JPH02178902A - Voltage dependent nonlinear resistance element - Google Patents

Voltage dependent nonlinear resistance element

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Publication number
JPH02178902A
JPH02178902A JP63332830A JP33283088A JPH02178902A JP H02178902 A JPH02178902 A JP H02178902A JP 63332830 A JP63332830 A JP 63332830A JP 33283088 A JP33283088 A JP 33283088A JP H02178902 A JPH02178902 A JP H02178902A
Authority
JP
Japan
Prior art keywords
zno
sintered body
voltage
varistor
resistance element
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.)
Pending
Application number
JP63332830A
Other languages
Japanese (ja)
Inventor
Koichi Tsuda
孝一 津田
Kazuo Koe
向江 和郎
Toyoshige Sakaguchi
豊重 坂口
Takashi Ishii
石井 孝志
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP63332830A priority Critical patent/JPH02178902A/en
Publication of JPH02178902A publication Critical patent/JPH02178902A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To extinguish shottky barrier between a sintered substance and a metallic electrode so as to make it excellent in mechanical strength and surge resistance by providing a contact layer, consisting of a specific zinc oxide, between the sintered substance and the metallic electrode. CONSTITUTION:Proper amounts of Pr, Co, B, etc., in the form of compounds such as oxides, etc., are added to ZnO powder, and then are mixed and granulated so as to make up granulated powder for ZnO varistor, and this granulated powder is formed into disc shape. Next, solution, wherein nitric acid indium In(No3).-9H2O is dissolved in acetylacetone, is applied on opposing both main faces of a sintered substance 3 which is made by firing, and is heat-treated after drying so as to disperse In into a ZnO sintered substance. Since the contact layers 2A and 2B, wherein In is introduced into zinc oxides, are low resistant layers, schottky barrier between the zinc oxides and the metallic electrodes 1A and 1B disappears, and mechanical strength and surge resistance become favorable.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 この発明は酸化亜鉛を主成分とする低電圧回路用電圧非
直線抵抗素子に係り、特に酸化亜鉛焼結体と金属電極間
の接触層に関する。
[Detailed Description of the Invention] [Field of Industrial Application] This invention relates to a voltage nonlinear resistance element for low voltage circuits containing zinc oxide as a main component, and particularly relates to a contact layer between a zinc oxide sintered body and a metal electrode. .

〔従来の技術〕[Conventional technology]

ZnOを主成分としこれに微量の添加物を加えて混合し
た後焼結して作られるセラミックスは、優れた電圧非直
線性を示すことが知られており、電気回路における異常
電圧(サージ)を制御するためのバリスタとして広く実
用に供されている。このようなバリスタは第3図に示す
工程に従って製造される。
Ceramics, which are made by mixing ZnO with a small amount of additives and sintering it as a main component, are known to exhibit excellent voltage nonlinearity, and are useful for suppressing abnormal voltages (surges) in electrical circuits. It is widely used as a varistor for control purposes. Such a varistor is manufactured according to the steps shown in FIG.

ZnOバリスタの電圧非直線性は、ZnO結晶粒の粒界
に形成される二重ショットキー障壁に起因するものであ
る。実用的なバリスタにおいては、ZnO結晶粒が結合
して形成される粒界1層当たりのバリスタ電圧は結晶粒
径の大きさにかかわらずほぼ一定であり、その値は2■
程度である。 (バリスタ電圧とは、バリスタに1mA
の電流を流したときの端子間電圧で、通常■1□で表わ
される。)したがって、電圧非直線抵抗素子のバリスタ
電圧はZnO焼結体の対向する面上に設けられた電極間
に存在する粒界層の数によって決定される。
The voltage nonlinearity of ZnO varistors is due to double Schottky barriers formed at grain boundaries of ZnO crystal grains. In a practical varistor, the varistor voltage per grain boundary layer formed by the combination of ZnO crystal grains is almost constant regardless of the crystal grain size, and its value is 2
That's about it. (Varistor voltage is 1mA to the varistor.
It is the voltage between the terminals when a current of ) Therefore, the varistor voltage of the voltage non-linear resistance element is determined by the number of grain boundary layers existing between the electrodes provided on the opposing surfaces of the ZnO sintered body.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

