JPH0343985A - Thin high temperature heater and manufacture thereof - Google Patents
Thin high temperature heater and manufacture thereofInfo
- Publication number
- JPH0343985A JPH0343985A JP1181016A JP18101689A JPH0343985A JP H0343985 A JPH0343985 A JP H0343985A JP 1181016 A JP1181016 A JP 1181016A JP 18101689 A JP18101689 A JP 18101689A JP H0343985 A JPH0343985 A JP H0343985A
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- JP
- Japan
- Prior art keywords
- layer
- heater
- insulating member
- resistor
- resistor layer
- 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.)
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- Non-Adjustable Resistors (AREA)
- Surface Heating Bodies (AREA)
- Solid Thermionic Cathode (AREA)
- Apparatuses And Processes For Manufacturing Resistors (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
この発明は、高温加熱用小型ヒータあるいは電子銃用ヒ
ータのように使用温度が1000’C程度の薄型高温用
ヒータの構造および製造方法に関する。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to the structure and manufacturing method of a thin high-temperature heater whose operating temperature is about 1000'C, such as a small heater for high-temperature heating or a heater for an electron gun.
[従来の技術]
従来、平板型ヒータは例えば、特公昭55−24646
号公報に記載されているように、スクリーン印刷等のい
わゆる厚膜回路形成技術を用いて製造されていた。第3
図はこのようにして製造された従来のヒータを利用した
電子管カソード装置を示す断面構成図である。図におい
て、〈10)は七うミンクス基板、(11)は発熱体層
、(12〉は絶縁層、<13)はカソード利層、(14
)はカソードリード層、〈15)はベースメタル層であ
る。[Prior Art] Conventionally, flat plate heaters have been disclosed in Japanese Patent Publication No. 55-24646, for example.
As described in the publication, the circuit was manufactured using a so-called thick film circuit forming technique such as screen printing. Third
The figure is a cross-sectional configuration diagram showing an electron tube cathode device using a conventional heater manufactured in this manner. In the figure, <10) is the seventh minx substrate, (11) is the heating element layer, (12> is the insulating layer, <13) is the cathode layer, and (14) is the insulating layer.
) is a cathode lead layer, and <15) is a base metal layer.
次に製造方法について説明する。まず、七うミンクス基
板<10>を構成する原材料を用意し、ロール間を通す
押し出し法、あるいはキャスティング法の印刷技術によ
ってシート上に所望のパターン形状の発熱体層(11)
を形成する。この発熱体層(11)はヒータ剤に焼成助
剤を添加したペーストを基板(10)上にスクリーン印
刷して形成される。スクリーン印刷後、高温(1000
〜2000’C)で焼成処理され、平板型ヒータが形成
される。Next, the manufacturing method will be explained. First, raw materials constituting the Seven Minx substrate <10> are prepared, and a heating element layer (11) is formed in a desired pattern on a sheet by extrusion or casting printing technology by passing between rolls.
form. This heating element layer (11) is formed by screen printing a paste containing a heating agent and a baking aid on the substrate (10). After screen printing, high temperature (1000
-2000'C) to form a flat plate heater.
この方法では、製造時に高温処理過程か入るのでヒータ
をこの処理温度以下で使用する場合、抵抗の経時変化が
小さい等のヒータとしての高温長期安定性が期待されて
いた。しかし、スクリーン印刷によって得られるパター
ン精度は低く、しかも発熱体(11)の厚さ制御(薄型
化)が困難にため、消費電力が大きく、しかも複数のヒ
ータ間では抵抗のばらつきが大きかった。そのため、精
度良くパターンの形成ができる手法としてPVDやCV
Dによる成膜法の開発が進められていた。In this method, a high-temperature treatment process is involved during manufacturing, so when the heater is used at a temperature below this treatment temperature, high-temperature long-term stability as a heater, such as a small change in resistance over time, was expected. However, the pattern accuracy obtained by screen printing is low, and it is difficult to control the thickness (thinning) of the heating element (11), resulting in high power consumption and large variations in resistance among multiple heaters. Therefore, PVD and CV are methods that can form patterns with high precision.
