JPS6247472A - Formation of cubic boron nitride film - Google Patents

Formation of cubic boron nitride film

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Publication number
JPS6247472A
JPS6247472A JP18582785A JP18582785A JPS6247472A JP S6247472 A JPS6247472 A JP S6247472A JP 18582785 A JP18582785 A JP 18582785A JP 18582785 A JP18582785 A JP 18582785A JP S6247472 A JPS6247472 A JP S6247472A
Authority
JP
Japan
Prior art keywords
boron nitride
cubic boron
nitride film
density plasma
bias voltage
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.)
Granted
Application number
JP18582785A
Other languages
Japanese (ja)
Other versions
JPH031377B2 (en
Inventor
Kazuhiro Watanabe
一弘 渡辺
Ichiro Tanaka
一郎 田中
Kazuya Saito
一也 斉藤
Konosuke Inagawa
幸之助 稲川
Akio Ito
昭夫 伊藤
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.)
Ulvac Inc
Original Assignee
Ulvac Inc
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 Ulvac Inc filed Critical Ulvac Inc
Priority to JP18582785A priority Critical patent/JPS6247472A/en
Publication of JPS6247472A publication Critical patent/JPS6247472A/en
Publication of JPH031377B2 publication Critical patent/JPH031377B2/ja
Granted legal-status Critical Current

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Abstract

PURPOSE:To easily obtain a cubic boron nitride film having a large area and satisfactory crystallizability by utilizing high density plasma and high frequency bias during reaction and vapor deposition by electric discharge with a hollow cathode. CONSTITUTION:DC or AC bias voltage is applied to a reactive gas introducing nozzle 5 from a power source 8 to generate high density plasma. High frequency voltage 9 is then applied to a body 3 to be processed to form a high frequency electric field around the body 3. By the electric field, bias voltage effective on the high density plasma is applied to the body 3. Thus, a cubic boron nitride film having a large area is obtd. at a high rate of deposition.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、中空陰極放電を利用した反応蒸着による立方
晶チッ化ホウ素膜の形成方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a method for forming a cubic boron nitride film by reactive vapor deposition using hollow cathode discharge.

[従来の技4IFI] 従来、立方晶チッ化ホウ素(C−BN)は、高温高圧法
や気相法を用いて合成することが試みられいる。高温高
圧法では、完全性の高い結晶を得ることができる。また
、気相法では、イオンビームスパッタ法、イオン注入と
真空蒸着とを組合せた方法および活性化反応蒸着法を用
いて立方晶チッ化ホCり素を作ることが試みられている
[Conventional Technique 4IFI] Conventionally, attempts have been made to synthesize cubic boron nitride (C-BN) using a high temperature/high pressure method or a gas phase method. The high-temperature, high-pressure method can yield highly perfect crystals. Furthermore, in the vapor phase method, attempts have been made to produce cubic phosphorus nitride using an ion beam sputtering method, a method combining ion implantation and vacuum evaporation, and an activated reaction evaporation method.

一方、中空陰極放電を利用した反応蒸着による化合物膜
の形成方法として、先に特願昭60−43617号(特
開昭 −号公報)において中空陰極放電によって生じる
プラズマ中に人聞に存在する電子の一部を電界により反
応ガス導入口に引き込み、反応ガスを活性化して化成蒸
着における反応性を高める方法を提案した。この方法に
より、DCおよびR「グロー放電に比較して一桁以上大
きな電流を青ることができ、しかも反応ガス導入口付近
に電流が集中するため、プラズマ密度は飛躍的に地大す
ることが認められた。
On the other hand, as a method for forming a compound film by reactive vapor deposition using hollow cathode discharge, Japanese Patent Application No. 60-43617 (Japanese Unexamined Patent Application Publication No. 1983-1989) previously described the method of forming a compound film by using the electrons present in the plasma generated by hollow cathode discharge. We proposed a method to activate the reactive gas by drawing a part of it into the reactive gas inlet using an electric field to increase the reactivity in chemical vapor deposition. With this method, it is possible to generate a current that is more than an order of magnitude larger than that of DC and R glow discharges, and because the current is concentrated near the reactant gas inlet, the plasma density can dramatically increase. Admitted.

