JPS592626B2 - Thin film thermal head - Google Patents
Thin film thermal headInfo
- Publication number
- JPS592626B2 JPS592626B2 JP52002059A JP205977A JPS592626B2 JP S592626 B2 JPS592626 B2 JP S592626B2 JP 52002059 A JP52002059 A JP 52002059A JP 205977 A JP205977 A JP 205977A JP S592626 B2 JPS592626 B2 JP S592626B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- heating resistor
- thermal head
- insulating
- glass 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.)
- Expired
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Description
【発明の詳細な説明】
本発明は小さな薄膜抵抗体のジュール熱を利用して感熱
紙を安定に発色させるための薄膜型サーマルヘッドに関
し、特に耐熱衝撃性、耐酸化性、安定性にすぐれた薄膜
型サーマルヘッドを提供するものである。[Detailed Description of the Invention] The present invention relates to a thin-film thermal head for stably coloring thermal paper using Joule heat from a small thin-film resistor, which has particularly excellent thermal shock resistance, oxidation resistance, and stability. The present invention provides a thin film type thermal head.
一般に、薄膜型サーマルヘッドに利用されている発熱抵
抗体としてはTa2N、NiCrがよく知られた例であ
り、その構成としてはセラミック基板上に保護層として
数十μのガラス層を設け、この上に発熱抵抗体としてT
a2N、NiCr等の薄膜を約0.1μ程度の膜厚で形
成し、さらにこの発熱抵抗体上に電極を形成して発熱体
を構成するとともに、その発熱抵抗体と電極の一部を覆
うように酸化防止膜および耐摩耗層を形成することによ
り構成されている。In general, Ta2N and NiCr are well-known examples of heating resistors used in thin-film thermal heads, and their structure consists of a glass layer of several tens of microns thick as a protective layer on a ceramic substrate, and T as a heating resistor
A thin film of a2N, NiCr, etc. is formed with a film thickness of about 0.1μ, and an electrode is further formed on this heating resistor to constitute a heating element, and a part of the heating resistor and electrode is covered. It is constructed by forming an anti-oxidation film and a wear-resistant layer on the surface.
ところで、Na2N、NiCr等は比抵抗ρが5×10
−4Ω】程度であり、サーマルヘッドとして要求される
抵抗値Rが100〜300Ω、発熱ドットのL /W(
Lはドットの長さ、wはドットの幅)が1〜3という要
求から発熱抵抗体を約0.1μ前後の極めてうすい膜厚
に設定することが必要になる。By the way, Na2N, NiCr, etc. have a specific resistance ρ of 5×10
-4Ω], the resistance value R required for a thermal head is 100 to 300Ω, and the L/W of the heating dot (
Since L is the length of the dot and W is the width of the dot), it is necessary to set the heat generating resistor to an extremely thin film thickness of about 0.1 μm because of the requirement that the value is 1 to 3.
しかし、サーマルヘッドは、通常300〜400℃に達
する敬重secの熱パルスを繰返し印加して用いるため
、このような薄い発熱抵抗体を用いると、機械的強度が
小さいため、基板との熱膨張率差等により、前記薄い発
熱抵抗体にクラックが生じ耐熱衝撃性が極めて悪くなる
。この欠点を除去するため、本発明者らは従来のTa2
N、NiCrより優れた耐熱衝撃性、耐酸化性を有する
サーマルヘッドの発熱抵抗体としてTa、Mo、Ti、
W、Zr等の高融点金属とSiとの合金を用いたものを
先に提案している。However, since thermal heads are used by repeatedly applying thermal pulses that reach 300 to 400 degrees Celsius, the thermal expansion coefficient with the substrate is low when using such a thin heat generating resistor due to its low mechanical strength. Due to the difference, cracks occur in the thin heating resistor, resulting in extremely poor thermal shock resistance. In order to eliminate this drawback, we have developed a conventional Ta2
Ta, Mo, Ti,
A method using an alloy of high melting point metals such as W and Zr and Si was previously proposed.