Development of a film forming method using D was in progress.
第4図に薄膜形成法による従来の平板薄型ヒータの製造
方法を示す。平滑たセラミックス基板(絶縁部材)〈l
)上にヒータ用の抵抗体膜(3)(通常はWのような金
属が用いられる)を−様に形成し、次にエツチングによ
り所望のヒータパターンを形成しこれにリード線(図示
せず)を接合するという手法で平板薄型ヒータを実現し
ていた。FIG. 4 shows a conventional method for manufacturing a thin flat heater using a thin film forming method. Smooth ceramic substrate (insulating member)
), a resistor film (3) for the heater (usually made of a metal such as W) is formed in the shape of -, then a desired heater pattern is formed by etching, and a lead wire (not shown) is formed on this. ) was used to create a thin flat heater.
[発明が解決しようとする課題]
以上のような成膜法を用いて平板薄型ヒータを製造する
場合、ヒータ用の抵抗体膜り3)と絶縁部材(1)との
密着力が小さいことが非常に問題となっていた。そのた
め、ヒータ用の抵抗体膜り3)と絶縁部材(1)との密
着力を高めるために密着層を挿入する手法が取られてい
た。通常この密着層として数10〜数1100nのTi
膜を設け、そのうえに抵抗体膜を形成することによ()
薄型高温ヒータを実現していた。しかし、 リード線に
電圧を印加しヒータとして使用している間に、即ち10
00°Cという高温負荷の間にTiが高温劣化を起こし
てしてしまいヒータが断線してしまう等の問題か生して
いた。参考図面に断線状態のSEM写真を示す。 〈な
お、写真中、20.0KVは走査電子顕微鏡の加速電圧
、×350は倍$350倍、100μmはその直上の線
の長さが100μmに相当することを表す。)この原因
はTiには882°Cにα−βの変態点く以下変態点と
略す)があり、ヒータを使用することによりこの変態点
を繰り返し通過するためと考えられる。また、通常、薄
膜抵抗体は使用中に抵抗の変化が生じる。第5図に抵抗
値の経時変化を示す。初期に抵抗が低下するのは、薄膜
の再結晶化が進み、膜中の結晶粒が粗大化するためであ
る。例えば抵抗体く発熱体)を密着層を持たないW(タ
ングステン)で形成シ、これを1ooo’cで使用した
場合、1000°CはWの再結晶温度に相当するため、
再結晶化は進む。次に時間経過に従って抵抗が増加する
のは使用中の雰囲気により膜中に不純物が混入する、あ
るいは酸化することに起因する。そのため、従来の薄膜
法による薄型高温ヒータはヒータとしては不安定で、し
かも長期信頼性に欠けるものであった。[Problems to be Solved by the Invention] When manufacturing a flat thin heater using the above-described film formation method, there is a problem that the adhesion between the resistor film 3) for the heater and the insulating member (1) is small. It was a huge problem. Therefore, in order to increase the adhesion between the heater resistor film 3) and the insulating member (1), a method has been adopted in which an adhesion layer is inserted. Usually, this adhesion layer consists of several tens to several 1100 nanometers of Ti.
By providing a film and forming a resistor film on it ()
A thin, high-temperature heater was realized. However, while applying voltage to the lead wire and using it as a heater,
During a high temperature load of 00°C, Ti deteriorates at high temperatures, causing problems such as heater breakage. The reference drawing shows an SEM photograph of the disconnected state. (In the photo, 20.0 KV means the accelerating voltage of the scanning electron microscope, x350 means 350 times as much, and 100 μm means that the length of the line directly above it corresponds to 100 μm. ) The reason for this is thought to be that Ti has an α-β transformation point (hereinafter abbreviated as “transformation point”) at 882°C, and that this transformation point is repeatedly passed through by using a heater. Further, the resistance of thin film resistors usually changes during use. Figure 5 shows the change in resistance value over time. The reason why the resistance initially decreases is that recrystallization of the thin film progresses and the crystal grains in the film become coarser. For example, if a resistor (heating element) is formed of W (tungsten) without an adhesive layer and used at 100°C, 1000°C corresponds to the recrystallization temperature of W, so
Recrystallization progresses. Next, the reason why the resistance increases over time is due to impurities being mixed into the film or being oxidized due to the atmosphere during use. Therefore, thin high-temperature heaters based on the conventional thin film method are unstable as heaters and lack long-term reliability.
