JP
Japan
Prior art keywords
weight
pulse voltage
batio
amount
present
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
JP56015968A
Other languages
Japanese (ja)
Other versions
JPS57130302A (en
Inventor
Masaru Masujima
Yoshishige Towatari
Shoichi Iwatani
Hitoshi Masumura
Hisao Abe
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.)
TDK Corp
Original Assignee
TDK Corp
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 TDK Corp filed Critical TDK Corp
Priority to JP56015968A priority Critical patent/JPS57130302A/en
Publication of JPS57130302A publication Critical patent/JPS57130302A/en
Publication of JPS6312324B2 publication Critical patent/JPS6312324B2/ja
Granted legal-status Critical Current

Links

Description

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

本発明は非直線性誘電体素子にかかり、特に
BaTiO3系多結晶体からなる、非直線性特性及び
絶縁破壊電圧の優れた非直線性誘電体素子に関す
るものである。 一般にBaTiO3系磁器を中心とするペロブスカ
イト形構造を有するABO3系強誘電体の応用分野
としては、高誘電率の利用、圧電的性質の利用の
外に強誘電体の非直線性の応用が知られている。
つまり誘電率が電界の強度によつて変化すること
を利用する非線形(可飽和)素子、ヒステリシス
特性を利用する記憶蓄積素子、論理演算素子等の
用途にBaTiO3単結晶を用いると、その使用周波
数の限界も上がり、消費電力も非常に小さく小型
大容量のものが容易に得られる等の大きな効果が
予想されて、この応用研究がすでにベル研究所で
Andreson等によつて発表されている。ところが
疲労現象やしきい(threshold)の電場がない等
の欠点が明らかになり実用化に至つていない。 最近、新規の用途例として非線形(可飽和)素
子として螢光灯、水銀灯、ナトリウム放電灯類の
放電灯・無接点起動装置に用いることが特公昭48
−28726に開示され、更に強誘電体素体表面を鏡
面加工、エツチング処理によつて可飽和曲線の良
好な非線形素子が得られることは特開昭52−
146069等で知られている。 ところが、かかる用途に使用される非線形素子
(以下非直線性誘電体素子と称す)としてはD−
Eヒステリシス曲線の傾斜が急しゆんなこと、誘
電率が高い値でしかも温度に対して非直線性特性
が安定であること、D−Eヒステリシスの温度特
性が良好であること、つまりその電圧Vと電荷Q
の関係が第1図Aに示すようなD−Eヒステリシ
ス曲線が角形特性であり、温度に対して安定でる
ことが要求されている。 BaTiO3単結晶は、かかる曲線が角形特性を示
す為に非直線性誘電体素子としては有効であるが
温度変化に対して非直線特性が不安定である。又
BaTiO3単結晶の育成にフラツクス法、溶融法等
が知られている。しかるに製造方法そのものがま
だ研究段階で実用化に至つていない。そこで、従
来のBaTiO3系多結晶体は一般に第1図Bに示す
ようなD−Eヒステリシス曲線がある程度の飽和
特性を示すが、残留分極のバラツキが大きく誘電
率を温度に対して不安定であり、かつD−Eヒス
テリシス曲線の傾斜が緩慢であり非直線性誘電体
素子として実用化に至つていないのが現状であ
る。 そこで本発明者らは、BaTiO3系の多結晶体体
で、BaTiO3単結晶に近い特性を持ち安定して工
業的に製造可能とすることを目的に鋭意研究を重
ねた結果、BaTiO3系多結晶体、特に良好なもの
としてBaTiO3のTiの一部をZrで置換した固溶体
BaO−TiO2−ZrO2がZrの添加量によつてキユリ
ー点が低温側に移行した状態の固溶体を選択して
実験を行なつた結果、容量電圧特性がもつとも非
直線性を示す、最適な領域としてBaO−TiO2
ZrO2系でBaO………63.39〜65.62重量%、TiO2
………26.42〜33.85重量%、ZrO2……0.53〜10.19
重量%の範囲(これらの合計は100.00重量%)か
らなる基本組成がもつとも良好であることが確認
された。 更にこのような基本組成物100に対し添加剤と
してMn酸化物、Cr酸化物、Mnの炭酸塩、Crの
炭酸塩の少なくとも一種類を0.01〜0.40重量%
(複合添加の場合は、合計値)含有させることに
よつてBaTiO3の持つ固有のヒステリシス特性を
損うことなく磁器焼結に際して、還元防止あるい
はその焼結性が向上し、より緻密で均質な優れた
多結晶体が得られることが判明した(第7図及び
第2表を参照)。 また、Al2O3やSiO2のように通常原料中に混入
されたり製造工程で混入するいわゆる不純物や
又、時として意図的に添加するような酸化物も前
記基本組成物100に対し0.15重量%以下にしなけ
ればならないことが明確となつた。これらの許容
量は通常コンデンサ用誘電体を製造する際の添加
剤や不純物の量に比較し極めて少なく特異であ
る。 これらの結果、すなわち本発明の非直線性誘電
体素子は新規なものとして、D−Eヒステリシス
曲線の傾斜が急しゆんで、誘電率が高い値で、し
かも温度特性がBaTiO3単結晶に比較し極めて安
定であり、誘電体損失の小さい極めて優れた特徴
を有するものでありパルス発生器、放電灯・点灯
装置等の非直線性誘電体素子としての実用化が可
能となつたものである。 以下実施例をあげて本発明を詳細に説明する。
第1図AはBaTiO3単結晶体のD−Eヒステリシ
ス曲線例図であり、同図Bは従来のBaTiO3多結
晶体のD−Eヒステリシス曲線例図である。 第2図は本発明の実施例である非直線性誘電体
素子のD−Eヒステリシス曲線例図である。 第3図は本発明の非直線性誘電体素子を用いた
放電灯・無接点起動装置の回路図である。 第4図及び第5図は第3図に示す回路の動作原
理を示す回路および動作波形図である。 第6図〜第10図は本発明の実施例に係るもの
で、第6図は本発明によるBaTiO3多結晶体の
BaO−TiO2−ZrO2系組成比別のパルス電圧の温
度特性を示す。 第7図は添加物−パルス電圧の関係を示す。 第8図は不純物−パルス電圧の関係を示す。 第9図は不純物の量と結晶体構造との関係を示
すもので、この結晶体の結晶構造の顕微鏡写真で
ある。 第10図は本発明素子の、不純物量別の時間経
過とパルス電圧との関係を示すものである。 実施例 1 原料粉末BaCO3、TiO2、ZrO2、MnCO3を第1
表の組成となるようにポリエチレンポツト、メノ
ーボールを用いて湿式混合した。脱水乾燥後1150
℃で2時間保持し、仮焼成せしめ、その後ふたた
びポリエチレンポツト、メノーボールを用いて粉
砕を行なつた。水分を蒸発させたのちこれに適当
量のバインダーを加え、直径16.5mmφ、厚さ0.45
mmの円板に10トンプレスで加圧成型した。ついで
1300〜1400℃で2時間焼成せしめた。 かくして得られた磁器素子に銀電極を焼付、そ
の後パルス電圧特性、パルス電圧温度特性を第3
図の回路で測定し、ついでそのD−Eヒステリシ
ス曲線を測定した。その例図を第2図に示す。ま
た誘電率(εs)、誘電体損失tanδ(%)及び絶縁抵
抗IRを測定した。上記電気的特性の測定値は第
1表にまとめたとおりである。 上記パルス発生の簡単な動作原理については、
動作原理図及び動作波形図を第4図、第5図に示
す。 第3図においてCnは非直線性誘電体素子であ
り、その特性は第2図に示す通りである。 第5図においてはAは通常のコンデンサの特性
であり、QはEに比例する。しかるにBは本発明
による素子の特性であり、E0以上ではQがほぼ
一定となる。Q<C>=C(F)×V(V)であるか
ら、同図Bになる特性は電圧がE0以上では見掛
