JPH01298097A - Production of diamondlike carbon film - Google Patents
Production of diamondlike carbon filmInfo
- Publication number
- JPH01298097A JPH01298097A JP63128456A JP12845688A JPH01298097A JP H01298097 A JPH01298097 A JP H01298097A JP 63128456 A JP63128456 A JP 63128456A JP 12845688 A JP12845688 A JP 12845688A JP H01298097 A JPH01298097 A JP H01298097A
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- film
- carbon film
- diamond
- substrate
- high frequency
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Abstract
(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.
Description
【発明の詳細な説明】 [産業上の利用分野] 本発明は、ダイヤモンド状炭素膜の製造方法に関する。[Detailed description of the invention] [Industrial application field] The present invention relates to a method for manufacturing a diamond-like carbon film.
[従来の技術]
ダイヤモンドは、物質の中では最も硬度および熱伝導率
等に優れるので、その薄膜の応用が幅広く検討されてい
る。[Prior Art] Diamond has the highest hardness, thermal conductivity, etc. of all substances, and therefore its thin film applications are being widely studied.
ダイヤモンド状炭素膜の製造方法としては、従来より、
例えば、熱フイラメントCVD法(特開昭58−911
00号公報等)、マイクロ波プラズマCVD法(特公昭
61−3320公報等)などのCVD法による製造方法
が知られている。Conventionally, the manufacturing method of diamond-like carbon film is as follows.
For example, the hot filament CVD method (Japanese Patent Application Laid-Open No. 58-911
Manufacturing methods using CVD methods such as the microwave plasma CVD method (Japanese Patent Publication No. 61-3320, etc.) are known.
また、その他のダイヤモンド状炭素膜の製造方法として
は、黒鉛ターゲットをスパッタすることによるスパッタ
法(特公昭52−42159号公報、特開昭61−61
98号公報等)がある。In addition, as another method for producing a diamond-like carbon film, a sputtering method by sputtering a graphite target (Japanese Patent Publication No. 52-42159, Japanese Patent Application Laid-open No. 61-61
Publication No. 98, etc.).
[発明が解決しようとする課題]
上記CVD法は、一般に基体温度を800℃前後の高温
にする必要がある。したがって゛、得られるダイヤモン
ド状炭素膜の応用範囲は狭かった。[Problems to be Solved by the Invention] The above CVD method generally requires the substrate temperature to be as high as about 800°C. Therefore, the range of applications of the obtained diamond-like carbon film was narrow.
一方、スパッタ法は、基板温度が比較的低温でも成膜可
能であるが、成膜速度が遅く、かつ得られる膜中に水素
等のガスが不純物として残留してしまう傾向が強く、そ
の結晶性が低い等の欠点があった。On the other hand, the sputtering method allows film formation even when the substrate temperature is relatively low, but the film formation rate is slow and there is a strong tendency for gases such as hydrogen to remain as impurities in the resulting film, resulting in poor crystallinity. There were disadvantages such as low
本発明の目的は、基体温度が比較的低温であっても成膜
が可能であり、成膜速度が速く、不純物の混入が少なく
、結晶性の良好なダイヤモンド状炭素膜を製造できる方
法を提供することにある。An object of the present invention is to provide a method for producing a diamond-like carbon film that can be formed even when the substrate temperature is relatively low, has a fast film formation rate, contains few impurities, and has good crystallinity. It's about doing.
本発明は、ガス圧5×lO鴫〜5 X 1O−ITor
rの範囲内で水素ガスおよび希ガスから選択した一種以
上を含むガスにより、磁界中の黒鉛カソードをスパッタ
し、かつ基体に対して高周波バイアスを印加することを
特徴とするダイヤモンド炭素膜の製造方法である。The present invention has a gas pressure of 5 x 1O - 5 x 1O-ITor.
A method for producing a diamond carbon film, which comprises sputtering a graphite cathode in a magnetic field with a gas containing one or more selected from hydrogen gas and rare gas within the range of r, and applying a high frequency bias to the substrate. It is.
なお、ここでいう「ダイヤモンド状炭素膜」とは、ビッ
カース硬度で〜2000kg/mm2程度の硬度をもち
、1010ΩCm程度といった高い値の絶縁性をもった
、ダイヤモンド類似の性質を持つ膜である。The "diamond-like carbon film" referred to herein is a film having properties similar to diamond, having a Vickers hardness of about 2000 kg/mm2 and high insulation properties of about 1010 ΩCm.