この発明は、上記のような問題点を解決するためになさ
れたもので、ヒータ用抵抗体膜と絶縁部材との密着力の
高い、使用時の抵抗変化の少ない、信頼性の高い薄型高
温ヒータを提供することを目的としている。This invention was made to solve the above-mentioned problems, and provides a highly reliable thin high-temperature heater that has high adhesion between the heater resistor film and the insulating member, and has little resistance change during use. is intended to provide.
[課題を解決するための手段]
この発明に係る薄型高温ヒータは、絶縁部材上に形成さ
れたTiよりなる密着層、およびこの密着層を介して上
記絶縁部材上に形成されたTi化合物よ+、)なる抵抗
体層を備えたものである。[Means for Solving the Problems] A thin high temperature heater according to the present invention includes an adhesion layer made of Ti formed on an insulating member, and a Ti compound formed on the insulating member via this adhesion layer. , ).
また、本発明の別の発明に係る薄型高温ヒータの製造方
法は、絶縁基板上にTiよりなる密着層およびTi化合
物よりなる抵抗体層を形成するのに、上記密着層および
抵抗体層共に上記Tiのα−βの変態点未満の温度で形
成するか、または上記密着層および抵抗体層共に上記変
態点以上の温度で形成するものである。Further, in the method for manufacturing a thin high-temperature heater according to another aspect of the present invention, in forming an adhesive layer made of Ti and a resistor layer made of a Ti compound on an insulating substrate, both the adhesive layer and the resistor layer are It is formed at a temperature below the α-β transformation point of Ti, or both the adhesive layer and the resistor layer are formed at a temperature above the transformation point.
[作用]
この発明においては、Ti膜は絶縁部材とヒータ用抵抗
体層の密着力の向上に作用し、抵抗体層であるTiC,
TiN、T1CNの単体もしくはその混合物等のTi化
合物はセラミックスであるため金属材によるヒータと比
べて高温安定性は優れている上に、ヒータ使用中に密着
層として余分なTi成分が抵抗体層へ拡散しても、抵抗
体層もTi成分を盆んでいるので悪影響を及ぼさず、密
着層は安定化される。[Function] In the present invention, the Ti film acts to improve the adhesion between the insulating member and the resistor layer for the heater, and the Ti film, which is the resistor layer,
Since Ti compounds such as TiN, T1CN alone or their mixtures are ceramics, they have superior high-temperature stability compared to heaters made of metal materials, and also act as an adhesion layer during use of the heater, allowing excess Ti components to be transferred to the resistor layer. Even if it diffuses, since the resistor layer also contains the Ti component, it will not have an adverse effect, and the adhesion layer will be stabilized.
また、本発明の別の発明においては、密着層および抵抗
体層の形成温度は共にTiの変態点より低いかまたは共
に高いため、ヒータを製造している間に、Tiの高温劣
化を起こす事もない。すなわち、共に変態点より低い場
合にはヒータ製造中にTiのα−β変態が起こらムいた
め、体積変化による劣化が発生しにくく、また、共に変
態点より高い場合には、密着層としては余分なTi成分
を製造中に拡散させてしまうので、その後、変態点以上
の温度で使用してもTiのα−β変態に伴う高温劣化を
生じることはない。Further, in another aspect of the present invention, since the formation temperatures of the adhesive layer and the resistor layer are both lower than or higher than the transformation point of Ti, high temperature deterioration of Ti is prevented during manufacturing of the heater. Nor. In other words, if both are lower than the transformation point, α-β transformation of Ti will not occur during heater manufacturing, so deterioration due to volume change will be less likely to occur, and if both are higher than the transformation point, there will be no need to Since the Ti component is diffused during manufacturing, high-temperature deterioration due to the α-β transformation of Ti does not occur even if it is subsequently used at a temperature higher than the transformation point.