上の容積が急激に減少し、蓄積される電荷は飽和
し結果として、充電電流が急激に減少する。 このため、安定器では第4図に示す様にL×
di/dtに比例した逆起電力が生じ、放電灯FLを
起動させるトリガー(パルス)電圧が発生する。 Lは安定器のインダクタンスでありdi/dtは非
直線性誘電体素子の充電電流の変化である。di/
dtを大きくとるために、第5図に於けるE0(V)
以下の充電電流の傾きとE0(V)以上で飽和充電
電流の傾きの差が大きい程トリガー(パルス)電
圧が高くなり安定に起動させることが出来る。故
にCn素子のD−Eヒステリシスとしては角形特
性に近いことが必要となる。このヒステリシス形
態を定量的に表わすことは容易ではないが本実験
では第3図に示す回路によるパルス電圧をこのヒ
ステリシス形態の定量的な尺度とした。第4図に
於いて例えばE0(V)を適当な値に設定した交流
電圧をCn素子に印加した時、第5図に示される
ようにE0に於て充電電流は急激に変化し、前述
の如く安定器のインダクタンスLに比例した逆起
電力によるパルスが交流電圧のE0に重畳される。
このパルス電圧が第3図に於ける放電灯の起動パ
ルス即ちトリガーとなるものである。 以上、第1表からわかるように本発明範囲範囲
内のものはパルス電圧特性が450〜900Vの高い値
を示している。 尚試料No.1、7は本発明範囲外である。 更に第6図に示すようにBaOが63.39〜65.62重
量%、ZrO2が0.53〜10.19重量%としたものは−
30〜+60℃に於て470〜900Vと高電圧パルスが発
生し十分に実用可能であることが確認された。 以上第1表および第6図により、本発明では
BaO−TiO2−ZrO2系基本組成物に於てBaOを
63.39〜65.62重量%、TiO226.42〜33.85重量%、
ZrO20.53〜10.19重量%に限定するものである。
The present invention relates to nonlinear dielectric elements, and particularly
The present invention relates to a nonlinear dielectric element made of BaTiO 3 -based polycrystalline material and having excellent nonlinearity characteristics and breakdown voltage. In general, the application fields of ABO 3 -based ferroelectrics, which have a perovskite structure centered on BaTiO 3 -based porcelain, include the use of high permittivity and piezoelectric properties, as well as the application of nonlinearity of ferroelectrics. Are known.
In other words, if BaTiO 3 single crystal is used for nonlinear (saturable) elements that utilize the fact that the dielectric constant changes depending on the strength of the electric field, memory storage elements that utilize hysteresis characteristics, logical operation elements, etc., the operating frequency This applied research is already being carried out at Bell Laboratories, as it is expected to have great effects, such as raising the limits of energy consumption and making it easier to create small, large-capacity devices with very low power consumption.
Published by Andreson et al. However, drawbacks such as fatigue and the absence of a threshold electric field have become apparent, and it has not been put into practical use. Recently, as a new application example, nonlinear (saturable) elements have been used in discharge lamps and non-contact starting devices for fluorescent lamps, mercury lamps, and sodium discharge lamps.
-28726, and that a nonlinear element with a good saturability curve can be obtained by mirror-finishing and etching the surface of a ferroelectric element is disclosed in JP-A-52-28726.
It is known as 146069 etc. However, D-
The slope of the E hysteresis curve is steep, the dielectric constant is high and the nonlinearity characteristics are stable with respect to temperature, and the temperature characteristics of the D-E hysteresis are good, that is, the voltage V and charge Q
The D-E hysteresis curve as shown in FIG. 1A has a rectangular characteristic and is required to be stable with respect to temperature. BaTiO 3 single crystal is effective as a nonlinear dielectric element because its curve exhibits square characteristics, but its nonlinear characteristics are unstable with respect to temperature changes. or
Flux methods, melting methods, etc. are known for growing BaTiO 3 single crystals. However, the manufacturing method itself is still in the research stage and has not yet been put into practical use. Therefore, conventional BaTiO 3 -based polycrystals generally exhibit a certain degree of saturation characteristics in the DE hysteresis curve shown in Figure 1B, but the residual polarization varies widely and the dielectric constant is unstable with respect to temperature. However, the slope of the DE hysteresis curve is slow, and at present it has not been put to practical use as a nonlinear dielectric element. Therefore, the present inventors conducted extensive research with the aim of creating a BaTiO 3 -based polycrystalline body that has properties similar to BaTiO 3 single crystals and can be stably manufactured industrially. Polycrystals, particularly good ones include solid solutions in which part of the Ti in BaTiO 3 is replaced with Zr.