[発明が解決しようとするt1題点] ところで、高温高圧法で立方晶チッ化ホウ素(c−BN
)を形成する場合には、完全性の高い結晶を得ることが
できるが、大ぎさや形状の制御が困難であり、製造コス
・トも高くつく。一方、イオン注入と真空蒸着とを組合
せた方法を用いて作られた膜には六方晶チッ化ホウ素(
h−BN)相が混在□しでおり、また装置が大かがりの
割りには処理面積が小さいため、生産性が悪いだけでな
く再現性の点でも問題がある。イオンビームスパッタ法
においては、プラズマ密度が低いため、速い析゛出速度
で大面積のコーティングはできない。また活性化反応蒸
着法による立方晶チッ化ホウ素の形成については、従来
詳細な報告がなされてない。
[Problem t1 to be solved by the invention] By the way, cubic boron nitride (c-BN
), it is possible to obtain a highly perfect crystal, but it is difficult to control the size and shape, and the manufacturing cost is also high. On the other hand, films made using a method that combines ion implantation and vacuum deposition contain hexagonal boron nitride (
Since the h-BN) phase is mixed, and the processing area is small considering the large size of the device, there are problems not only in productivity but also in reproducibility. In the ion beam sputtering method, since the plasma density is low, it is not possible to coat a large area at a high deposition rate. Furthermore, there have been no detailed reports regarding the formation of cubic boron nitride by activated reactive vapor deposition.

イオンを加速するために、メツシュ状の電極を用いるこ
とがあるが、立方晶チッ化ホウ素は絶縁体であるため、
メツシュ状の電極に絶縁体が付着し、それによりバイア
ス電圧が変動し、コーテイング膜の再現性を得ることは
困難である。またメツシュ状の電極にイオン化した原子
の一部が奪われるために、イオンの基板への入rAmが
低下し、このため生成したプラズマを有効に使うことが
できなくなる。さらに、メツシュ状の電極に印加される
電力が犬さくなる場合には、メツシュ状の電極自体がイ
オンによってスパッタされ、膜中に含まれる不純物汚染
の原因となる。また、立方晶チッ化ホウ素股を形成寸べ
ぎ被処理物にDCバイアスを印加する場合には、100
人程度[3N膜が形成されると、基板電流は流れなくな
る。
A mesh-like electrode is sometimes used to accelerate ions, but since cubic boron nitride is an insulator,
An insulator adheres to the mesh-like electrode, which causes the bias voltage to fluctuate, making it difficult to obtain reproducibility of the coating film. Furthermore, since some of the ionized atoms are taken away by the mesh-like electrode, the amount of ions rAm entering the substrate decreases, making it impossible to use the generated plasma effectively. Furthermore, if the electric power applied to the mesh-like electrode becomes too low, the mesh-like electrode itself will be sputtered by ions, causing contamination with impurities contained in the film. In addition, when applying a DC bias to the workpiece for forming cubic boron nitride, 100
Once the 3N film is formed, no substrate current will flow.

そこで、本発明の目的は、先に提案した中空陰極放電を
利用した反応蒸着による化合物膜の形成方法を応用して
量産性に優れ、結晶性のよい立方晶チッ化ホウ素膜の形
成方法を提供することにある。
Therefore, an object of the present invention is to provide a method for forming a cubic boron nitride film with excellent mass productivity and good crystallinity by applying the previously proposed method for forming a compound film by reactive vapor deposition using hollow cathode discharge. It's about doing.

U問題点を解決するための手段] 上記の目的を達成するために、本発明による立方晶チッ
化ホウ素膜の形成方法は、反応ガス導入ノズルに直流ま
たは交流のバイアス電圧を印加して高密度のプラズマを
生成し、立方晶チッ化ホウ素膜を形成すべき被処理物に
高周波電圧を印加して上記被処理物の表面近傍に高周波
電界を形成し、蒸発源および反応ガス導入ノズル前面の
上記高密度プラズマに対して有効なバイアス電圧が上記
被処理物にかかるようにしたことを特徴としている。
Means for Solving Problem U] In order to achieve the above object, the method for forming a cubic boron nitride film according to the present invention applies a DC or AC bias voltage to the reaction gas introduction nozzle to form a high-density A high-frequency voltage is applied to the object to be processed to form a cubic boron nitride film, a high-frequency electric field is formed near the surface of the object, and the It is characterized in that a bias voltage effective for high-density plasma is applied to the object to be processed.

反応ガス導入ノズルに印加される正のバイアス電圧は、
直流または交流電源から供給され得る。
The positive bias voltage applied to the reaction gas introduction nozzle is
It can be supplied from DC or AC power.

また反応ガスとしてはN2またはNH3を用いることが
できる。
Further, N2 or NH3 can be used as the reaction gas.