すなわち、高融点金属とSiとの合金よりなる発熱抵抗
体は、Ta2N、NiCr等の薄膜よりなる従来の薄膜
抵抗体にくらべて、比抵抗ρの値を大きくすることがで
きる。That is, a heat generating resistor made of an alloy of a high melting point metal and Si can have a larger specific resistance ρ than a conventional thin film resistor made of a thin film of Ta2N, NiCr or the like.
そのためサーマルヘッドの発熱抵抗体として、高融点金
属とSiの合金を用いた場合、必要な抵抗100〜30
0Ωを得るために、その膜厚を従来と比較して厚くする
ことができ、前記したNa2N,NiCr等よりなる発
熱抵抗体のクラツクの問題を除去できることになる。Therefore, when an alloy of high melting point metal and Si is used as the heating resistor of the thermal head, the required resistance is 100 to 30.
In order to obtain 0Ω, the film thickness can be increased compared to the conventional one, and the above-mentioned problem of cracks in the heating resistor made of Na2N, NiCr, etc. can be eliminated.
事実本発明者等ら先に提案したサーマルヘツドでは、優
れた耐熱衝撃性、耐酸化性を得るため、前述のTa,M
O,Ti,W,Zr等の高融点金属TaとSiとの合金
の重量比M/Siを適切に定めることにより比抵抗ρを
1XI0−3〜5×10−2Ωo程度と従来の発熱抵抗
体より1〜2桁高くし、膜厚を0.1μ以上数μに厚く
設定することによりサーマルヘツドとしての発熱抵抗体
として使用していた。In fact, in the thermal head previously proposed by the present inventors, in order to obtain excellent thermal shock resistance and oxidation resistance, the above-mentioned Ta and M
By appropriately determining the weight ratio M/Si of the alloy of high melting point metal Ta such as O, Ti, W, and Zr and Si, the specific resistance ρ can be set to about 1XI0-3 to 5x10-2Ωo, which is the conventional heating resistor. By increasing the film thickness by one to two orders of magnitude and setting the film thickness to 0.1 μm or more and several μm, it was used as a heating resistor for a thermal head.
しかしながら、一方、比抵抗ρが1×10−3〜5×1
0−2Ωoとなるように高融点金属とSiとの重量比M
/Siを調整して絶縁性基板1上に安定に形成すること
は製造上非常に難しいことが実験的に明らかになつてき
た。However, on the other hand, the specific resistance ρ is 1×10−3 to 5×1
The weight ratio M of high melting point metal and Si is set to 0-2Ωo.
It has become experimentally clear that it is very difficult to adjust /Si and stably form it on the insulating substrate 1 in terms of manufacturing.
すなわち、第2図はTa,MO,Ti,W,Zr等の高
融点金属MとSiとの合金についてその重量比M/Si
と比抵抗ρとの相関を示しており、同図より明らかなよ
うに、比抵抗ρが1×10−3〜5X10−2Ωoの範
囲では、重量比M/Siの変化に対して比抵抗ρが急激
に変化している。That is, FIG. 2 shows the weight ratio M/Si of alloys of high melting point metals M such as Ta, MO, Ti, W, and Zr and Si.
As is clear from the figure, in the range of resistivity ρ from 1 x 10-3 to 5 is changing rapidly.