As a result of conducting experiments by selecting a solid solution of BaO−TiO 2 −ZrO 2 in which the Curie point shifted to the lower temperature side depending on the amount of Zr added, the results showed that the optimal capacitance-voltage characteristic showed nonlinearity. BaO−TiO 2 − as a region
ZrO 2 system with BaO……63.39~65.62% by weight, TiO 2
......26.42 ~ 33.85 wt%, ZrO 2 ...0.53 ~ 10.19
It was confirmed that the basic composition consisting of a range of weight % (the sum of these is 100.00 weight %) is very good. Furthermore, 0.01 to 0.40% by weight of at least one of Mn oxide, Cr oxide, Mn carbonate, and Cr carbonate is added as an additive to 100% of the basic composition.
(Total value in case of combined addition) By adding BaTiO 3 , it prevents reduction or improves sinterability during porcelain sintering without impairing the inherent hysteresis characteristics of BaTiO 3, resulting in more dense and homogeneous sintering. It was found that an excellent polycrystalline material was obtained (see FIG. 7 and Table 2). In addition, so-called impurities such as Al 2 O 3 and SiO 2 that are usually mixed into raw materials or mixed in the manufacturing process, and oxides that are sometimes intentionally added are also added by weight of 0.15 to 100 of the basic composition. It became clear that it had to be kept below %. These allowable amounts are extremely small and unique compared to the amounts of additives and impurities used when manufacturing dielectrics for capacitors. As a result of these results, the nonlinear dielectric element of the present invention is novel, has a steep slope of the D-E hysteresis curve, has a high dielectric constant, and has temperature characteristics compared to BaTiO 3 single crystal. However, it is extremely stable and has extremely excellent characteristics of low dielectric loss, making it possible to put it to practical use as a nonlinear dielectric element in pulse generators, discharge lamps, lighting devices, etc. The present invention will be explained in detail below with reference to Examples.
FIG. 1A is an example of a DE hysteresis curve of a BaTiO 3 single crystal, and FIG. 1B is an example of a DE hysteresis curve of a conventional BaTiO 3 polycrystal. FIG. 2 is an example of a DE hysteresis curve of a nonlinear dielectric element according to an embodiment of the present invention. FIG. 3 is a circuit diagram of a discharge lamp/non-contact starting device using the nonlinear dielectric element of the present invention. 4 and 5 are circuits and operation waveform diagrams showing the operating principle of the circuit shown in FIG. 3. FIG. Figures 6 to 10 relate to embodiments of the present invention, and Figure 6 shows a BaTiO 3 polycrystalline body according to the present invention.
The temperature characteristics of the pulse voltage according to the BaO−TiO 2 −ZrO 2 system composition ratio are shown. FIG. 7 shows the additive-pulse voltage relationship. FIG. 8 shows the impurity-pulse voltage relationship. FIG. 9 shows the relationship between the amount of impurities and the crystal structure, and is a microscopic photograph of the crystal structure of this crystal. FIG. 10 shows the relationship between the time course and the pulse voltage for each impurity amount in the device of the present invention. Example 1 Raw material powders BaCO 3 , TiO 2 , ZrO 2 , MnCO 3 as the first