[実施例]
以下にこの発明の一実施例について図に基づいて説明す
る。第1図はこの発明の一実施例による薄型高温ヒータ
を示す断面構成図である。図において、<1)は絶縁部
材、<2〉は絶縁部材<1)との密着層であるTi、(
3)は密着層(2〉を介して絶縁部材(1)の上に設け
られ例えばTiC,TiN。[Example] An example of the present invention will be described below based on the drawings. FIG. 1 is a sectional view showing a thin high temperature heater according to an embodiment of the present invention. In the figure, <1) is an insulating member, <2> is a Ti adhesion layer with the insulating member <1), (
3) is provided on the insulating member (1) via the adhesive layer (2>) and is made of, for example, TiC or TiN.
T1CNの単体もしくはその混合物等のTi化合物より
なる抵抗体層である。絶縁部材り1)に対しては、例え
ば、次のような要求を満たすことが望ましい。熱伝導性
が良く、熱膨張率が抵抗体層(3)のそれに近いこと、
長線縁体であること、高温で絶縁破壊しないこと、平滑
なこと。そのため、入手性から考えてAIN、Al2O
3等が考えられる。The resistor layer is made of a Ti compound such as T1CN alone or a mixture thereof. For example, it is desirable for the insulating member 1) to satisfy the following requirements. It has good thermal conductivity and a coefficient of thermal expansion close to that of the resistor layer (3);
It must be a long wire edge, not cause dielectric breakdown at high temperatures, and be smooth. Therefore, considering availability, AIN, Al2O
3rd prize is possible.
ここで、抵抗体層(3)をTiC,TiN、T1CNの
単体もしくはその混合物等のTi化合物で形成する理由
は、再結晶温度が高く、高温での電気的安定性が高いか
らである。例えばW、Mo等の一般的なヒータ材で形成
することも考えられる。Here, the reason why the resistor layer (3) is formed of a Ti compound such as TiC, TiN, T1CN alone or a mixture thereof is that the recrystallization temperature is high and the electrical stability at high temperatures is high. For example, it is conceivable to form it with a general heater material such as W or Mo.
しかし、こういった材料系は例えば絶縁部材(1)とし
てAl2O3基板を用いて形成し、1000″C程度の
高温で使用している際に基板(1)中の酸素を奪って(
還元して)蒸気圧の高い酸化物を形成して飛散していく
。即ち抵抗体層がエツチングされ、形状が変化してしま
う。そのため、ヒータとして安定に使用できる環境、例
えば基板〈1)材、雰囲気、温度が限定されてしまう。However, such material systems are formed using, for example, an Al2O3 substrate as the insulating member (1), and when used at a high temperature of about 1000"C, the oxygen in the substrate (1) is taken away (
(reduction) to form oxides with high vapor pressure and scatter. That is, the resistor layer is etched and its shape changes. Therefore, the environment in which it can be stably used as a heater, such as the substrate (1) material, atmosphere, and temperature, is limited.
以上の理由からである。This is for the reasons mentioned above.
ここでは絶縁部材<1)として単結晶サファイヤ基板(
A1203 )を選び、薄型高温ヒータを製造する例に
ついて2手法述べる。Here, a single crystal sapphire substrate (
A1203) will be selected and two methods will be described for an example of manufacturing a thin high-temperature heater.
まず第1の手法について例をあげて説明する。First, the first method will be explained by giving an example.
