JPS598233B2 - thermal head - Google Patents
thermal headInfo
- Publication number
- JPS598233B2 JPS598233B2 JP52160138A JP16013877A JPS598233B2 JP S598233 B2 JPS598233 B2 JP S598233B2 JP 52160138 A JP52160138 A JP 52160138A JP 16013877 A JP16013877 A JP 16013877A JP S598233 B2 JPS598233 B2 JP S598233B2
- Authority
- JP
- Japan
- Prior art keywords
- thermal head
- heating resistor
- oxygen
- electron beam
- substrate
- 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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- Apparatuses And Processes For Manufacturing Resistors (AREA)
- Non-Adjustable Resistors (AREA)
Description
【発明の詳細な説明】
本発明は硼化ジルコニウムと酸素とからなる薄膜発熱抵
抗体を有するサーマルヘッドさらにはその製造方法に関
する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a thermal head having a thin film heating resistor made of zirconium boride and oxygen, and also to a method for manufacturing the same.
熱印字記録に用いられるサーマルヘッドは例えばガラス
のような電気的な絶縁体と平滑面とを有する基板上に複
数個の発熱抵抗体と、この発熱抵抗体に電力を供給する
ための電気導体とを設け、記録すべき情報に従つて必要
な熱パターンが得られるように、対応する発熱抵抗体に
電気導体を介して電流を流して発熱させ、記録媒体に接
触することにより記録を行なうものである。A thermal head used for thermal print recording includes a plurality of heat generating resistors on a substrate having an electrical insulator such as glass and a smooth surface, and an electric conductor for supplying power to the heat generating resistors. Recording is performed by applying a current to the corresponding heat-generating resistor through an electric conductor to generate heat, and contacting the recording medium with a corresponding heat-generating resistor so as to obtain the necessary thermal pattern according to the information to be recorded. be.
そこに用いられる発熱抵抗体としては、従来窒化タンタ
ル、ニクロム酸化錫等の薄膜発熱抵抗体、銀−パラジウ
ム等を用いた厚膜発熱抵抗体、シリコン半導体を用いた
半導体発熱抵抗体がある。このうち薄膜発熱抵抗体を用
いたサーマルヘッドは厚膜発熱抵抗体、半導体発熱抵抗
体等と比較して熱応答性がよく耐熱性、耐熱衝撃性に優
れ、寿命が長く、信頼性が高い等の特徴を有している。
この薄膜発熱抵抗体としては、従来、窒化タンタルが耐
熱性に優れ、信頼性も高く、又固有抵抗値も250〜3
00μΩ?と比較的高い値で製造の制御性もよいため、
特に多く用いられる。しかるに窒化タンタルは約300
℃以上の高温に於ては急激に酸化されその抵抗値が急激
に増加し、記録紙に印字する場合、印字濃度を劣化させ
る欠点がある。Heat generating resistors used therein include conventional thin film heat generating resistors such as tantalum nitride and dichrome tin oxide, thick film heat generating resistors using silver-palladium, etc., and semiconductor heat generating resistors using silicon semiconductor. Among these, thermal heads using thin film heating resistors have better thermal response, superior heat resistance and thermal shock resistance, longer lifespan, and higher reliability than thick film heating resistors, semiconductor heating resistors, etc. It has the following characteristics.
Conventionally, tantalum nitride has been used for this thin film heating resistor, which has excellent heat resistance, high reliability, and has a specific resistance value of 250 to 3.
00 μΩ? Since the value is relatively high and the controllability of manufacturing is good,
Especially often used. However, tantalum nitride has about 300
At high temperatures above .degree. C., it is rapidly oxidized and its resistance value increases rapidly, which has the disadvantage of deteriorating the print density when printing on recording paper.