Wet mixing was performed using a polyethylene pot and an agate ball to obtain the composition shown in the table. 1150 after dehydration and drying
The mixture was kept at ℃ for 2 hours to undergo temporary calcination, and then pulverized again using a polyethylene pot and an agate ball. After evaporating the water, add an appropriate amount of binder to it and make it with a diameter of 16.5mmφ and a thickness of 0.45mm.
It was press-molded into a 10-ton press into a disc of mm. Then
It was baked at 1300-1400°C for 2 hours. A silver electrode was baked on the thus obtained ceramic element, and then the pulse voltage characteristics and pulse voltage temperature characteristics were
Measurements were made using the circuit shown in the figure, and then its DE hysteresis curve was measured. An example diagram is shown in FIG. In addition, the dielectric constant (ε s ), dielectric loss tan δ (%), and insulation resistance IR were measured. The measured values of the above electrical characteristics are summarized in Table 1. Regarding the simple operating principle of the above pulse generation,
The operating principle and operating waveform diagrams are shown in FIGS. 4 and 5. In FIG. 3, Cn is a nonlinear dielectric element whose characteristics are as shown in FIG. In FIG. 5, A is the characteristic of a normal capacitor, and Q is proportional to E. However, B is a characteristic of the device according to the present invention, and Q becomes approximately constant above E 0 . Since Q<C>=C(F)×V(V), the characteristic shown in B in the same diagram is that when the voltage exceeds E0 , the apparent volume decreases rapidly, the accumulated charge saturates, and the result is As a result, the charging current decreases rapidly. For this reason, in the ballast, as shown in Figure 4,
A back electromotive force proportional to di/dt is generated, generating a trigger (pulse) voltage that starts the discharge lamp FL. L is the inductance of the ballast and di/dt is the change in the charging current of the nonlinear dielectric element. di/
In order to increase dt, E 0 (V) in Figure 5
The larger the difference between the slope of the charging current below and the slope of the saturated charging current above E 0 (V), the higher the trigger (pulse) voltage becomes, allowing stable activation. Therefore, the DE hysteresis of the Cn element needs to be close to the square characteristic. Although it is not easy to express this hysteresis form quantitatively, in this experiment, the pulse voltage from the circuit shown in FIG. 3 was used as a quantitative measure of this hysteresis form. In Fig. 4, for example, when an AC voltage with E 0 (V) set to an appropriate value is applied to the Cn element, the charging current changes rapidly at E 0 as shown in Fig. 5. As described above, a pulse due to a back electromotive force proportional to the inductance L of the ballast is superimposed on the AC voltage E 0 .
This pulse voltage serves as a starting pulse or trigger for the discharge lamp in FIG. As can be seen from Table 1, the pulse voltage characteristics within the range of the present invention exhibit high values of 450 to 900V. Note that Samples Nos. 1 and 7 are outside the scope of the present invention. Furthermore, as shown in Fig. 6, when BaO is 63.39 to 65.62% by weight and ZrO 2 is 0.53 to 10.19% by weight, -
It was confirmed that high voltage pulses of 470 to 900V were generated at temperatures of 30 to +60°C, and that it was sufficiently practical. According to Table 1 and FIG. 6 above, in the present invention,
BaO in the basic composition of BaO−TiO 2 −ZrO 2
63.39-65.62 wt%, TiO2 26.42-33.85 wt%,
ZrO 2 is limited to 0.53 to 10.19% by weight.