本発明の製造方法においては、基体に対して適当な高周
波バイアスを印加するので、基体表面が活性化し、結合
状態の弱い、アモルファス相や二重結合を含んだ炭素お
よび膜中の水素等の不純物などが除去され、得られる膜
の結晶性が向上する。In the manufacturing method of the present invention, an appropriate high frequency bias is applied to the substrate, so that the surface of the substrate is activated and impurities such as weakly bonded amorphous phase and carbon containing double bonds and hydrogen in the film are removed. etc. are removed, and the crystallinity of the resulting film is improved.
なお、従来のスパッタ法においては、スパッタされた炭
素原子または分子のエネルギーだけにより、基体上に炭
素−炭素結合を形成していたので、得られる膜の結晶性
は悪く、二重結合を含ん −だ炭素などを十分
に除去できるようなエネルギーは付与されなかった。In addition, in the conventional sputtering method, carbon-carbon bonds are formed on the substrate only by the energy of sputtered carbon atoms or molecules, so the resulting film has poor crystallinity and does not contain double bonds. However, there was not enough energy provided to remove carbon and other substances.
本発明における基体に対する高周波バイアスの印加は1
00k Hz〜IGHz程度の高周波により行なえばよ
く、一般には13.56MHzの通常の高周波電源を用
いて印加すればよい。In the present invention, the application of high frequency bias to the substrate is 1
The application may be performed using a high frequency of approximately 00 kHz to IGHz, and generally a normal high frequency power source of 13.56 MHz may be used.
高周波バイアスの出力は、高周波バイアスを印加するこ
とによって発生する基体の自己バイアスの電圧が望まし
くは20〜250■、更に望ましくは50〜200vと
なるように印加する。その電圧が20Vよりも低い場合
には、高周波バイアスの印加による本発明の効果が認め
られないことがあり、また250vよりも高い場合には
、成膜中に基体温度が上昇し高温になってしまうので、
スパッタ法の利点(基体温度が比較的低温でも成膜可能
)を有しつつ良好な膜を得るという本発明の目的を達成
できないことがあり、かつ成膜速度が遅くなる。The output of the high frequency bias is applied so that the self-bias voltage of the substrate generated by applying the high frequency bias is preferably 20 to 250 V, more preferably 50 to 200 V. If the voltage is lower than 20V, the effect of the present invention due to the application of high frequency bias may not be recognized, and if it is higher than 250V, the substrate temperature will rise during film formation and become high temperature. Because I put it away,
The purpose of the present invention, which is to obtain a good film while having the advantage of the sputtering method (capable of forming a film even at a relatively low substrate temperature), may not be achieved, and the film formation rate becomes slow.
本発明の方法に用いるスパッタガスは、水素ガスまたは
希ガス(He、Ar、Ne等)を単独またはそれらの2
種以上を混合して用いたガスである。上記希ガスを混入
することで放電の安定および成膜速度の増加がみられる
。The sputtering gas used in the method of the present invention includes hydrogen gas or a rare gas (He, Ar, Ne, etc.) alone or in combination.
This gas is a mixture of more than one species. By mixing the above-mentioned rare gas, it is possible to stabilize the discharge and increase the film formation rate.
また、反応室内のガスの圧力は、ターゲット間距離、磁
界強度などにより、放電を安定させ高密度のプラズマ得
る点においての好適な値は異なってくるが、5 X l
O= 〜5 X 10−’ Torrの範囲内が望まし
く、I X 10’ 〜5 X 1O−2Torrの範
囲内が更に好ましい。In addition, the preferable value for the gas pressure in the reaction chamber in terms of stabilizing the discharge and obtaining high-density plasma varies depending on the distance between targets, magnetic field strength, etc.
The range of O= to 5 x 10-' Torr is desirable, and the range of I x 10' to 5 x 10-2 Torr is more preferable.
本発明の方法における磁界の強度は、300〜1000
エルステツドが望ましく、400〜600エルステツド
が更に望ましい。The strength of the magnetic field in the method of the present invention is 300 to 1000
A diameter of Oersted is desirable, and a range of 400 to 600 Oersted is more desirable.
本発明の方法における基体温度は、CVD法のように8
00℃程度の高温にする必要はなく200〜400℃程
度であればよい。The substrate temperature in the method of the present invention is 8
It is not necessary to set the temperature to a high temperature of about 00°C, but it may be about 200 to 400°C.