一般にはこの欠点を補うために酸化シリコン(SiO2
)の耐酸化保護層を設け更にその上に酸化タンタル(T
a2O3)の耐摩耗層を設けてサーマルヘツドとして使
用しているが、サーマルヘツドを長時間駆動させた時の
抵抗変化はなお十分満足できるものではなかつた。特に
近年、高速サーマルヘツドの要求が増加しつつあるため
ヘツドの通電パルス巾を短かくして感熱紙を発色させる
必要があり、従つて電力は従来より増加することになり
、発熱抵抗体はさらに高温になるから寿命はより短くな
る。そのためさらに耐熱性のある発熱抵抗体が要求され
ている。また、窒化タンタルの面積抵抗は、通常50μ
Ω/口前後で、サーマルヘツドとして特に大きくした場
合でも100Ω/口程度であり更に抵抗値を大きくする
ためにはトリミングを行なつたり、膜厚を薄くする等の
方法を用いるが、その際製造工程が複雑になつたり、寿
命に対して悪影響を生じたりする等の欠点が発生する。Generally, silicon oxide (SiO2) is used to compensate for this drawback.
) is provided with an oxidation-resistant protective layer of tantalum oxide (T
Although a wear-resistant layer of a2O3) is provided and used as a thermal head, the change in resistance when the thermal head is operated for a long time is still not fully satisfactory. Particularly in recent years, as the demand for high-speed thermal heads has increased, it is necessary to shorten the energizing pulse width of the head to color the thermal paper.This means that the electric power required is higher than before, and the heating resistor is heated to even higher temperatures. Therefore, the lifespan becomes shorter. Therefore, there is a demand for a heating resistor with even higher heat resistance. Also, the sheet resistance of tantalum nitride is usually 50μ
The resistance value is around 100 Ω/hole even when the thermal head is made particularly large.In order to further increase the resistance value, methods such as trimming or thinning the film are used, but in this case manufacturing There are disadvantages such as the process becomes complicated and the lifespan is adversely affected.
このように窒化タンタル薄膜発熱抵抗体では面積抵抗を
大きくとれないため、抵抗体を加熱するだけの電力を供
給するためには必然的に電流が大きくなるり、電気導体
の抵抗値が問題になる。In this way, the tantalum nitride thin film heating resistor cannot have a large sheet resistance, so in order to supply enough power to heat the resistor, the current inevitably becomes large, and the resistance value of the electric conductor becomes a problem. .
即ち、薄膜発熱抵抗体の抵抗値に対して電気導体の抵抗
値が無視できなくなるから、抵抗体に接続された各電気
導体の距離の差異により各抵抗体の発熱量が異つてしま
い、記録パターンに濃度差が生じ記録品質が劣る。更に
記録密度を上げるため、薄膜発熱抵抗体の大きさを小さ
くすると、薄膜発熱抵抗体の面積抵抗値は不変で電気導
体の抵抗値のみ増大するから、電気導体における電力消
費が問題になるし、又これを避けるために電気導体の厚
さを極端に大きくすると多層配線の場合に表面の凹凸が
激しくなり摩耗にも弱くなるなど構造上大きな不都合が
生じることになる。In other words, since the resistance value of the electric conductor cannot be ignored compared to the resistance value of the thin film heating resistor, the amount of heat generated by each resistor will differ due to the difference in the distance of each electric conductor connected to the resistor, and the recording pattern will be different. There will be a difference in density between the images and the recording quality will be poor. Furthermore, if the size of the thin film heating resistor is reduced in order to increase the recording density, the sheet resistance value of the thin film heating resistor remains unchanged and only the resistance value of the electrical conductor increases, so power consumption in the electrical conductor becomes a problem. Furthermore, if the thickness of the electrical conductor is made extremely large in order to avoid this, in the case of multi-layer wiring, the surface becomes extremely uneven and becomes susceptible to abrasion, resulting in major structural problems.
又電流が大きいことは加熱用電源、スイツチング回路等
の容量を大きくしなければならない等の不都合も生じる
。本発明は上記の点を改良し、酸化されにくく抵抗値が
安定で、比抵抗を高い値まで選択できる薄膜発熱抵抗体
を用いたサーマルヘツドを提供し、その特徴とするとこ
ろは硼化ジルコニウムと酸素とからなる発熱抵抗体にあ
る。In addition, the large current also causes disadvantages such as the need to increase the capacity of the heating power source, switching circuit, etc. The present invention improves the above points and provides a thermal head using a thin film heating resistor that is resistant to oxidation, has a stable resistance value, and allows the specific resistance to be selected up to a high value. The heating resistor consists of oxygen.