【表】 実施例 2 第1表に示したBaTiO392モル%、BaZrO38モ
ル%のBaO−TiO2−ZrO2系組成物(MnCO3を含
まず)に添加剤(鉱化剤)としてMnCO3
Cr2O3の一方又は双方(複合添加)を第2表及び
第7図に示すように添加せしめて、実施例1と同
様にしてパルス電圧を求めた。 第2表(試料No.1〜18)において、添加物の添
加量によつてパルス電圧が格段に向上する効果を
有する。これ等の添加物を添加する時は、例えば
MnはMnCO3、CrはCr2O3として添加したがこれ
に限定するものではなく、他の形の化合物として
用いても、同様の効果がみとめられるものであ
り、その添加量も添加する化合物の状態を勘案す
べきであるが、主成分100に対して0.01〜0.4重量
%が実用範囲内と考えられ、0.4重量%を超える
範囲では電気的特性の劣化が著しくなつて好まし
くない。第7図は添加量とパルス電圧との関係を
グラフに示したものであるが、この図から見ても
添加量が0.01〜0.4重量%の範囲が電気的特性、
特にパルス電圧が満足される範囲であると言つて
よい。この場合、0.01重量%未満では添加による
効果が全くみとめられない。 更に、MnCO3、Cr2O3の添加によつて焼結に
際し、磁器の還元防止あるいはより緻密なる焼結
を促進する効果がある。 なお、〇印を付していない試料No.1、6、7、
8、13、14、17、18は本発明範囲外である。
[Table] Example 2 As an additive (mineralizer) to the BaO-TiO 2 -ZrO 2 composition (not containing MnCO 3 ) containing 92 mol% of BaTiO 3 and 8 mol% of BaZrO 3 shown in Table 1. MnCO3 ,
One or both of Cr 2 O 3 (combined addition) were added as shown in Table 2 and FIG. 7, and the pulse voltage was determined in the same manner as in Example 1. In Table 2 (Samples Nos. 1 to 18), the pulse voltage was significantly improved depending on the amount of the additive added. When adding these additives, for example
Although Mn is added as MnCO 3 and Cr is added as Cr 2 O 3 , the present invention is not limited to these. Similar effects can be observed even when other forms of compounds are used, and the amount of addition also depends on the compound added. However, 0.01 to 0.4% by weight based on 100% of the main component is considered to be within the practical range, and if it exceeds 0.4% by weight, the electrical characteristics will deteriorate significantly, which is not preferable. Figure 7 is a graph showing the relationship between the amount of addition and the pulse voltage. From this figure, it can be seen that the range of the amount of addition of 0.01 to 0.4% by weight is the electrical property.
In particular, it can be said that this is a range that satisfies the pulse voltage. In this case, if the amount is less than 0.01% by weight, no effect will be observed at all. Furthermore, the addition of MnCO 3 and Cr 2 O 3 has the effect of preventing reduction of the porcelain or promoting denser sintering during sintering. In addition, sample No. 1, 6, 7, which is not marked with 〇
8, 13, 14, 17, and 18 are outside the scope of the present invention.