したがつて、この比抵抗ρの範囲では高融点金属とSi
との重量比M/Siを調整して、発熱抵抗体を絶縁性基
板上に安定に形成することは非常に難しい。一方、比抵
抗ρが5X104〜5X10−3ΩGの範囲では、重量
比M/Siの変化に対して比抵抗ρの変化が小さく、サ
ーマルヘツドの発熱抵抗体として安定に形成できること
になる。以上を要するに、Ta,MO,Ti,W,Zr
等の高融金属とSiとの合金を用いた場合には製造上の
問題から、その比抵抗ρを5×10−4〜5×10−3
Ωoと低くすることが望ましく、そのためサーマルヘツ
ドの発熱抵抗体として用いた場合、膜厚が従来のTa2
N,NiCr等の場合と同様に0.1μ程度になり、耐
熱衝撃性を十分に大きくできなかつた。本発明は、この
ようなTa,MO,Ti,W,Zr等の高融点金属とS
iとの合金からなる発熱抵抗体において、その膜厚が0
.1μ程度と薄くなつても十分な耐熱衝撃性、耐酸化性
が得られるようにすることを目的としている。Therefore, in this range of resistivity ρ, high melting point metal and Si
It is very difficult to stably form a heating resistor on an insulating substrate by adjusting the weight ratio M/Si. On the other hand, when the resistivity .rho. is in the range of 5.times.10@4 to 5.times.10@-3 .OMEGA.G, the change in the resistivity .rho. is small with respect to the change in the weight ratio M/Si, and it can be stably formed as a heating resistor for a thermal head. In summary, Ta, MO, Ti, W, Zr
When using an alloy of Si and a high-melting metal such as
It is desirable that the film thickness be as low as Ωo, so when used as a heating resistor for a thermal head, the film thickness will be lower than that of the conventional Ta2.
As in the case of N, NiCr, etc., the thickness was about 0.1μ, and the thermal shock resistance could not be sufficiently increased. The present invention combines such high melting point metals such as Ta, MO, Ti, W, and Zr with S
In the heating resistor made of an alloy with i, its film thickness is 0
.. The purpose is to obtain sufficient thermal shock resistance and oxidation resistance even when the thickness is as thin as about 1 μm.
すなわち、本発明の薄膜型サーマルヘツドは少なくとも
表面にガラス層を有する絶縁性基板上に、フ高融点金属
とSiとの合金よりなる発熱抵抗体を絶縁性Si薄膜を
介して形成することを特徴とする。That is, the thin film type thermal head of the present invention is characterized in that a heat generating resistor made of an alloy of a high melting point metal and Si is formed on an insulating substrate having a glass layer on at least the surface via an insulating Si thin film. shall be.
前記絶縁性Si薄膜は絶縁性基板と発熱抵抗体間のバツ
フア層として有効に作用し、発熱抵抗体の厚みが0.1
μ程度であつても十分な耐熱衝撃性、耐酸化性のサーマ
ルヘツドが得られることになる。以下、本発明の薄膜型
サーマルヘツドにつき、第1図〜第3図の図面を用いて
説明する。The insulating Si thin film effectively acts as a buffer layer between the insulating substrate and the heating resistor, and the thickness of the heating resistor is 0.1.
A thermal head with sufficient thermal shock resistance and oxidation resistance can be obtained even if the thickness is around μ. Hereinafter, the thin film type thermal head of the present invention will be explained with reference to the drawings of FIGS. 1 to 3.
第1図に本発明の一実施例による薄膜型サーマルヘツド
を示し、第1図において1はアルミナ等の絶縁性基板、
2はこの絶縁性基板1表面に形成したガラス層、3はこ
のガラス層2上に形成した比抵抗の高い絶縁性Si薄膜
で、この絶縁性Si薄膜3上には前述のTa,MO,T
i,W,Zr等の高融点金属とSiとの合金からなる比
抵抗ρが5×10−4〜5×10−3程度と低い発熱抵
抗体4が形成され、またこの発熱抵抗体4からは電極5
が電気的に接続されて引出されている。FIG. 1 shows a thin film thermal head according to an embodiment of the present invention, in which 1 is an insulating substrate made of alumina or the like;
2 is a glass layer formed on the surface of this insulating substrate 1, 3 is an insulating Si thin film with high specific resistance formed on this glass layer 2, and on this insulating Si thin film 3 are the aforementioned Ta, MO, T, etc.
A heat generating resistor 4 is formed which is made of an alloy of high melting point metal such as i, W, Zr, etc. and Si and has a low specific resistance ρ of about 5 x 10-4 to 5 x 10-3. is electrode 5
is electrically connected and pulled out.