本発明の方法に用いることのできる装置は、反応室内が
減圧でき、スパッタ法を行なうことのできる手段(磁石
、直流電源等)と、基体に対して高周波バイアスを印加
可能な手段(高周波電源等)とを有する装置であればよ
い。Apparatus that can be used in the method of the present invention includes means that can reduce the pressure in the reaction chamber and perform sputtering (magnets, DC power supplies, etc.), and means that can apply high frequency bias to the substrate (high frequency power supplies, etc.). ).
第1図は、本発明の方法に用いることのできる対向スパ
ッタリング装置の一例を示す模式図である。FIG. 1 is a schematic diagram showing an example of a facing sputtering apparatus that can be used in the method of the present invention.
図中の1はチャンバー、2はグラファイトターゲット、
3は直流電源、4は基体、5は基体ホルダー、6は高周
波電源、7はガス導入口、8はガス排気口、9は永久磁
石を内蔵したターゲットホルダーであり、その永久磁石
から生じる磁界は図中の矢印の方向に印加されている。In the figure, 1 is a chamber, 2 is a graphite target,
3 is a DC power source, 4 is a substrate, 5 is a substrate holder, 6 is a high frequency power source, 7 is a gas inlet, 8 is a gas exhaust port, 9 is a target holder with a built-in permanent magnet, and the magnetic field generated by the permanent magnet is The voltage is applied in the direction of the arrow in the figure.
この装置においては、ガス導入ロアより導入されたスパ
ッタガスを放電電流により解離し、プラズマ化すると、
そのプラズマによりグラファイトターゲット2がスパッ
タされ、高周波電源6により高周波バイアスの印加され
る。そして、基体ホルダー5上の基体4の上にダイヤモ
ンド膜が形成される。なお、チャンバー内は排気系(不
図示)により排気口8より排気され、所定の圧力に調節
される。In this device, when the sputtering gas introduced from the gas introduction lower is dissociated by a discharge current and turned into plasma,
The graphite target 2 is sputtered by the plasma, and a high frequency bias is applied by the high frequency power source 6. Then, a diamond film is formed on the substrate 4 on the substrate holder 5. Note that the inside of the chamber is evacuated through an exhaust port 8 by an exhaust system (not shown), and the pressure is adjusted to a predetermined pressure.
上記装置における代表的な放電特性(放電電流とターゲ
ット電圧との関係)を第2図に示す。Typical discharge characteristics (relationship between discharge current and target voltage) in the above device are shown in FIG.
なお、本発明の方法を実施する為の装置は、上述の装置
に限られるものではない。例えば上述の装置においては
、ターゲットを2個用いているが、1個または3個以上
用いてもかまわない。また、磁石には永久磁石を用いて
いるが、電磁石でもかまわない。Note that the apparatus for carrying out the method of the present invention is not limited to the above-mentioned apparatus. For example, in the above-mentioned apparatus, two targets are used, but one or three or more targets may be used. Further, although a permanent magnet is used as the magnet, an electromagnet may also be used.
以下、実施例によって本発明を具体的に説明する。 Hereinafter, the present invention will be specifically explained with reference to Examples.
実施例1
第1図に示した対向スパッタリング装置を用い、以下の
条件にて本発明のダイヤモンド状炭素膜の製造方法を実
施した。Example 1 Using the facing sputtering apparatus shown in FIG. 1, the method for manufacturing a diamond-like carbon film of the present invention was carried out under the following conditions.
基体4にはシリコン基板を用い、不図示のヒーターを用
いて200℃に加熱した。スパッタガスとして水素ガス
を50 SCCMで導入し、チャンバー内の圧力を2
X 1O−3Torrとした。磁場強度は500エルス
テツド、ターゲット電圧はlkVで、放電電流は0.5
Aとした。基体4への高周波バイアスは自己バイアスが
5QVとなるように印加した。このとき高周波の出力は
20Wであった。なお、その高周波の周波数は13.5
6M Hzとした。A silicon substrate was used as the base 4 and heated to 200° C. using a heater (not shown). Hydrogen gas was introduced as sputtering gas at 50 SCCM, and the pressure inside the chamber was reduced to 2.