【表】 実施例 3 通常の誘電体組成物に於ては実施例2でのベた
ような添加剤の他にSiO2、Al2O3等を焼結促進助
剤として0.3〜1.0重量%添加することが多い。又
原料中に不純物として含有されていたり、製造す
る際に工程の中で混入される場合もあり、これら
は不純物とみなされるが、いずれにしても、通常
の誘電体としては1.0重量%程度は許容されてい
る。そこで不純物量が非直線容量素子に及ぼす影
響を調査するため BaTiO3………92.0mol% BaZrO3………8.0mol% MnO………0.05重量%の組成物に Al2O3、B2O3、MgO、SiO2等の不純物を第8
図に示すように添加し、実施例1と同様にパルス
電圧を測定してみた。その結果を第8図及び第2
表(試料No.19、20)にまとめた。 第8図に示されるように不純物の量とパルス電
圧の関係には明瞭な相関が認められる。 特に不純物量が上記組成物100に対し0.15重量
%を越えるとパルス電圧の急激な低下が見られ
た。 第9図に示す写真によつても、それが裏付けら
れている。 すなわち、不純物(SiO2)が0.1〜0.15重量%
のものは結晶も良く成長し、粒界層の厚みも小さ
いが0.25重量%のものは粒界層が非常に厚くな
り、0.6重量%のものは結晶の成長がそれ以下の
ものに比べ極端に不良である。 その理由として、これら不純物はBaO−TiO2
−ZrO2系固溶体結晶の粒界に析出するためにそ
の量により粒界の発達と相関関係があると考えら
れる。 つまり、粒界は誘電率の低い残留分極の小さな
ヒステリシス特性を示さない常誘電体で構成され
ていると考えられ、粒界の成長したものは非直線
性誘電体素子としては不適当である。 又、BaTiO3の単結晶に於ても歪の残留してい
るものはヒステリシスが変形し、第1図Aのよう
な形態とはならないことは良く知られている。 しかるに粒界は結晶との物理的性質の相違によ
り、結晶に対し歪を与える要因となることは容易
に考えられ、ヒステリシスに悪い影響を与えるも
のと考えられる。 このような粒界は出来るだけ発達しない方がパ
ルス電圧が高くなることは、第9図の写真および
第8図のデータからも明確となつた。 更にこのような不純物が多量に入ると結晶の発
達を抑える抑制剤として働くこともわかつてお
り、第9図の写真でも不純物が0.6重量%のもの
は結晶が小さく、このことを裏付けしている。 本発明の素子はBaO−TiO2−ZrO2系結晶のも
つ性質を引き出すものであるから、結晶の発達し
ない範囲ではパルス電圧が低いことも当然であろ
う。 更に、第10図に示すように不純物量別の自然
放置時間に対するパルス電圧の変化率を測定し
た。 その結果0.15重量%を超える不純物量では初期
のパルス電圧が低いのみでなく、自然放置時間に
対するパルス電圧の変化率が大きく実用的でない
ことが明らかとなつた。 以上のように不純物としては、0.15重量%以下
に限定するものであり、これは通常のコンデンサ
用誘電体磁器と異る大きな相違点と考えられるも
のである。 以上の様に、本発明の非直線性誘電体素子は第
2図に示すようなD−Eヒステリシス曲線の傾斜
が急しゅんで誘電率が高く、誘電体損失が小さ
く、パルス電圧が高いうえ、パルス電圧の経時変
化が小さく安定しているなど優れた特徴を有する
ものであり、非直線性誘電体素子として、従来全
くなかつた新規のものとして本発明によつて始め
て実用化が可能となつたものである。 したがつて非直線性誘電体素子として用いる前
述の放電灯・無接点起動装置のほかパルス発生器
等への用途に実用化が可能となり、今後この非直
線性を積極的に利用した用途開発も課題となつ
た。このように本発明による非直線性誘電体素子
の電子工業界における有用性は多大なるものがあ
る。
[Table] Example 3 In addition to the sticky additives used in Example 2, SiO 2 , Al 2 O 3 and the like are added in an amount of 0.3 to 1.0% by weight as sintering accelerators in a typical dielectric composition. Often added. In addition, they may be contained as impurities in the raw materials or mixed in during the manufacturing process, and these are considered impurities, but in any case, as a normal dielectric material, about 1.0% by weight is It is allowed. Therefore, in order to investigate the influence of the amount of impurities on the non-linear capacitance element, Al 2 O 3 and B 2 O were added to a composition containing BaTiO 3 92.0 mol% BaZrO 3 8.0 mol% MnO 0.05 wt%. 3 , impurities such as MgO, SiO 2 etc.
It was added as shown in the figure, and the pulse voltage was measured in the same manner as in Example 1. The results are shown in Figure 8 and 2.
The results are summarized in the table (Sample Nos. 19 and 20). As shown in FIG. 8, there is a clear correlation between the amount of impurities and the pulse voltage. In particular, when the amount of impurities exceeded 0.15% by weight based on 100% of the above composition, a rapid decrease in pulse voltage was observed. This is also supported by the photograph shown in Figure 9. That is, the impurity (SiO 2 ) is 0.1 to 0.15% by weight.
With 0.25% by weight, the grain boundary layer becomes very thick, and with 0.6% by weight, the crystal growth is extreme compared to those with less than 0.25% by weight. It is defective. The reason is that these impurities are BaO−TiO 2
-ZrO precipitates at the grain boundaries of 2 -based solid solution crystals, so it is thought that there is a correlation with the development of grain boundaries depending on the amount. In other words, the grain boundaries are considered to be composed of a paraelectric material with a low dielectric constant and small residual polarization that does not exhibit small hysteresis characteristics, and those with grown grain boundaries are unsuitable for use as a nonlinear dielectric element. Furthermore, it is well known that even in single crystals of BaTiO 3 where strain remains, the hysteresis is deformed and the crystal does not take the form shown in FIG. 1A. However, due to the difference in physical properties between grain boundaries and crystals, it is easy to think that grain boundaries become a factor that imparts strain to crystals, and are thought to have a negative effect on hysteresis. It became clear from the photograph in FIG. 9 and the data in FIG. 8 that the pulse voltage would be higher if such grain boundaries were not developed as much as possible. Furthermore, it is known that when such impurities are present in large quantities, they act as inhibitors that suppress the growth of crystals, and the photograph in Figure 9 shows that the crystals are small when the impurities are 0.6% by weight, supporting this fact. . Since the device of the present invention brings out the properties of BaO- TiO2 - ZrO2 -based crystals, it is natural that the pulse voltage is low in the range where the crystals do not develop. Furthermore, as shown in FIG. 10, the rate of change in pulse voltage with respect to the natural standing time for each impurity amount was measured. As a result, it became clear that when the amount of impurities exceeds 0.15% by weight, not only the initial pulse voltage is low, but also the rate of change of the pulse voltage with respect to the natural standing time is large, making it impractical. As mentioned above, the impurities are limited to 0.15% by weight or less, and this is considered to be a major difference from ordinary dielectric ceramics for capacitors. As described above, the nonlinear dielectric element of the present invention has a steep DE hysteresis curve as shown in FIG. 2, a high dielectric constant, a small dielectric loss, a high pulse voltage, and It has excellent characteristics such as small and stable changes in pulse voltage over time, and the present invention has made it possible to put it into practical use for the first time as a new nonlinear dielectric element that has never existed before. It is something. Therefore, in addition to the aforementioned discharge lamps and non-contact starting devices that are used as nonlinear dielectric elements, it can be put to practical use in pulse generators, etc. In the future, applications that actively utilize this nonlinearity will be developed. It became an issue. As described above, the nonlinear dielectric element according to the present invention has great utility in the electronic industry.