[作    用] 本発明による立方晶チッ化ホウ素膜の形成方法では、立
方晶チッ化ホウ素膜を形成すべき被処理物に印加される
高周波バイアス電圧により、イオン衝撃に必要である有
効なイオンエネルギを得ることができ、これにより、反
応ガス導入ノズルに直流または交流のバイアス電圧を印
加することによって生成された高密度のプラズマ中に大
ωに存在するイオンは、被処理物に有効に入射し、被処
理物上に立方晶チッ化ホウ素膜が効果的に形成され得る
[Function] In the method for forming a cubic boron nitride film according to the present invention, the effective ion energy necessary for ion bombardment is generated by the high-frequency bias voltage applied to the workpiece on which the cubic boron nitride film is to be formed. As a result, ions existing at large ω in the high-density plasma generated by applying a DC or AC bias voltage to the reaction gas introduction nozzle can effectively enter the workpiece. , a cubic boron nitride film can be effectively formed on the workpiece.

[実  施  例] 以下、添附図面を参照して本発明の実施例について説明
する。
[Example] Hereinafter, an example of the present invention will be described with reference to the accompanying drawings.

第1図には、本発明による立方晶チッ化ホウ素膜の形成
方法を実施している装置の一例を概略的に示し、真空容
31内には、蒸発源であるホウ素の入った水冷銅製ハー
ス2と、この水冷銅製ハース2に対向した立方晶チッ化
ホウmlを形成すべき被処pl+物3と、中空陰極型電
子銃4と、N2よたはNH3を真空容鼎1内に導入する
反応ガス導入ノズル5と、被処理物3に対するヒータ6
とが配置されている。水冷銅製ハース2と中空l!2h
型電子銃4との間にはそれらの間に中空熱陰極放電を起
すための直流電源7が図示した極性で接続されている。
FIG. 1 schematically shows an example of an apparatus implementing the method for forming a cubic boron nitride film according to the present invention. 2, a material 3 to be treated to form cubic boron nitride ml facing the water-cooled copper hearth 2, a hollow cathode electron gun 4, and N2 or NH3 introduced into the vacuum volume 1. Reaction gas introduction nozzle 5 and heater 6 for the object to be treated 3
and are arranged. Water-cooled copper hearth 2 and hollow l! 2h
A DC power source 7 is connected to the type electron gun 4 with the polarity shown in the figure for generating a hollow hot cathode discharge therebetween.

直流または交流電源8(:t、中空陰(参放電空聞内の
電子の一部を反応ガス導入ノズル5に引き込む電界を発
生するため反応ガス導入ノズル5と中空陰極型電子銃4
との間に接続され、直流正または交流の数十〜数百ボル
トの電圧を印加する。また、被処理物3には各辺結合型
マツチング要素を介して高周波電−源9が接続されてい
る。
DC or AC power supply 8 (:t, hollow cathode) In order to generate an electric field that draws some of the electrons in the discharge space into the reaction gas introduction nozzle 5, the reaction gas introduction nozzle 5 and the hollow cathode type electron gun 4 are connected.
A positive DC or AC voltage of several tens to hundreds of volts is applied. Further, a high frequency power source 9 is connected to the workpiece 3 via a matching element of each side coupling type.

水冷銅製ハース2と中空陰極型電子銃4との間に発生さ
れる中空熱陰極放電は、低電圧、大電流であり、また、
直流または交流電源8によって反応ガス導入ノズル5と
中空陰極型電子銃4との間に印加される正のバイアス電
圧により、中空陰極放電空間内の電子の一部は反応ガス
導入ノズル5に引き込まれ、それにより電子と反応ガス
分子との間で衝突が起り、高密度なM電状態となる。そ
の結束、反応ガスは一部イオン化されると共に中性の励
起状態に活性化される。
The hollow hot cathode discharge generated between the water-cooled copper hearth 2 and the hollow cathode electron gun 4 has a low voltage and a large current.
A part of the electrons in the hollow cathode discharge space are drawn into the reaction gas introduction nozzle 5 by a positive bias voltage applied between the reaction gas introduction nozzle 5 and the hollow cathode type electron gun 4 by the DC or AC power supply 8. , which causes collisions between electrons and reactive gas molecules, resulting in a high-density M electric state. Due to its binding, the reactant gas is partially ionized and activated to a neutral excited state.