ところで、ZnOバリスタの電極には、銀、アルミニウ
ムが用いられるが、避雷器用のZnO素子以外は銀ペー
ストを焼付けてこれを電極とするのが一般的である。こ
の場合銀電極とZnO焼結体界面にシロットキー障壁が
形成され1mAの電流をながしたときに電極/ZnO焼
結体界面のショットキー障壁により約3vの電圧が発生
する。したがって、この電極/ZnO焼結体界面障壁は
バリスタ電圧が低くなるほど、無視できなくなってくる
By the way, silver and aluminum are used for the electrodes of ZnO varistors, and except for ZnO elements for lightning arresters, it is common to bake silver paste and use this as the electrode. In this case, a Schottky barrier is formed at the interface between the silver electrode and the ZnO sintered body, and when a current of 1 mA is passed, a voltage of about 3 V is generated due to the Schottky barrier at the electrode/ZnO sintered body interface. Therefore, this electrode/ZnO sintered body interface barrier becomes impossible to ignore as the varistor voltage becomes lower.

例えばDC12V回路にZnOバリスタを適用する場合
、回路電圧の変動などを考慮してバリスタ電圧は一般に
22Vのものが使用されるが、前述のように粒界1層当
たりのバリスタ電圧は約2vであるからこの素子の対向
する電極間に11層の粒界が存在することになる。とこ
ろが上述の電極/ZnO焼結体界面障壁のため、ZnO
焼結体の粒界が有するバリスタ電圧と電極/焼結体界面
が有するバリスタ電圧の合計を22Vとしなければなら
ない。このため実際にはバリスタ電圧が低くなるにつれ
て、焼結体の数から求められるバリスタ電圧と実測した
バリスタ電圧間の差が大きくなるので焼結体の粒界の数
を減らさなければならない。このために焼結体厚さを減
らすと(1)焼結体の機械的強度が低下する(2)雷サ
ージ、開閉サージなどのサージエネルギの吸収能力 (
サージ耐量)は焼結体の体積に比例するのでサージ耐量
特性が低下するなどの問題があった。
For example, when applying a ZnO varistor to a DC 12V circuit, a varistor voltage of 22V is generally used in consideration of circuit voltage fluctuations, but as mentioned above, the varistor voltage per grain boundary layer is approximately 2V. Therefore, 11 layers of grain boundaries exist between the opposing electrodes of this element. However, due to the barrier at the electrode/ZnO sintered body interface mentioned above, ZnO
The sum of the varistor voltage at the grain boundaries of the sintered body and the varistor voltage at the electrode/sintered body interface must be 22V. Therefore, in reality, as the varistor voltage decreases, the difference between the varistor voltage determined from the number of sintered bodies and the actually measured varistor voltage increases, so the number of grain boundaries in the sintered body must be reduced. For this reason, if the thickness of the sintered body is reduced, (1) the mechanical strength of the sintered body will decrease (2) the ability to absorb surge energy such as lightning surges and switching surges (
Since the surge resistance (surge resistance) is proportional to the volume of the sintered body, there were problems such as a decrease in surge resistance characteristics.

また、電極/焼結体界面のショットキー障壁は、ZnO
焼結体自身の粒界に存在するショットキー障壁に比ベサ
ージ耐量が低いので、バリスタ電圧が低くなるほどサー
ジによるバリスタ電圧の変化量が大きくなるという欠点
があり、さらに電極/焼結体界面に形成されるショット
キー障壁は、組立て工程例えばハンダ付工程、樹脂モー
ルド工程で変動しやすくバリスタ電圧の工程管理が困難
になるという問題があった。
In addition, the Schottky barrier at the electrode/sintered body interface is
The Schottky barrier existing at the grain boundaries of the sintered body itself has a low relative Vesage resistance, so the lower the varistor voltage is, the greater the change in varistor voltage due to surges becomes. The problem with the Schottky barrier is that it tends to fluctuate during the assembly process, such as the soldering process and the resin molding process, making process control of the varistor voltage difficult.