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

第1図A,Bは従来例に係るもので同図Aは
BaTiO3単結晶体のD−Eヒステリシス曲線例
図、同図BはBaTiO3多結晶体のD−Eヒステリ
シス曲線例図である。第2図は本発明の実施例に
係る非直線性誘電体素子のD−Eヒステリシス曲
線例図であり、第3図はこの素子を用いた放電
灯・無接点起動装置の回路図である。第4図、第
5図はそれぞれ第3図に示す回路の動作原理を示
す回路図、動作波形図である。第6図〜第10図
は本発明の実施例に係るもので、第6図は
BaTiO3多結晶体のBaO−TiO2−ZrO2系組成比
別のパルス電圧の温度特性を示すグラフである。
第7図は添加物の種類、量とパルス電圧の関係を
示すグラフである。第8図は不純物の種類、量と
パルス電圧の関係を示すグラフである。第9図は
不純物(SiO2)の量と結晶体の結晶の構造の関
係を示す顕微鏡写真である。第10図は不純物量
別の、自然放置時間に対するパルス電圧の変化を
示すグラフである。
Figure 1 A and B are related to the conventional example, and Figure A is
An example of a D-E hysteresis curve of a BaTiO 3 single crystal, and B of the same figure is an example of a D-E hysteresis curve of a BaTiO 3 polycrystal. FIG. 2 is an example of a DE hysteresis curve of a nonlinear dielectric element according to an embodiment of the present invention, and FIG. 3 is a circuit diagram of a discharge lamp/non-contact starting device using this element. 4 and 5 are a circuit diagram and an operation waveform diagram showing the operating principle of the circuit shown in FIG. 3, respectively. Figures 6 to 10 relate to embodiments of the present invention, and Figure 6 is
It is a graph showing the temperature characteristics of the pulse voltage according to the BaO- TiO2 - ZrO2 system composition ratio of the BaTiO3 polycrystalline body.
FIG. 7 is a graph showing the relationship between the type and amount of additives and pulse voltage. FIG. 8 is a graph showing the relationship between the type and amount of impurities and pulse voltage. FIG. 9 is a micrograph showing the relationship between the amount of impurity (SiO 2 ) and the crystal structure of the crystal. FIG. 10 is a graph showing changes in pulse voltage with respect to natural standing time for each impurity amount.