Al2O3基板上にスパッタ法により所望の厚さく数μ
m〜10/l□)のTi膜を一様に形成する。この時の
T1膜形成温度は例えば200〜300°Cである。そ
の後、所望のパターン形状に湿式あるいは乾式法でエツ
チングする。例えば湿式法であれば第2図に示すごく一
般的な工程でエツチングを行う。次に、パターンの形成
されたサンフルをイオン窒化用の真空炉内に設置し、T
iの変態点以下の温度、列えば400〜500 ’C;
でイオン窒化を施し、Ti表面からNを拡散させ、Ti
Nとする。窒化の深さは数71 m〜10ノzm程度に
達し、基板との界面でTiとAl2O3の密着に寄与す
る層まで(10nm以下)、あるいはこの層を含むまで
窒化される。イオン窒化をり、C電源を用いて行えば絶
縁部材であるAl2O3には損傷を与えることなく、電
気的に導通のあるTiにのみ窒化される。A desired thickness of several μm is deposited on an Al2O3 substrate by sputtering.
A Ti film having a thickness of m to 10/l□ is uniformly formed. The T1 film forming temperature at this time is, for example, 200 to 300°C. Thereafter, it is etched into a desired pattern shape using a wet or dry method. For example, in the case of a wet method, etching is performed using a very general process shown in FIG. Next, the patterned sample was placed in a vacuum furnace for ion nitriding, and T
Temperature below the transformation point of i, for example 400-500'C;
Perform ion nitriding to diffuse N from the Ti surface, and
Let it be N. The depth of nitriding reaches approximately several 71 m to 10 nm, and nitridation is performed up to or including a layer (10 nm or less) that contributes to adhesion between Ti and Al2O3 at the interface with the substrate. When ion nitriding is performed using a C power source, only the electrically conductive Ti is nitrided without damaging the insulating material Al2O3.
また、上記実施例ではTi膜をスパッタ法により形成す
る方法について説明したが、電子ビーム蒸着、レーザP
VD法、イオンブレーティング等のいわゆるPVD法や
TiCl4ガス等を用いたプラズマCVD法等の方法で
形成することができることは言うまでもない。 また
、上記実施例ではTiのパターンを形成した後、イオン
窒化を施す例を示したが、Tiの底膜1&イオン窒化を
施し、その後熱硝酸等でパターンエツチングしても良い
。In addition, in the above embodiment, a method of forming a Ti film by sputtering method was explained, but electron beam evaporation, laser P
It goes without saying that it can be formed by a method such as a so-called PVD method such as a VD method or ion blating, or a plasma CVD method using TiCl4 gas or the like. Further, in the above embodiment, an example was shown in which ion nitriding was performed after forming a Ti pattern, but it is also possible to perform ion nitriding with a Ti bottom film 1 and then pattern etching with hot nitric acid or the like.
また、N2ガスを用いたイオン窒化の例について示した
か、例えば、CH4やN2ガスとの混合ガスを用いた炭
化等によil T i C,T i N、 T i
CNの単体もしくはその混合物を形成しても良い。In addition, an example of ion nitriding using N2 gas is shown, for example, il T i C, T i N, T i
A simple substance of CN or a mixture thereof may be formed.
以上のように第1の手法というのはパターン形成の前段
はあるが、−旦Ti膜を形成した後1表面から窒化や炭
化により改質する手法である。As described above, the first method is a method in which a Ti film is first formed and then modified by nitriding or carbonizing from one surface, although there is a step before pattern formation.
次に第2の手法について例をあげて説明する。Next, the second method will be explained using an example.
Tiの変態点以下の所望の温度、例えば200〜300
’Cに加熱されたAl2O3基板上にパターンマスク
を置き、最初は通常のArスパッタ法によりTi膜を形
成する。Ti膜の厚さが10nmに達する前の極薄膜が
形成されると、スパッタ雰囲気中にN2ガスを導入し、
反応性スパンタ広によりTN膜を所望の厚さく数μnt
”−10p m )まで形成する。 後から、導入
するガスを炭素を含んだガス例えばCH4単体やこれと
N2との混合ガス等に変えることによりTiC,TiN
、T1CNの単体もしくはその混合物を形成することが
できることはいうまでもない。A desired temperature below the transformation point of Ti, e.g. 200-300
A pattern mask is placed on an Al2O3 substrate heated to 'C, and a Ti film is initially formed by the usual Ar sputtering method. When an extremely thin Ti film is formed before the thickness reaches 10 nm, N2 gas is introduced into the sputtering atmosphere,
A reactive spunter is used to make the TN film to the desired thickness of several μnt.