この発明は上述の点に鑑みてなされたものでその目的は
焼結体と金属電極間のショットキバリアをなくすことに
より、機械的強度、サージ耐量に優れ、工程管理も容易
な低電圧用電圧非直線抵抗素子を提供することにある。
This invention was made in view of the above points, and its purpose is to eliminate the Schottky barrier between the sintered body and the metal electrode, thereby providing a low-voltage non-conductor with excellent mechanical strength and surge resistance, and easy process control. An object of the present invention is to provide a linear resistance element.

〔課題を解決するための手段〕[Means to solve the problem]

上述の目的はこの発明によれば、酸化亜鉛の粉末と電圧
非直線性を生じさせる微量の添加物粉末とを混合し焼成
した焼結体に金属電極を配してなる電圧非直線抵抗素子
において、In、 八/、 Gaの少なくとも1つの元
素を含む酸化亜鉛からなりかつ前記焼結体と金属電極と
の間に設けられた接触層を備えることにより達成される
According to the present invention, the above-mentioned object is achieved in a voltage nonlinear resistance element comprising a metal electrode arranged on a sintered body made by mixing zinc oxide powder and a small amount of additive powder that causes voltage nonlinearity. This is achieved by providing a contact layer made of zinc oxide containing at least one element of , In, 8/, Ga and provided between the sintered body and the metal electrode.

接触層はIn、 ki、 Gaの熱拡散、イオンインプ
ランテーションにより焼結体に直接的に形成する他、ス
パッタ法やIn、 AI、 Gaを含む酸化亜鉛を塗布
する方法等によって形成することができる。
The contact layer can be formed directly on the sintered body by thermal diffusion of In, Ki, Ga or ion implantation, or can be formed by a sputtering method or a method of coating zinc oxide containing In, AI, or Ga. .

〔作用〕[Effect]

酸化亜鉛にJn、 A/、 Gaをを導入した接触層は
低抵抗層であるので、酸化亜鉛と金属電極間のショット
キバリアが消滅する。
Since the contact layer in which Jn, A/, and Ga are introduced into zinc oxide is a low resistance layer, the Schottky barrier between the zinc oxide and the metal electrode disappears.

〔実施例〕〔Example〕

次に本発明の実施例を図面に基づいて説明する。 Next, embodiments of the present invention will be described based on the drawings.

第2図にこの発明の実施例に係る抵抗素子の製造工程が
示される。まずZnO粉末にPr、 Co、 Eなどを
酸化物などの化合物の形で適量添加したあと混合、造粒
しZnOバリスタ用造粒粉が調製される。
FIG. 2 shows the manufacturing process of a resistance element according to an embodiment of the present invention. First, appropriate amounts of Pr, Co, E, etc. in the form of compounds such as oxides are added to ZnO powder, and then mixed and granulated to prepare granulated powder for ZnO varistors.

この造粒粉を直径17寵の金型を使用して厚さ]、25
nの円板状に成形する。次いでこの成形体を酸化性雰囲
気中において1350℃の温度で4h焼成する。得られ
た焼結体の大きさは直径14鶴、厚さ1.0額であった
This granulated powder was molded using a mold with a diameter of 17 mm to a thickness of 25 mm.
Shape into n disc shape. Next, this molded body is fired at a temperature of 1350° C. for 4 hours in an oxidizing atmosphere. The size of the obtained sintered body was 14 mm in diameter and 1.0 mm in thickness.