6は耐摩耗層である。6 is a wear-resistant layer.
ここで、前記絶縁性基板1として数?厚のガラス板を用
いてもよく、この場合にはガラス層2を形成しなくても
よい。次に、絶縁性Si薄膜3の作用、効果について説
明する。Here, the number of insulating substrates 1? A thick glass plate may be used, and in this case, the glass layer 2 may not be formed. Next, the function and effect of the insulating Si thin film 3 will be explained.
第3図に発熱抵抗体に対する熱衝撃試験の結果を示し、
この第3図に示す特性は、パルス幅6msecで20m
sec毎の繰返しパルスを30分間印加した後の抵抗変
化を面積で規格化した電力G″/Wlt)で表わしたも
のである。Figure 3 shows the results of a thermal shock test on a heating resistor.
The characteristics shown in Fig. 3 are 20 m with a pulse width of 6 msec.
The change in resistance after repeatedly applying pulses every sec for 30 minutes is expressed as power (G''/Wlt) normalized by area.
なお、発熱部の面積は約0.015Td〜0.03T!
RlL程度である。また、第3図で特性Aは絶縁性Si
薄膜3がある場合、特性Bはこの絶縁性Si薄膜3がな
い場合のものである。第3図から明らかなように、A,
Bとも従来のNiCr,Ta2N等より優れた特性を示
している。In addition, the area of the heat generating part is approximately 0.015Td to 0.03T!
It is about RIL. In addition, in Figure 3, characteristic A is insulating Si.
When the thin film 3 is present, characteristic B is the case when this insulating Si thin film 3 is not present. As is clear from Figure 3, A,
Both B exhibit properties superior to conventional NiCr, Ta2N, etc.
またA,Bの場合、すなわち高融点金属MとSiとの合
金の場合、発熱部表面に保護層等を設けなくても良好な
特性が得られる。ここで、特にBよりAが優れている理
由、すなわち絶縁性Si薄膜3を設けた場合の方が、優
れた耐熱衝撃性を示している理由は、絶縁性Si薄膜3
によるガラス層2と発熱抵抗体4との間の熱ストレスの
緩和現象によるものと考えられる。すなわち比抵抗の小
さな膜厚数百Aの発熱抵抗体4がガラス層2(グレ−ス
トアルミナ等)上に直接形成されていると、熱ストレス
により発熱抵抗体4において電流方向と垂直方向にクラ
ツクが生じ発熱体が破壊される。この時、絶縁性Si薄
膜3をガラス層2と抵抗発熱体4との間に形成すると、
絶縁性S1薄膜3が、サーマルヘツドとして使用中の発
熱にて生じる熱ストレスに対するバツフアとなり、クラ
ツクが生じにくくなり、発熱抵抗体の寿命が増加する。
さらに、前記絶縁性Si薄膜3を設けることにより、製
造において発熱抵抗体4が02,H2等のガス成分より
受ける悪影響を緩和でき、発熱抵抗体4を安定的に形成
できる利点が生じる。すなわち、高融点金属とSiとの
合金よりなる発熱抵抗体4は膜形成中において02,H
2等のガス成分の影響を受け易く、ガスを多く含有した
発熱抵抗体膜は形成直後の比抵抗が大きくなり、熱スト
レスによりガスが放出され抵抗劣化(抵抗減少)を生ず
る。この場合、絶縁性Si薄膜3があると、01.,H
2等のガス成分を吸着し、発熱抵抗体4への悪影響を緩
和できる。Further, in the case of A and B, that is, in the case of an alloy of high melting point metal M and Si, good characteristics can be obtained without providing a protective layer or the like on the surface of the heat generating part. Here, the reason why A is particularly superior to B, that is, the reason why the case where the insulating Si thin film 3 is provided shows superior thermal shock resistance is that the insulating Si thin film 3
This is thought to be due to the phenomenon of relaxation of thermal stress between the glass layer 2 and the heat generating resistor 4 due to the above. In other words, if the heating resistor 4 with a film thickness of several hundred amps and a small resistivity is formed directly on the glass layer 2 (grayst alumina, etc.), the heating resistor 4 will crack in the direction perpendicular to the current direction due to thermal stress. occurs and the heating element is destroyed. At this time, if an insulating Si thin film 3 is formed between the glass layer 2 and the resistance heating element 4,
The insulating S1 thin film 3 acts as a buffer against thermal stress caused by heat generation during use as a thermal head, making it difficult for cracks to occur and extending the life of the heating resistor.