Claims (1)

【特許請求の範囲】 1 BaO−TiO2−ZrO2を主成分とし、酸化物に
換算してBaO63.39〜65.62重量%、TiO226.42〜
33.85重量%、ZrO20.53〜10.19重量%の範囲から
なる基本組成物100に対しMn、Crの酸化物、炭
酸塩の少なくとも一種を合計0.01〜0.40重量%含
有し、その他の不純物、添加物となる酸化物の量
を0.15重量%以下としたことを特徴とする非直線
性誘電体素子。 2 パルス発生器、放電燈、点燈装置等の非直線
性誘電体素子とすることを特徴とする特許請求の
範囲第1項記載の非直線性誘電体素子。
[Scope of Claims] 1 BaO-TiO 2 -ZrO 2 as the main component, BaO 63.39 to 65.62% by weight and TiO 2 26.42 to 65.62% by weight in terms of oxides.
33.85% by weight, ZrO 2 in the range of 0.53 to 10.19% by weight, a total of 0.01 to 0.40% by weight of at least one of Mn and Cr oxides and carbonates, and other impurities and additives. A nonlinear dielectric element characterized in that the amount of oxide is 0.15% by weight or less. 2. The nonlinear dielectric element according to claim 1, which is used as a nonlinear dielectric element for a pulse generator, a discharge lamp, a lighting device, etc.
JP56015968A 1981-02-05 1981-02-05 Nonlinear dielectric element Granted JPS57130302A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56015968A JPS57130302A (en) 1981-02-05 1981-02-05 Nonlinear dielectric element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56015968A JPS57130302A (en) 1981-02-05 1981-02-05 Nonlinear dielectric element

Publications (2)

Publication Number Publication Date
JPS57130302A JPS57130302A (en) 1982-08-12
JPS6312324B2 true JPS6312324B2 (en) 1988-03-18

Family

ID=11903507

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56015968A Granted JPS57130302A (en) 1981-02-05 1981-02-05 Nonlinear dielectric element

Country Status (1)

Country Link
JP (1) JPS57130302A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103408298B (en) * 2013-08-05 2015-12-23 无锡鑫圣慧龙纳米陶瓷技术有限公司 One is applicable to low sintering microwave dielectric ceramic materials and preparation method thereof

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5556621A (en) * 1978-10-20 1980-04-25 Tdk Electronics Co Ltd Nonnlinear dielectric element

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5556621A (en) * 1978-10-20 1980-04-25 Tdk Electronics Co Ltd Nonnlinear dielectric element

Also Published As

Publication number Publication date
JPS57130302A (en) 1982-08-12

Similar Documents

Publication Publication Date Title
US4447549A (en) Non-linear dielectric element
JPS637012B2 (en)
Ho et al. Effects of zirconium on the structural and dielectric properties of (Ba, Sr) TiO 3 solid solution
JPH11100263A (en) Dielectric ceramic composition
US4404029A (en) Non-linear polycrystalline barium titanate-type dielectric element
JPS6312324B2 (en)
US3676351A (en) Ceramic dielectric comprising calcium titanosilicate
Syamaprasad et al. Capacitor ceramics in pure and doped Ba0. 71Sr0. 29TiO3
Shen et al. Reduced high temperature dielectric loss in BSB glass modified Ba 0.3 Sr 0.7 TiO 3 ceramics for energy storage
JPS6051207B2 (en) High dielectric constant porcelain composition
JP2696118B2 (en) Manufacturing method of nonlinear dielectric element
Wang et al. The effect of dysprosium on the microstructure and dielectric properties of (Ba/sub 1-x/Sr/sub x/) TiO/sub 3/ceramics
JPH0440853B2 (en)
JPS6230682B2 (en)
JP2694209B2 (en) High dielectric constant porcelain composition
JP2643197B2 (en) Dielectric porcelain composition
KR940004381B1 (en) Composition of ceramic dielectric substance
JPS6230483B2 (en)
JPH05213666A (en) Dielectric porcelain composition and its production
JPH10167814A (en) Dielectric ceramic composition
JPS5919442B2 (en) Semiconductor ceramic material and its manufacturing method
JPH0132647B2 (en)
Chen et al. Energy-storage performance of PbO-B^ sub 2^ O3-SiO2 added (Pb^ sub 0.92^ Ba^ sub 0.05^ La^ sub 0.02^)(Zr^ sub 0.68^ Sn^ sub 0.27^ Ti^ sub 0.05^) O3 antiferroelectric ceramics prepared by microwave sintering method
JPS58188122A (en) Nonlinear ceramic condenser
WO1983003028A1 (en) Voltage sensitive current limiting element