Later, by changing the introduced gas to a gas containing carbon, such as CH4 alone or a mixed gas of CH4 and N2, TiC, TiN
, T1CN alone or a mixture thereof can be formed.
以上のように第2の手法というのは膜を形成するインプ
ロセス中で′、Ti−+TiNのように連続的に異々る
膜を形成する方法である。As described above, the second method is a method in which different films, such as Ti-+TiN, are continuously formed during the in-process of forming the film.
このようにして製造された薄型高温ヒータは、密着層お
よび抵抗体層の形成温度が共にTiの変態点よ(]低い
ため、ヒータ製造中にTiのα→β変態が起こらないた
め体積変化による劣化が発生しにくく、また、ヒータ使
用中に密着層として余分なTi成分が抵抗体層に拡散し
ても、抵抗体層もTi成分を含んでいるので悪影響を及
ぼさず、密着層は安定化される。In the thin high-temperature heater manufactured in this way, the formation temperature of both the adhesive layer and the resistor layer is lower than the transformation point of Ti, so the α→β transformation of Ti does not occur during heater manufacturing, so the change in volume is Deterioration is less likely to occur, and even if excess Ti components diffuse into the resistor layer as an adhesive layer during use of the heater, there will be no adverse effects as the resistor layer also contains Ti components, and the adhesive layer will be stabilized. be done.
なお、以上のような2手法で形成した薄型高温ヒータを
基板上に複数並べて形成することにより大面積化や大量
生産に適していることは言うまでもない。It goes without saying that forming a plurality of thin high-temperature heaters formed using the two methods described above on a substrate is suitable for increasing the area and mass production.
さらに、上記実施例では密着層および抵抗体層を共にT
iの変態点未満の温度で形成した場合に1
ついて説明したが、密着層および抵抗体層を共にTiの
変態点以上の温度で形成してもよく、この場合は、密着
層としては余分なTi成分な製造中に拡散させてしまう
ので、その後変態点以上の例えば1000°C程度で使
用しても上記T1のα→β変態に伴う高温劣化を生じる
ことはない。Furthermore, in the above embodiment, both the adhesive layer and the resistor layer are T
Although 1 has been described in the case where the adhesive layer and the resistor layer are formed at a temperature lower than the transformation point of Ti, both the adhesive layer and the resistor layer may be formed at a temperature higher than the transformation point of Ti. Since the Ti component is diffused during manufacture, even if it is subsequently used at temperatures above the transformation point, for example, about 1000° C., high temperature deterioration associated with the α→β transformation of T1 will not occur.
[発明の効果]
以上のように、この発明によれば、絶縁部材上に形成さ
れたTiよりなる密着層、およびこの密着層を介して上
記絶縁部材上に形成されたTi化合物よiJなる抵抗体
層を備えたので、抵抗体層と絶縁部材との密着性が高く
、しかも使用時の抵抗変化の少々い、長期信頼性の高い
薄型高温ヒータが得られる効果がある。[Effects of the Invention] As described above, according to the present invention, the adhesion layer made of Ti formed on the insulating member and the Ti compound formed on the insulating member via this adhesion layer create a resistance of iJ. Since the resistor layer is provided, there is an effect that a thin high temperature heater with high adhesion between the resistor layer and the insulating member, little change in resistance during use, and high long-term reliability can be obtained.
また、本発明の別の発明によれば、絶縁基板上にTiよ
りなる密着層およびTi化合物よりなる抵抗体層を形成
するのに、上記密着層および抵抗体層共に上記Tiのα
→βの変態点未満の温度で形成するか、または上記密着
層および抵抗体層共に上記変態点以上の温度で形成する
ので、ヒータ2
製造中にTiが高温劣化するのを防止できる。According to another aspect of the present invention, when forming an adhesion layer made of Ti and a resistor layer made of a Ti compound on an insulating substrate, both the adhesion layer and the resistor layer are made of α of the Ti compound.