この発熱抵抗体においては、硼化ジルコニウムと酸素と
が原子的なスケールで混在している。以下、図面を参照
しながら詳細に説明する。In this heating resistor, zirconium boride and oxygen are mixed on an atomic scale. A detailed description will be given below with reference to the drawings.
第1図は本発明に適用するサーマルヘツドの形状例の要
部断面図である。同図中の1はセラミツクス、ガラスあ
るいは、クレーストセラミックスのような電気的な絶縁
物で形成された基板である。2は硼化ジルコニウムと酸
素とからなる本発明に係る薄膜発熱抵抗体である。FIG. 1 is a sectional view of a main part of an example of the shape of a thermal head applied to the present invention. Reference numeral 1 in the figure is a substrate made of an electrical insulator such as ceramics, glass, or crystal ceramics. 2 is a thin film heating resistor according to the present invention made of zirconium boride and oxygen.
3は該薄膜発熱抵抗体に電力を供給するための電気導体
で、アルミニユウム、金等の電気良導体で、形成されて
いる。Reference numeral 3 denotes an electric conductor for supplying power to the thin film heating resistor, which is made of a good electric conductor such as aluminum or gold.
又4は薄膜発熱抵抗体及び電気導体の保護層で、例えば
電子ビーム蒸着、スパツタ一等によつて作製した酸化シ
リコン、酸化マグネシユウム、酸化アルミニウム、酸化
タンタルあるいはこれらを組合せた多層構成が用いられ
、これによつてサーマルヘツドの寿命を一層長くするこ
とができる。4 is a protective layer for the thin film heating resistor and electric conductor, for example, a multilayer structure made of silicon oxide, magnesium oxide, aluminum oxide, tantalum oxide, or a combination of these, manufactured by electron beam evaporation, sputtering, etc.; This makes it possible to further extend the life of the thermal head.
本発明の硼化ジルコニウムと酸素とからなる薄膜発熱抵
抗体の製造はスパツタリング、電子ビーム蒸着いずれも
可能であるが、電子ビーム蒸着での製造は大面積のサー
マルヘツドの製造や量産性に優れている。電子ビーム蒸
着で硼化ジルコニウムと酸素とからなるサーマルヘツド
を製造するには、硼化ジルコニウムの粉末を約100k
g/CTll以上の圧力でプレスしてタブレツトを作り
1刈『4T0rr以上の高真空度であらかじめ一定温度
に保つた基板上に蒸着させることができる。この時、酸
素の含有量を制御するために二ードルバルブ等によつて
酸素を含む気体を電子ビーム蒸着中に導入することも可
能である。このようにすると、発熱抵抗体中に酸素を原
子比でジルコニウム0.005以上含有させることがで
きる。酸素含有量は少なすぎては効果がなく、逆に多す
ぎると比抵抗の制御が難かしく、耐熱性も悪くなるので
ジルコニウムの0.01〜1.0(原子比)が適当であ
り、0.05〜0.6がより好ましく0.1〜0.3が
最も好ましい。また電子ビーム蒸着中に於いて200℃
〜500℃の基板加熱を行うことによつて基板に対して
本発明薄膜発熱抵抗体の密着性が向上し、又膜の安定性
に効果がある。このようにして製造された発熱抵抗体は
電子ビーム蒸着時に導入する酸素の量や基板加熱温度な
どによつて固有抵抗値で80μΩ?〜5000μΩ?ま
での選択が可能である。The thin film heating resistor of the present invention made of zirconium boride and oxygen can be manufactured by either sputtering or electron beam evaporation, but manufacturing by electron beam evaporation is superior in manufacturing large-area thermal heads and in mass production. There is. To manufacture a thermal head made of zirconium boride and oxygen by electron beam evaporation, approximately 100 kg of zirconium boride powder is required.