Further, by providing the insulating Si thin film 3, the adverse effects of gas components such as O2 and H2 on the heat generating resistor 4 during manufacturing can be alleviated, resulting in the advantage that the heat generating resistor 4 can be formed stably. That is, the heat generating resistor 4 made of an alloy of high melting point metal and Si has a temperature of 02,H during film formation.
A heating resistor film containing a large amount of gas has a high specific resistance immediately after formation, and gas is released due to thermal stress, causing resistance deterioration (resistance reduction). In this case, if there is an insulating Si thin film 3, 01. ,H
It is possible to adsorb gas components such as No. 2, etc., and alleviate the adverse effects on the heating resistor 4.
さらに、絶縁性薄膜としてSiを用いるとガラス層2上
に直接発熱抵抗体4を形成する場合と比較してガラス層
2と発熱抵抗体4との間の密着力が良好になる。Furthermore, when Si is used as the insulating thin film, the adhesion between the glass layer 2 and the heating resistor 4 becomes better than when the heating resistor 4 is formed directly on the glass layer 2.
これは、絶縁性Si薄膜3は、02の吸蔵効果が大きく
、ガラス層2と発熱抵抗体4との間で02を介して強い
接着力を生じるためと考えられる。This is considered to be because the insulating Si thin film 3 has a large 02 occlusion effect, and a strong adhesive force is generated between the glass layer 2 and the heating resistor 4 via the 02.
さらに、このような薄膜型のサーマルヘツドは発熱抵抗
体4の薄膜を絶縁性基板1上に蒸着してからエツチング
によりパターンを形成するが、MSi系の発熱抵抗体4
、特にMとしてTaを用いる場合には、エツチング液と
して弗硝酸系を使用しなければならず、これにより発熱
抵抗体4はもとよりガラス層2(ガラス基板を用いた場
全は基板自体)もエツチングされてしまう。これを防ぐ
ためにも絶縁性薄膜3の存在が有効であり、弗硝酸系の
エツチング液でエツチングされる材料を使用しても発熱
抵抗体4の厚み0.1μ前後の膜厚に対し数倍の厚みを
つけておけば、ガラス層2をエツチングしない選択エツ
チングが可能となる効果もある。Furthermore, in such a thin film type thermal head, a pattern is formed by depositing a thin film of the heating resistor 4 on the insulating substrate 1 and then etching it.
In particular, when Ta is used as M, it is necessary to use a fluoronitric acid-based etching solution, which etches not only the heating resistor 4 but also the glass layer 2 (or the substrate itself if a glass substrate is used). It will be done. The presence of the insulating thin film 3 is effective to prevent this, and even if a material that is etched with a fluoro-nitric acid-based etching solution is used, the thickness of the heating resistor 4 is several times the thickness of about 0.1 μm. If the thickness is increased, selective etching without etching the glass layer 2 can be performed.
以上の説明から明らかなように、本発明の薄膜型サーマ
ルヘツドは、Ta,MO,Ti,W,Zr等の高融点金
属とSiとの合金からなる発熱抵抗体を絶縁性Si薄膜
を介して表面にガラス層を形成したアルミナ基板やガラ
ス基板等の少なくとも表面にガラス層を有する絶縁性基
板上に形成したものであり、前記絶縁性Si薄膜はバッ
フア層として極めて有効に作用しサーマルヘツドを耐熱
衝撃性、耐酸化性の優れたものとすることができるとと
もに、製作上における発熱抵抗体の安定性も良好にでき
る。As is clear from the above description, the thin film thermal head of the present invention has a heating resistor made of an alloy of Si and a high melting point metal such as Ta, MO, Ti, W, or Zr, which is connected to the heating resistor through an insulating Si thin film. It is formed on an insulating substrate that has a glass layer on at least the surface, such as an alumina substrate or a glass substrate that has a glass layer on its surface.The insulating Si thin film acts extremely effectively as a buffer layer and makes the thermal head heat resistant. Not only can it have excellent impact resistance and oxidation resistance, but also the stability of the heating resistor during manufacturing can be improved.