高周波電源9によって、被処理物3に高周波電圧を印加
することにより、被処理物3の近傍に高周波電界が発生
され、水冷銅製ハース2の前面および反応ガス導入ノズ
ル5の前面の高密度プラズマに対して有効なバイアス電
圧が被処理物3に掛るようにされる。この高周波バイア
ス電圧によって、高密度のプラズマ中に条苗に存在する
イオンは被処理物3に有効に入射され得る。
By applying a high-frequency voltage to the workpiece 3 by the high-frequency power supply 9, a high-frequency electric field is generated near the workpiece 3, and a high-density plasma is generated in the front surface of the water-cooled copper hearth 2 and the front surface of the reactive gas introduction nozzle 5. An effective bias voltage is applied to the object 3 to be processed. By this high-frequency bias voltage, ions present in the seedlings in the high-density plasma can be effectively incident on the object 3 to be treated.

次に、図示装置を用いて本発明の方法を実施した具体例
を例示する。
Next, a specific example of implementing the method of the present invention using the illustrated apparatus will be illustrated.

蒸着条件として中空陰極型電子銃4を通してアルゴンガ
スを圧力0.13Paで供給し、反応ガス導入ノズル5
にチッ素ガスを圧力0.05 paで導入し、中空熱陰
極tIl電を30V 、  150Δに設定し、析出速
度を005μm/m i nとし、直流または交流電源
8によって反応ガス導入ノズル5に印加される正のバイ
アス電圧を80V、2△とし、被処理物3に印加する高
周波電力を80Wとし、被処理物3として石英、シリコ
ンウェハおよびMo  (モリブデン)基板を使用し、
その温度を500℃に設定し、基板上に立方晶チッ化ホ ウ素膜を形成した。こうして形成した立方晶チッ化ホウ
素膜の赤外線吸収スペクトルを第2図に示す。
As a deposition condition, argon gas is supplied at a pressure of 0.13 Pa through the hollow cathode electron gun 4, and the reaction gas introduction nozzle 5
Nitrogen gas was introduced at a pressure of 0.05 pa, the hollow hot cathode voltage was set to 30 V and 150 Δ, the deposition rate was 0.05 μm/min, and the voltage was applied to the reaction gas introduction nozzle 5 by a DC or AC power source 8. The positive bias voltage applied was 80V, 2Δ, the high frequency power applied to the object 3 to be processed was 80W, and the object 3 to be processed was quartz, a silicon wafer, and a Mo (molybdenum) substrate.
The temperature was set at 500° C., and a cubic boron nitride film was formed on the substrate. FIG. 2 shows the infrared absorption spectrum of the cubic boron nitride film thus formed.

第2図のグラフから認られるように、C−BN固有の1
045cs−1の吸収が示されており、1350cm−
1750crm−’付近のh = [3Nの吸収は観祭
されない。
As seen from the graph in Figure 2, the C-BN-specific 1
The absorption of 045cs-1 is shown and is 1350cm-
The absorption of h = [3N around 1750 crm-' is not observed.

また、電子線回折によって求めた立方晶チッ化ホウ素膜
の格子面間隔とΔSTM回折(X線回折)データカード
との比較をF表に示す。
Further, Table F shows a comparison between the lattice spacing of the cubic boron nitride film determined by electron beam diffraction and the ΔSTM diffraction (X-ray diffraction) data card.

上記の表から、電子線回折によって求めた立方晶チッ化
ホウ素膜の格子面間隔は、ASTM回折(X線回折)デ
ータカードと一致していることがわかる。得られた膜の
組成はX線マイクロアナライザによると、N/B=1で
あった。
From the above table, it can be seen that the lattice spacing of the cubic boron nitride film determined by electron beam diffraction is consistent with the ASTM diffraction (X-ray diffraction) data card. The composition of the obtained film was determined by an X-ray microanalyzer to be N/B=1.