It is possible to make a tablet by pressing at a pressure of more than g/CTll and deposit it on a substrate that has been kept at a constant temperature in advance at a high vacuum level of 4T0rr or more. At this time, in order to control the oxygen content, it is also possible to introduce a gas containing oxygen during electron beam evaporation using a needle valve or the like. In this way, the heating resistor can contain oxygen and zirconium in an atomic ratio of 0.005 or more. If the oxygen content is too low, it will not be effective, and if it is too high, it will be difficult to control the specific resistance and the heat resistance will deteriorate, so 0.01 to 1.0 (atomic ratio) of zirconium is appropriate 0.05 to 0.6 is more preferable, and 0.1 to 0.3 is most preferable. Also, during electron beam evaporation, 200°C
By heating the substrate to 500 DEG C., the adhesion of the thin film heating resistor of the present invention to the substrate is improved and the stability of the film is also improved. The heat generating resistor manufactured in this way has a specific resistance value of 80 μΩ or more, depending on the amount of oxygen introduced during electron beam evaporation, the substrate heating temperature, etc. ~5000μΩ? It is possible to select up to.
つまり固有抵抗値を高く作成すれば、電極の抵抗値もあ
る程度高くても良いから製造工程が容易になり、電極が
薄くて良いから表面の凹凸が少なくなるので耐摩耗性が
改良され、電極部での電圧降下が無視できる程度である
ことから薄膜発熱抵抗体の発色濃度ムラが小さくなり、
マトリクス配線などの電極のパターン設剖(支){自由
になる。またこのようにして得られた発熱抵抗体は硼化
ジルコニウムと酸素とより成るが、不純物として若干の
窒素、炭素などを含むのが常である。In other words, if the specific resistance value is high, the manufacturing process will be easier because the electrode resistance value can be high to a certain extent, and the electrode can be made thinner, so the surface unevenness will be reduced, which will improve the abrasion resistance and improve the electrode part. Since the voltage drop at
Electrode pattern design (support) such as matrix wiring {Freedom. The heating resistor thus obtained is made of zirconium boride and oxygen, but usually contains some impurities such as nitrogen and carbon.
次に実施例に基づいて説明する。実施例 1
硼化ジルコニウムの粉末(三津和化学薬品製)を100
kg/d以上でプレスしたタブレツトを作成し、あらか
じめ充分に洗浄されたクレーストセラミックス基板上に
基板加熱300℃、真空度2×10−6T0rrまで真
空にひらいた後、乾燥空気を二ードルバルブで導入しな
がら真空度5×10−6T0rrで1000λの厚さに
電子ビームで蒸着した。Next, an explanation will be given based on an example. Example 1 100% of zirconium boride powder (manufactured by Mitsuwa Chemicals)
A tablet is made by pressing at a pressure of more than kg/d, and after heating the substrate to 300℃ and vacuuming it to a vacuum level of 2×10-6T0rr on a creste ceramic substrate that has been thoroughly cleaned in advance, dry air is introduced using a needle valve. At the same time, electron beam evaporation was performed to a thickness of 1000λ at a vacuum degree of 5×10 −6 T0rr.
この面積抵抗は約80Ω/口(固有抵抗値は約800P
0c:m)であつた。この膜の組成をイオンマイクロア
ナライザで調べたところ酸素がジルコニウムの0.18
(原子比)含まれていた。この上にチタン20λ、アル
ミニウムを1μm電子ビーム蒸着で付け、選択エツチン
グで4本/Mmの分解能をもつサーマルヘツドパターン
を形成し、これをサーマルヘツドA1とした。さらにこ
の上に保護層として酸化シリコン(SiO2)を1μm
1酸化タンタル、(Ta2O5)を10μm連続的にス
パツタで積層し、サーマルヘツドA2とした。比較の為
に、高周波2極の反応スパツタリングによつてタンタル
をターゲツトとし、アルゴンと窒素の全圧力が8X10
−2T0rr1窒素分圧が1×10−4T0rrの条件
で1000人の厚さの窒化タンタル薄膜発熱抵抗体のサ
ーマルヘツドB1を作成した。This area resistance is approximately 80Ω/mouth (specific resistance value is approximately 800P)
0c:m). When the composition of this film was examined using an ion microanalyzer, oxygen was found to be 0.18% of zirconium.
(atomic ratio) included. On top of this, titanium 20λ and aluminum were deposited to a thickness of 1 μm by electron beam evaporation, and a thermal head pattern with a resolution of 4 lines/mm was formed by selective etching, and this was designated as thermal head A1. Furthermore, silicon oxide (SiO2) with a thickness of 1 μm is added as a protective layer on top of this.