X 1O-3 Torr. The magnetic field strength was 500 oersted, the target voltage was lkV, and the discharge current was 0.5
I gave it an A. A high-frequency bias was applied to the substrate 4 so that the self-bias was 5QV. At this time, the high frequency output was 20W. In addition, the frequency of the high frequency is 13.5
The frequency was set to 6 MHz.
以上のようにして得られた炭素膜のX線回折により、ダ
イヤモンド結晶が確認された。Diamond crystals were confirmed by X-ray diffraction of the carbon film obtained as described above.
そのダイヤモンド状炭素膜はビッカース硬度が6000
kg/ mm2と硬く、走査型電子線顕微鏡観察によれ
ば平滑な膜であった。また、IR測測定よれば、C−H
吸収は確認されたが弱いものであった。成膜速度は4胛
/時であった。The diamond-like carbon film has a Vickers hardness of 6000.
The film had a hardness of kg/mm2 and was smooth according to scanning electron microscopy. Also, according to IR measurement, C-H
Absorption was confirmed, but it was weak. The film formation rate was 4 coats/hour.
実施例2
スパッタガスとして水素ガス、アルゴンガスをそれぞれ
25 SCCMで導入し、チャンバー内の圧力を2 X
1O−3Torrとし、ターゲット電圧を900vと
して放電電流を0.5Aとした以外は実施例1と同様に
して成膜を行なった。Example 2 Hydrogen gas and argon gas were introduced as sputtering gases at 25 SCCM each, and the pressure inside the chamber was set to 2
Film formation was performed in the same manner as in Example 1, except that the temperature was 10-3 Torr, the target voltage was 900 V, and the discharge current was 0.5 A.
以上のようにして得られた炭素膜のX線回折により、ダ
イヤモンド結晶が確認された。Diamond crystals were confirmed by X-ray diffraction of the carbon film obtained as described above.
そのダイヤモンド状炭素膜はビッカース硬度が6000
kg/mm2と硬く、走査型電子線顕微鏡観察によれば
平滑な膜であった。また、IR測測定よれば、Hの混入
はほとんどみられなかった。成膜速度は6)+111/
時であった。The diamond-like carbon film has a Vickers hardness of 6000.
The film had a hardness of kg/mm2 and was smooth when observed using a scanning electron beam microscope. Further, according to IR measurement, almost no H was observed. The film formation rate is 6) + 111/
It was time.
実施例3
排気バルブ(不図示)を調整して圧力を5×1O−3T
orrとし、ターゲット電圧を700Vとして放電電流
を0.5Aとした以外は実施例2と同様にして成膜を行
なった。Example 3 Adjust the exhaust valve (not shown) to reduce the pressure to 5×1O-3T
The film was formed in the same manner as in Example 2 except that the target voltage was 700 V and the discharge current was 0.5 A.
以上のようにして得られた炭素膜のX線回折により、ダ
イヤモンド結晶が確認された。Diamond crystals were confirmed by X-ray diffraction of the carbon film obtained as described above.
そのダイヤモンド状炭素膜はビッカース硬度が5800
kg/ mm2と硬く、走査型電子線顕微鏡観察によれ
ば平滑な膜であった。また、IR測測定よれば、Hの混
入はほとんどみられなかった。成膜速度は4μffi/
時であった。The diamond-like carbon film has a Vickers hardness of 5800.
The film had a hardness of kg/mm2 and was smooth according to scanning electron microscopy. Further, according to IR measurements, almost no H was observed. The film formation rate is 4μffi/
It was time.
実施例4
高周波バイアスを自己バイアスが100 Vとなるよう
に調整して印加した以外は実施例2とと同様、にして成
膜を行なった。Example 4 Film formation was performed in the same manner as in Example 2, except that the high frequency bias was adjusted and applied so that the self-bias was 100 V.
以上のようにして得られた炭素膜のX線回折により、ダ
イヤモンド結晶が確認された。Diamond crystals were confirmed by X-ray diffraction of the carbon film obtained as described above.
そのダイヤモンド状炭素膜はビッカース硬度が9000
kg7mm2と硬く、走査型電子線顕微鏡観察によれば
平滑な膜であった。また、IR測測定よれば、Hの混入
はほとんどみられなかった。成膜速度は4麟/時であっ
た。The diamond-like carbon film has a Vickers hardness of 9000
The film was hard, weighing 7 mm2, and was smooth when observed using a scanning electron microscope. Further, according to IR measurement, almost no H was observed. The film formation rate was 4 in/hour.