しかもTa−Si等の発熱抵抗体を用いた場合にガラス
層との選択エツチングが可能となり、ガラス層がエツチ
ングされるのを防止できる。また、高融点金属とSiと
の合金のうちシリサイドを形成するもの、例えばTaを
例にとるとTaSi2,Ta5Si3,Ta2Si等を
中心とした合金を高温下で形成すると、膜厚が500A
程度でも充分な強さを得ることができ、比抵抗のばらつ
きも少なく、製作上の安定性がよい。Furthermore, when a heating resistor such as Ta-Si is used, selective etching with respect to the glass layer is possible, and etching of the glass layer can be prevented. In addition, when an alloy of high melting point metal and Si that forms silicide, such as TaSi2, Ta5Si3, Ta2Si, etc., is formed at high temperature, the film thickness is 500A.
Sufficient strength can be obtained even at a low level, there is little variation in specific resistance, and manufacturing stability is good.
このように本発明の薄膜型サーマルヘツドによれば、優
れた効果を有し、これからのこの分野における技術発展
に大きく貢献することができる。As described above, the thin film type thermal head of the present invention has excellent effects and can greatly contribute to future technological development in this field.
第1図は本発明の一実施例による薄膜型サーマルヘツド
の構造を示す断面図、第2図は高融点金属MとSiとの
合金の重量比M/Siと比抵抗との相関図、第3図は本
発明の薄膜型サーマルヘツドの効果を説明するための熱
衝撃試験の結果を示す特性図である。
1・・・・・・絶縁性基板、2・・・・・・ガラス層、
3・・・・・・絶縁性Si薄膜、4・・・・・・発熱抵
抗体。FIG. 1 is a sectional view showing the structure of a thin film thermal head according to an embodiment of the present invention, FIG. 2 is a correlation diagram between the weight ratio M/Si of an alloy of high melting point metal M and Si, and specific resistance. FIG. 3 is a characteristic diagram showing the results of a thermal shock test for explaining the effects of the thin film type thermal head of the present invention. 1... Insulating substrate, 2... Glass layer,
3... Insulating Si thin film, 4... Heat generating resistor.
Claims (1)
、高融点金属とSiとの合金よりなる発熱抵抗体を絶縁
性Si薄膜を介して形成した薄膜型サーマルヘッド。1. A thin film type thermal head in which a heating resistor made of an alloy of a high melting point metal and Si is formed on an insulating substrate having a glass layer on at least the surface thereof via an insulating Si thin film.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52002059A JPS592626B2 (en) | 1977-01-11 | 1977-01-11 | Thin film thermal head |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52002059A JPS592626B2 (en) | 1977-01-11 | 1977-01-11 | Thin film thermal head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5387242A JPS5387242A (en) | 1978-08-01 |
| JPS592626B2 true JPS592626B2 (en) | 1984-01-19 |
Family
ID=11518755
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52002059A Expired JPS592626B2 (en) | 1977-01-11 | 1977-01-11 | Thin film thermal head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS592626B2 (en) |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4892032A (en) * | 1972-02-29 | 1973-11-29 | ||
| JPS539399B2 (en) * | 1972-12-09 | 1978-04-05 | ||
| JPS559301B2 (en) * | 1974-12-16 | 1980-03-08 |
-
1977
- 1977-01-11 JP JP52002059A patent/JPS592626B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5387242A (en) | 1978-08-01 |
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