上記のようにして作られた焼結体の対向する両生面上に
硝酸インジウムIn(NO3)  ・9H,0をアセチ
ルアセトンに溶解した溶液を塗布し乾燥後700℃で4
h熱処理し、InをZnO焼結体中に拡散させた。In
を拡散させた面の表面抵抗は1mAの電流を流した時に
IKΩ以下であった。Inを拡散させない時には20に
Ω以上である。
A solution of indium nitrate (In(NO3) 9H,0) dissolved in acetylacetone was applied onto the opposing surfaces of the sintered body produced as described above, and after drying, it was heated at 700℃ for 4 hours.
h heat treatment was performed to diffuse In into the ZnO sintered body. In
The surface resistance of the surface on which it was diffused was less than IKΩ when a current of 1 mA was applied. When In is not diffused, the resistance is 20Ω or more.

上記処理をした焼結体に銀ペーストを塗布後焼付けてバ
リスタを構成した。第1図に模式断面図が示される。続
いてバリスタ特性を測定した。さらに組立後のバリスタ
特性も評価した。結果が第1表に示される。
A varistor was constructed by applying silver paste to the sintered body treated as described above and then baking it. A schematic cross-sectional view is shown in FIG. Subsequently, the varistor characteristics were measured. We also evaluated the varistor characteristics after assembly. The results are shown in Table 1.

第1表 るサージ耐量(A)を示しである。ただしサージ耐量は
8720μS標準電流パルスを素子に2分間隔で2回流
した後のVIffiAの変化率が±10%となる電流で
規定した。
The first table shows the surge resistance (A). However, the surge resistance was defined as the current at which the rate of change in VIffiA was ±10% after a standard current pulse of 8720 μS was passed through the device twice at 2-minute intervals.

第2表 第1表にはV I+nA + V ImAの変動係数、
電流100pA〜1mA領域における電圧非直線係数α
を、電極づけ後1組立後について従来法と比較して示し
た。さらに参考データとしてZnO焼結体とショットキ
ー障壁を形成しないIn−Ga電極を用いたときの特性
も併せて示した。この結果から本発明の方法によると電
極づけ後と組立て後の特性変動はなく、従来法に比べ優
れていることがわかる。
Table 2 Table 1 shows the coefficient of variation of V I+nA + V ImA,
Voltage nonlinear coefficient α in the current 100 pA to 1 mA region
This is shown in comparison with the conventional method after one assembly after electrode attachment. Further, as reference data, characteristics when using a ZnO sintered body and an In-Ga electrode that does not form a Schottky barrier are also shown. From these results, it can be seen that the method of the present invention has no characteristic variation after electrode attachment and after assembly, and is superior to the conventional method.

第2表はサージを加えたときの組立て後におけ第2表か
ら明らかなように、本発明方法の方が優れていることが
わかる。この理由は次のように考えられる。即ち、焼結
体そのもののサージ耐量は1200OAであるが、従来
の素子では電極/焼結体界面に形成される障壁がサージ
により変化しやすいためVlmAが20V素子の場合、
電極/焼結体界面障壁が2V変化すると10%の変化と
なるからである。このようにバリスタ電圧が低くなれば
なるほど従来方法で作製されたZnOバリスタ素子のサ
ージ耐量は見掛は上低くなるという欠点が解消される。
As is clear from Table 2, the method of the present invention is superior after assembly when a surge is applied. The reason for this is thought to be as follows. That is, the surge withstand capacity of the sintered body itself is 1200OA, but in the case of an element with VlmA of 20V, since the barrier formed at the electrode/sintered body interface in conventional elements is easily changed by surges,
This is because a 2V change in the electrode/sintered body interface barrier results in a 10% change. In this way, the disadvantage that the lower the varistor voltage is, the lower the surge resistance of the ZnO varistor element manufactured by the conventional method appears to be is solved.

なお、上述した実施例ではInを塗布、拡散する方法に
ついて述べたが、同様な効果はAI、Ga元素でも確認
された。また実施例では円板状焼結体について示したが
本発明の効果は形状によらず、また対向する電極の場合
のみならず二つの電極を同一平面上に設けたときにも確
かめられる。
Although the above-mentioned embodiments described a method of coating and diffusing In, similar effects were also confirmed with Al and Ga elements. Further, although the embodiments have been described with respect to a disk-shaped sintered body, the effects of the present invention are not dependent on the shape, and can be confirmed not only when the electrodes are opposed to each other but also when two electrodes are provided on the same plane.