Tantalum monoxide (Ta2O5) was continuously laminated to a thickness of 10 μm by sputtering to form a thermal head A2. For comparison, tantalum was targeted by high frequency bipolar reactive sputtering and the total pressure of argon and nitrogen was 8X10.
-2T0rr1 A thermal head B1 of a tantalum nitride thin film heating resistor having a thickness of 1000 was fabricated under the condition that the nitrogen partial pressure was 1 x 10-4T0rr.
この窒化タンタル薄膜発熱抵抗体は比抵抗が260μΩ
?で面積抵抗は26Ω/口であつた。サーマルヘツドB
1に対し、さらに保護膜として酸化シリコン(SiO2
)を1μm1酸化タンタル(Ta2O5)を10μm連
続的にスパツタで積層し、サーマルヘツドB2とした。
これらのサーマルヘツドに対して、50zで6msの矩
形波を30分ごとに1w/MIずつパワーアツプしなが
ら加速テストを行つた。この結果を第2図に示す。同図
から明らかなように、本発明にかかる製造方法で作成し
た薄膜発熱抵抗体を有するサーマルヘツドは高印加電力
に耐えることができ、高温での抵抗変化が少いことがわ
かつた。つまり、比較例では保護膜なしでは実用するの
が難かしいのに対して、杢発明に係るサーマルヘツドは
保護膜なしでも実用でき、保護膜をつけた場合には非常
に良い耐熱性が得られた。実施例 2
硼化ジルコニウム(ZrB2)の粉末を100kg/C
d以上でプレスしたタブレツトを作成し、あらかじめ充
分に洗浄されたクレーストセラミックス基板上に基板加
熱500℃乾燥空気を導入しながら真空度4×10−5
T0rrで800λの厚さに電子ビーム蒸着した。This tantalum nitride thin film heating resistor has a specific resistance of 260 μΩ.
? The area resistance was 26Ω/mouth. Thermal head B
1, silicon oxide (SiO2
) was continuously laminated with 10 μm of tantalum oxide (Ta2O5) by sputtering to form a thermal head B2.
These thermal heads were subjected to an acceleration test using a 6 ms rectangular wave at 50 z while increasing the power by 1 w/MI every 30 minutes. The results are shown in FIG. As is clear from the figure, it was found that the thermal head having a thin film heating resistor produced by the manufacturing method according to the present invention can withstand high applied power and has little change in resistance at high temperatures. In other words, while the comparative example is difficult to put into practical use without a protective film, the thermal head according to Moto's invention can be put into practical use without a protective film, and when a protective film is attached, very good heat resistance can be obtained. Ta. Example 2 Zirconium boride (ZrB2) powder at 100 kg/C
A tablet is made by pressing at a temperature of d or higher, and the substrate is heated at 500°C on a claest ceramic substrate that has been thoroughly cleaned in advance.While dry air is introduced, the degree of vacuum is 4 x 10-5.
Electron beam evaporation was performed at T0rr to a thickness of 800λ.
この時、面積抵抗は70Ω/口(固有抵抗値は560μ
ΩCrlL)であつた。この上にバナジウムを30λ、
金を1.5μm電子ビームで付け、選択エツチングで4
本/M7ltの分解能をもつサーマルヘツドパターンを
形成し、更にSlO23μM,.Al2O36μmをス
パツタリングによつて連続的に積層しサーマルヘツドと
した。このサーマルヘツドに対して実施例1と同じ加速
テストをおこなつたところ20w/mlまでの抵抗変化
率が2%以内であり、窒化タンタルを発熱抵抗体として
用いた場合に比して非常に良好な結果が得られた。実施
例 3
硼化ジルコニウム(ZrB2)の粉末を100k9/C
rit以上でプレスしたタブレツトを作成し、あらかじ
め充分に洗浄されたクレーストセラミックス基板上に基
板加熱200℃酸素を二ードルバルブで導入しながら真
空度2×10−5T0rrで800人の厚さに電子ビー
ム蒸着した。At this time, the area resistance is 70Ω/mouth (specific resistance value is 560μ
ΩCrlL). On top of this, add 30λ of vanadium,
Gold was attached using a 1.5 μm electron beam and selectively etched to 4
A thermal head pattern with a resolution of 1/M7lt was formed, and additionally 23 μM SlO, . A thermal head was made by continuously laminating Al2O with a thickness of 36 μm by sputtering. When this thermal head was subjected to the same acceleration test as in Example 1, the rate of change in resistance up to 20w/ml was within 2%, which was much better than when tantalum nitride was used as the heating resistor. The results were obtained. Example 3 Zirconium boride (ZrB2) powder at 100k9/C
A tablet was made by pressing at a temperature higher than R.I.T., and then an electron beam was applied to a 800-meter thick plate at a vacuum level of 2 x 10-5 T0rr while heating the substrate at 200°C and introducing oxygen using a needle valve onto a claest ceramic substrate that had been thoroughly cleaned in advance. Deposited.