比較例1
排気バルブ(不図示)を調整して圧力をI Torrと
した以外は実施例2と同様にして成膜を行なった。その
際には放電が不安定であり、グラファイトのターゲット
上で局所的な放電が発生した。Comparative Example 1 Film formation was performed in the same manner as in Example 2, except that the exhaust valve (not shown) was adjusted to set the pressure to I Torr. At that time, the discharge was unstable and localized discharge occurred on the graphite target.
このとき基体上には、スス上の析出物しか得られなかっ
た。At this time, only soot deposits were obtained on the substrate.
比較例2
排気バルブ(不図示)を調整して圧力をI×10” T
orrとした以外は実施例2と同様にして成膜を行なっ
た。その際には放電が弱く、十分な放電電流が得られな
かった。Comparative Example 2 Adjust the exhaust valve (not shown) to reduce the pressure to I×10”T
Film formation was performed in the same manner as in Example 2, except that orr was used. At that time, the discharge was weak and a sufficient discharge current could not be obtained.
このとき基体上には、はとんど析出物はみられなかった
。At this time, almost no precipitates were observed on the substrate.
比較例3
高周波バイアスを印加しない以外は実施例2と同様にし
て成膜を行なった。Comparative Example 3 Film formation was carried out in the same manner as in Example 2 except that no high frequency bias was applied.
以上のようにして得られた炭素膜のX線回折では、ダイ
ヤモンド結晶は認められなかった。No diamond crystals were observed in X-ray diffraction of the carbon film obtained as described above.
その炭素膜はビッカース硬度は3000kg/ mm2
と低く、IR測測定C−Hの強い吸収がみられた。The Vickers hardness of the carbon film is 3000 kg/mm2
A strong absorption of C-H was observed in the IR measurement.
比較例4
[発明の効果]
以上説明したように、スパッタ法に基づく本発明の方法
は、適当なガス圧のスパッタガスにより、磁界中の黒鉛
カソードをスパッタし、かつ基体に対して高周波バイア
スを印加するので、基体温度が比較的低温であっても成
膜が可能であり、成膜速度が速く、かつ不純物の混入の
少なく、結晶性の良好なダイヤモンド状炭素膜を製造で
きる。Comparative Example 4 [Effects of the Invention] As explained above, the method of the present invention based on the sputtering method sputters a graphite cathode in a magnetic field with a sputtering gas at an appropriate gas pressure, and also applies a high frequency bias to the substrate. Since the application is applied, film formation is possible even when the substrate temperature is relatively low, and a diamond-like carbon film with high film formation rate, less contamination of impurities, and good crystallinity can be manufactured.
第1図は、本発明の方法に用いることのできる装置の一
例を示す模式図、
第2図は、対向スパッタリング装置における代表的な放
電特性を示す図である。
1・・・・・・チャンバーFIG. 1 is a schematic diagram showing an example of an apparatus that can be used in the method of the present invention, and FIG. 2 is a diagram showing typical discharge characteristics in a facing sputtering apparatus. 1... Chamber
Claims (1)
の範囲内で水素ガスおよび希ガスから選択した一種以上
を含むガスにより、磁界中の黒鉛カソードをスパッタし
、かつ基体に対して高周波バイアスを印加することを特
徴とするダイヤモンド状炭素膜の製造方法。Gas pressure 5×10^-^4 to 5×10^-^1 Torr
A method for producing a diamond-like carbon film, which comprises sputtering a graphite cathode in a magnetic field with a gas containing one or more selected from hydrogen gas and rare gases within the range of 1 to 2, and applying a high frequency bias to the substrate. .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63128456A JPH01298097A (en) | 1988-05-27 | 1988-05-27 | Production of diamondlike carbon film |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63128456A JPH01298097A (en) | 1988-05-27 | 1988-05-27 | Production of diamondlike carbon film |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH01298097A true JPH01298097A (en) | 1989-12-01 |
Family
ID=14985158
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63128456A Pending JPH01298097A (en) | 1988-05-27 | 1988-05-27 | Production of diamondlike carbon film |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH01298097A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5607560A (en) * | 1993-03-25 | 1997-03-04 | Canon Kabushiki Kaisha | Diamond crystal forming method |
-
1988
- 1988-05-27 JP JP63128456A patent/JPH01298097A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US5607560A (en) * | 1993-03-25 | 1997-03-04 | Canon Kabushiki Kaisha | Diamond crystal forming method |
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