「発明の効果」 以上説明してきたように、本発明の方法によれば、中空
陰極放電を利用した反応蒸着において高密度プラズマと
高周波バイアスとを用いることによって結晶性のよい立
方晶チッ化ホウ素を被処理物に対して速い析出速度でし
かも大きな面積に容易に成膜することができる。従って
、本発明の方法は、切削工具等に被覆してズ1ωを伸づ
のに応用したり、高い電気絶縁性および高い熱伝導性を
利用して電子材料等にも応用され17る。
"Effects of the Invention" As explained above, according to the method of the present invention, cubic boron nitride with good crystallinity is produced by using high-density plasma and high-frequency bias in reactive vapor deposition using hollow cathode discharge. A film can be easily formed on a large area at a high deposition rate relative to the object to be processed. Therefore, the method of the present invention can be applied to coat cutting tools and the like to extend the gap 1ω, and can also be applied to electronic materials and the like by taking advantage of its high electrical insulation and high thermal conductivity.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明による方法を実施している中空陰極放電
を利用した反応蒸着装置の一例を示づ概略線図、第2図
は第1図の装置を用いて形成した立方晶チッ化ホウ素膜
の赤外線吸収スペクトルを示すグラフである。 図中、1:真空容器、2:蒸発源、3:立方晶チッ化ホ
ウ素膜を形成づ−べさ被処理物、4:中空陰極型電子銃
、5:反応ガス導入ノズル、6:ヒータ、7:直流電源
、8:直流または交流電源、9:高周波電源。 第1図 第2図
Fig. 1 is a schematic diagram showing an example of a reactive vapor deposition apparatus using hollow cathode discharge in which the method according to the present invention is carried out, and Fig. 2 shows cubic boron nitride formed using the apparatus of Fig. 1. It is a graph showing an infrared absorption spectrum of a film. In the figure, 1: vacuum container, 2: evaporation source, 3: object to be treated on which a cubic boron nitride film is to be formed, 4: hollow cathode electron gun, 5: reaction gas introduction nozzle, 6: heater, 7: DC power supply, 8: DC or AC power supply, 9: High frequency power supply. Figure 1 Figure 2

Claims (1)

【特許請求の範囲】[Claims] 中空陰極放電を利用した反応蒸着による立方晶チッ化ホ
ウ素膜の形成方法において、反応ガス導入ノズルに直流
または交流のバイアス電圧を印加して高密度のプラズマ
を生成し、立方晶チッ化ホウ素膜を形成すべき被処理物
に高周波電圧を印加して上記被処理物の表面近傍に高周
波電界を形成し、蒸発源および反応ガス導入ノズル前面
の上記高密度プラズマに対して有効なバイアス電圧が上
記被処理物にかかるようにしたことを特徴とする立方晶
チッ化ホウ素膜の形成方法。
In the method of forming a cubic boron nitride film by reactive vapor deposition using hollow cathode discharge, a direct current or alternating current bias voltage is applied to the reaction gas introduction nozzle to generate high-density plasma to form a cubic boron nitride film. A high-frequency electric field is formed near the surface of the object to be processed by applying a high-frequency voltage to the object to be processed, and a bias voltage effective for the high-density plasma in front of the evaporation source and the reaction gas introduction nozzle is applied to the object. A method for forming a cubic boron nitride film, characterized in that the film is coated on a processed material.
JP18582785A 1985-08-26 1985-08-26 Formation of cubic boron nitride film Granted JPS6247472A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18582785A JPS6247472A (en) 1985-08-26 1985-08-26 Formation of cubic boron nitride film

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18582785A JPS6247472A (en) 1985-08-26 1985-08-26 Formation of cubic boron nitride film

Publications (2)

Publication Number Publication Date
JPS6247472A true JPS6247472A (en) 1987-03-02
JPH031377B2 JPH031377B2 (en) 1991-01-10

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP18582785A Granted JPS6247472A (en) 1985-08-26 1985-08-26 Formation of cubic boron nitride film

Country Status (1)

Country Link
JP (1) JPS6247472A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH01116070A (en) * 1987-10-29 1989-05-09 Internatl Business Mach Corp <Ibm> Sputtering apparatus
US4941430A (en) * 1987-05-01 1990-07-17 Nihon Sinku Gijutsu Kabusiki Kaisha Apparatus for forming reactive deposition film
US5277939A (en) * 1987-02-10 1994-01-11 Semiconductor Energy Laboratory Co., Ltd. ECR CVD method for forming BN films
US5629053A (en) * 1990-04-06 1997-05-13 Siemens Aktiengesellschaft Method for manufacturing microcrystalline cubic boron-nitride-layers

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5277939A (en) * 1987-02-10 1994-01-11 Semiconductor Energy Laboratory Co., Ltd. ECR CVD method for forming BN films
US4941430A (en) * 1987-05-01 1990-07-17 Nihon Sinku Gijutsu Kabusiki Kaisha Apparatus for forming reactive deposition film
JPH01116070A (en) * 1987-10-29 1989-05-09 Internatl Business Mach Corp <Ibm> Sputtering apparatus
US5629053A (en) * 1990-04-06 1997-05-13 Siemens Aktiengesellschaft Method for manufacturing microcrystalline cubic boron-nitride-layers

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