この時、面積抵抗は150Ω/口(固有抵抗値は120
0,Ω(社)であつた。この上にチタンを30人、金を
1.5μm電子ビームで付け、選択エツチングで4本/
舅露の分解能をもつサーマルヘツドパターンを形成し、
更にMgO6μmをスパツタリングによつて連続的に積
層しサーマルヘツドとした。At this time, the area resistance is 150 Ω/mouth (the specific resistance value is 120
It was 0,Ω (sha). On top of this, 30 pieces of titanium and 1.5 μm of gold were added using an electron beam, and 4 pieces/piece were selectively etched.
Forms a thermal head pattern with a resolution of
Further, 6 μm of MgO was continuously laminated by sputtering to form a thermal head.
このサーマルヘツドに対して実施例1と同じ加速テスト
をおこなつたところ21w/M7lまでの抵抗変化率が
2%以内であり、窒化タンタルを発熱抵抗体として用い
た場合に比して非常に良好な結果が得られた。When this thermal head was subjected to the same acceleration test as in Example 1, the resistance change rate up to 21w/M7l was within 2%, which was much better than when tantalum nitride was used as the heating resistor. The results were obtained.
実施例 4
硼化ジルコニウム(ZrB2)の粉末100kg/d以
上でプレスしたタブレツトを作成し、あらかじめ充分に
洗浄されたクレーストセラミックス基板上に基板加熱3
00℃酸素を二ードルバルブで導入しながら8×10−
5T0rrで800人の厚さに電子ビーム蒸着した。Example 4 A tablet was made by pressing 100 kg/d or more of zirconium boride (ZrB2) powder, and the tablet was heated 3 times on a creest ceramic substrate that had been thoroughly cleaned in advance.
8×10− while introducing oxygen at 00℃ with a needle valve.
Electron beam evaporation was performed at 5T0rr to a thickness of 800 mm.
この時、面積抵抗は520Ω/口(固有抵抗値は410
0μΩ(1−JモV!)であつた。この上にチタンを30
λ、アルミニウムを1.5μm電子ビームで″付け、選
択エツチングで4本/mlの分解能をもつサーマルヘツ
ドパターンを形成し、更にSlO23μM,.Ta2O
56μmをスパツタリングによつて連続的に積層しサー
マルヘツドとした。At this time, the area resistance is 520 Ω/mouth (the specific resistance value is 410
It was 0μΩ (1-JmoV!). 30 titanium on top of this
λ, aluminum was attached with a 1.5 μm electron beam, a thermal head pattern with a resolution of 4 lines/ml was formed by selective etching, and 23 μM of SlO, .Ta2O
A thermal head was formed by continuously laminating 56 μm thick layers by sputtering.
このサーマルヘツドに対して実施例1と同じ加速テスト
をおこなつたところ23w/MIまでの抵抗変化率が2
%以内であり、窒化タンタルを発熱抵抗体として用いた
場合に比して非常に良好な結果が得られた。When this thermal head was subjected to the same acceleration test as in Example 1, the resistance change rate up to 23w/MI was 2.
%, and very good results were obtained compared to the case where tantalum nitride was used as the heating resistor.