In、 AI、 Gaの濃度はZnOのZnに対し10
0原子ppm以上あればよい。また接触層の厚さは10
00Å以上あればよい。
The concentrations of In, AI, and Ga are 10% compared to Zn in ZnO.
It is sufficient if it is 0 atomic ppm or more. Also, the thickness of the contact layer is 10
It is sufficient if the thickness is 00 Å or more.

〔発明の効果〕〔Effect of the invention〕

この発明によれば酸化亜鉛の粉末と電圧非直線性を生じ
させる微量の添加物粉末とを混合し焼成した焼結体に金
属電極を配してなる電圧非直線抵抗素子において、In
、 kl、 Gaの少なくとも1つの元素を含む酸化亜
鉛からなり前記焼結体と金属電極との間に設けられた接
触層を備えるので低い抵抗の接触層が焼結体と金属電極
の間に介在しその結果焼結体と金属電極との間のショッ
トキバリアが消滅して機械的強度とサージ耐量に優れか
つ製造上の工程管理の容易な電圧非直線抵抗素子が得ら
れる。
According to this invention, in a voltage nonlinear resistance element in which metal electrodes are arranged on a sintered body made by mixing zinc oxide powder and a small amount of additive powder that causes voltage nonlinearity,
, kl, and a contact layer made of zinc oxide containing at least one element of Ga and provided between the sintered body and the metal electrode, so that a low resistance contact layer is interposed between the sintered body and the metal electrode. As a result, the Schottky barrier between the sintered body and the metal electrode disappears, and a voltage nonlinear resistance element with excellent mechanical strength and surge resistance and easy manufacturing process control is obtained.

【図面の簡単な説明】 第1図はこの発明の実施例に係る電圧非直線抵抗素子を
示す模式断面図、第2図はこの発明の実施例に係る抵抗
素子の製造工程を示す流れ図、第3図は従来の素子の製
造工程を示す流れ図である。 IA、 IB:金属電極、録、2B:接触層、3:焼結
第 ■
[BRIEF DESCRIPTION OF THE DRAWINGS] FIG. 1 is a schematic sectional view showing a voltage nonlinear resistance element according to an embodiment of the present invention, and FIG. 2 is a flowchart showing the manufacturing process of a resistance element according to an embodiment of the invention. FIG. 3 is a flowchart showing a conventional device manufacturing process. IA, IB: metal electrode, record, 2B: contact layer, 3: sintered part ■

Claims (1)

【特許請求の範囲】[Claims] 1)酸化亜鉛の粉末と電圧非直線性を生じさせる微量の
添加物粉末とを混合し焼成した焼結体に金属電極を配し
てなる電圧非直線抵抗素子において、In,Al,Ga
の少なくとも1つの元素を含む酸化亜鉛からなりかつ前
記焼結体と金属電極との間に設けられた接触層を備える
ことを特徴とする電圧非直線抵抗素子。
1) In a voltage nonlinear resistance element in which metal electrodes are arranged on a sintered body made by mixing zinc oxide powder and a small amount of additive powder that causes voltage nonlinearity, In, Al, Ga
A voltage nonlinear resistance element comprising a contact layer made of zinc oxide containing at least one element and provided between the sintered body and a metal electrode.
JP63332830A 1988-12-29 1988-12-29 Voltage dependent nonlinear resistance element Pending JPH02178902A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63332830A JPH02178902A (en) 1988-12-29 1988-12-29 Voltage dependent nonlinear resistance element

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63332830A JPH02178902A (en) 1988-12-29 1988-12-29 Voltage dependent nonlinear resistance element

Publications (1)

Publication Number Publication Date
JPH02178902A true JPH02178902A (en) 1990-07-11

Family

ID=18259277

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63332830A Pending JPH02178902A (en) 1988-12-29 1988-12-29 Voltage dependent nonlinear resistance element

Country Status (1)

Country Link
JP (1) JPH02178902A (en)

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