Since it is formed at a temperature below the transformation point of →β, or both the adhesive layer and the resistor layer are formed at a temperature above the transformation point, it is possible to prevent Ti from deteriorating at high temperatures during manufacture of the heater 2.
第1図はこの発明の一実施例による薄型高温ヒータを示
す断面構成図、第2図は第1図の薄型高温ヒータの製造
工程一部である一般的な工・ンチング工程を示す工程図
、第3図は従来の薄型高温ヒータを利用した電子管カソ
ード装置を示す断面構成図、第3図は従来の薄膜形成法
による薄型高温ヒータの製造方法を示す工程図、第4図
は従来のヒータの抵抗値の経時変化を示す特性図である
。
図において、〈1)は絶縁部組、〈2)は密着層、〈3
〉は抵抗体層である。
なお、図中同一符号は同一部分または相当部分を示す。FIG. 1 is a cross-sectional configuration diagram showing a thin high-temperature heater according to an embodiment of the present invention, FIG. 2 is a process diagram showing a general machining process that is part of the manufacturing process of the thin high-temperature heater of FIG. 1, Figure 3 is a cross-sectional configuration diagram showing an electron tube cathode device using a conventional thin high-temperature heater. Figure 3 is a process diagram showing a method for manufacturing a thin high-temperature heater using a conventional thin film forming method. FIG. 3 is a characteristic diagram showing a change in resistance value over time. In the figure, <1) is the insulation part assembly, <2) is the adhesive layer, and <3
> is a resistor layer. Note that the same reference numerals in the figures indicate the same or equivalent parts.
Claims (2)
よびこの密着層を介して上記絶縁部材上に形成されたT
i化合物よりなる抵抗体層を備えた薄型高温ヒータ。(1) An adhesion layer made of Ti formed on the insulating member, and T formed on the insulating member via this adhesion layer.
A thin high temperature heater equipped with a resistor layer made of i-compound.
物よりなる抵抗体層を形成するのに、上記密着層および
抵抗体層共に上記Tiのα→βの変態点未満の温度で形
成するか、または上記密着層および抵抗体層共に上記変
態点以上の温度で形成する薄型高温ヒータの製造方法。(2) When forming an adhesion layer made of Ti and a resistor layer made of a Ti compound on an insulating substrate, are both the adhesion layer and the resistor layer formed at a temperature below the α→β transformation point of Ti? , or a method for manufacturing a thin high-temperature heater, in which both the adhesive layer and the resistor layer are formed at a temperature equal to or higher than the transformation point.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1181016A JPH0343985A (en) | 1989-07-12 | 1989-07-12 | Thin high temperature heater and manufacture thereof |
| DE69022651T DE69022651D1 (en) | 1989-07-12 | 1990-07-11 | Thin high temperature heating element and process for its production. |
| US07/550,976 US5155340A (en) | 1989-07-12 | 1990-07-11 | Thin high temperature heater |
| EP90307591A EP0408342B1 (en) | 1989-07-12 | 1990-07-11 | Thin high temperature heater and method for manufacturing the same |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1181016A JPH0343985A (en) | 1989-07-12 | 1989-07-12 | Thin high temperature heater and manufacture thereof |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0343985A true JPH0343985A (en) | 1991-02-25 |
Family
ID=16093280
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1181016A Pending JPH0343985A (en) | 1989-07-12 | 1989-07-12 | Thin high temperature heater and manufacture thereof |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0343985A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2020010004A (en) * | 2018-07-12 | 2020-01-16 | Koa株式会社 | Resistor and circuit substrate |
-
1989
- 1989-07-12 JP JP1181016A patent/JPH0343985A/en active Pending
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2020010004A (en) * | 2018-07-12 | 2020-01-16 | Koa株式会社 | Resistor and circuit substrate |
| WO2020012926A1 (en) * | 2018-07-12 | 2020-01-16 | Koa株式会社 | Resistor and circuit board |
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