第1図は本発明に係るサーマルヘツドの形状例の要部断
面図。
第2図は本発明の効果を示す特性図。1・・・・・・基
板、2・・・・・・薄膜発熱抵抗体、3・・・・・・電
気導体、4・・・・・・保護層。FIG. 1 is a sectional view of a main part of an example of the shape of a thermal head according to the present invention. FIG. 2 is a characteristic diagram showing the effects of the present invention. DESCRIPTION OF SYMBOLS 1... Substrate, 2... Thin film heating resistor, 3... Electric conductor, 4... Protective layer.
Claims (1)
熱抵抗体に電力を供給する電気導体とを有するサーマル
ヘッドにおいて、発熱抵抗体が硼化ジルコニウムと酸素
とからなることを特徴とするサーマルヘッド。 2 発熱抵抗体において、酸素の含有量がジルコニウム
の0.005(原子比)以上である特許請求の範囲第1
項記載のサーマルヘッド。 3 発熱抵抗体において、酸素の含有量がジルコニウム
の0.01〜1.0(原子比)である特許請求の範囲第
1項記載のサーマルヘッド。 4 発熱抵抗体が酸化シリコン薄膜で覆われている特許
請求の範囲第1項ないし第3項記載のサーマルヘッド。 5 酸化タンタルの保護膜を有する特許請求の範囲第1
項ないし第4項記載のサーマルヘッド。 6 酸化アルミニウムの保護膜を有する特許請求の範囲
第1項ないし第4項記載のサーマルヘッド。 7 酸化マグネシウムの保護膜を有する特許請求の範囲
第1項ないし第4項記載のサーマルヘッド。 8 硼化ジルコニウムと酸素とからなる発熱抵抗体を電
子ビーム蒸着で製造することを特徴とするサーマルヘッ
ドの製造方法。 9 酸素を含む気体を導入しながら電子ビーム蒸着を行
う時特許請求の範囲第8項記載の製造方法。 10 200℃〜500℃の基板加熱を行いながら電子
ビーム蒸着を行う特許請求の範囲第8項または第9項記
載の製造方法。[Scope of Claims] 1. A thermal head having a substrate, a heating resistor formed on the substrate, and an electric conductor for supplying power to the heating resistor, in which the heating resistor is composed of zirconium boride and oxygen. A thermal head comprising: 2. Claim 1 in which the heating resistor has an oxygen content of 0.005 (atomic ratio) or more of zirconium.
Thermal head described in section. 3. The thermal head according to claim 1, wherein the heating resistor has an oxygen content of 0.01 to 1.0 (atomic ratio) of zirconium. 4. The thermal head according to claims 1 to 3, wherein the heating resistor is covered with a silicon oxide thin film. 5 Claim 1 having a tantalum oxide protective film
The thermal head according to items 1 to 4. 6. The thermal head according to claims 1 to 4, which has a protective film of aluminum oxide. 7. The thermal head according to claims 1 to 4, which has a protective film of magnesium oxide. 8. A method for manufacturing a thermal head, characterized in that a heating resistor made of zirconium boride and oxygen is manufactured by electron beam evaporation. 9. The manufacturing method according to claim 8, in which electron beam evaporation is performed while introducing a gas containing oxygen. 10. The manufacturing method according to claim 8 or 9, wherein electron beam evaporation is performed while heating the substrate at 200°C to 500°C.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52160138A JPS598233B2 (en) | 1977-12-28 | 1977-12-28 | thermal head |
| US05/906,359 US4296309A (en) | 1977-05-19 | 1978-05-15 | Thermal head |
| DE19782821950 DE2821950A1 (en) | 1977-05-19 | 1978-05-19 | Head for thermal printing with stable resistance - obtd. by sputtering a metal boride resistance heating element onto a glazed substrate |
| US06/552,013 US4545881A (en) | 1977-05-19 | 1983-11-16 | Method for producing electro-thermal transducer |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52160138A JPS598233B2 (en) | 1977-12-28 | 1977-12-28 | thermal head |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5492267A JPS5492267A (en) | 1979-07-21 |
| JPS598233B2 true JPS598233B2 (en) | 1984-02-23 |
Family
ID=15708684
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52160138A Expired JPS598233B2 (en) | 1977-05-19 | 1977-12-28 | thermal head |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS598233B2 (en) |
-
1977
- 1977-12-28 JP JP52160138A patent/JPS598233B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5492267A (en) | 1979-07-21 |
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