JPH049465A - Method and device for controlling dc potential in thin film forming device - Google Patents
Method and device for controlling dc potential in thin film forming deviceInfo
- Publication number
- JPH049465A JPH049465A JP11015490A JP11015490A JPH049465A JP H049465 A JPH049465 A JP H049465A JP 11015490 A JP11015490 A JP 11015490A JP 11015490 A JP11015490 A JP 11015490A JP H049465 A JPH049465 A JP H049465A
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- 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]
本発明は高周波グロー放電を利用する薄膜処理技術に係
わり、特に高周波電源を用い、静電結合型放電電極及び
、又は電極上の処理対象物表面に発生する直流電位(セ
ルフバイアス)を所望する値に成る様、強制的に制御し
薄膜形成又は薄膜処理を行う方法および装置に関するも
のである。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a thin film processing technology using high frequency glow discharge, and in particular, uses a high frequency power source to process a capacitively coupled discharge electrode and/or an object to be processed on the electrode. The present invention relates to a method and apparatus for forming or processing a thin film by forcibly controlling the direct current potential (self-bias) generated on the surface to a desired value.
なお、上記、高周波グロー放電における直流電位(セル
フバイアス)は、電気絶縁性基板や電気絶縁性薄膜の堆
積又はエツチング(食刻)、アッシング(灰化)等の薄
膜処理を実施する際にグロー放電プラズマ中のイオンを
処理対象物表面に対し加速するのに必要となるもので、
近年の高機能薄膜デバイスの要求に対して、処理対象物
表面の電位制御の重要性が増している。Note that the DC potential (self-bias) in the high-frequency glow discharge mentioned above is the direct current potential (self-bias) in the glow discharge when performing thin film processing such as deposition, etching, and ashing of electrically insulating substrates and electrically insulating thin films. It is necessary to accelerate the ions in the plasma to the surface of the object to be processed.
In response to the recent demands for high-performance thin film devices, the importance of controlling the potential on the surface of the processing object is increasing.
[従来技術]
第1の従来技術としては、電気絶縁性基板や電気絶縁性
薄膜の堆積又はエツチング、アッシング等の薄膜処理に
は、高周波電源を用い、静電結合型放電電極及び、又は
電極上の処理対象物表面に発生する直流電位の制御を高
周波電源の出力電力(進行波電力)の調整で行っていた
。[Prior Art] A first conventional technology uses a high frequency power source for thin film processing such as deposition, etching, and ashing of electrically insulating substrates and electrically insulating thin films, The DC potential generated on the surface of the object to be processed is controlled by adjusting the output power (travelling wave power) of the high frequency power source.
本発明の目的に最も近い第2の従来技術として、特開平
1−180970号公報に記載されているように、高周
波電極に高周波をカットし直流電位のみを供給する高周
波フィルタを介し、DC(直流)電源に接続し、このD
C電源の出力電圧の調整で静電結合型放電電極及び電極
上の処理対象物表面に発生する直流電位を所望する値に
制御する技術がある。As a second prior art technique that is closest to the object of the present invention, as described in Japanese Unexamined Patent Publication No. 1-180970, a DC (direct current ) Connect to the power supply and connect this D
There is a technique for controlling the DC potential generated on the capacitively coupled discharge electrode and the surface of the object to be processed on the electrode to a desired value by adjusting the output voltage of the C power source.
[発明が解決しようとする課題]
日本に割当てられた工業用周波数で、グロー放電プラズ
マの生成に適した周波数は13.560MHz、27.
120MHz、40.68MHzであるが、−数的に、
高周波電源の周波数は13.560MHzが多用されて
いる。[Problems to be Solved by the Invention] Among the industrial frequencies assigned to Japan, the frequencies suitable for generating glow discharge plasma are 13.560 MHz, 27.
120MHz, 40.68MHz, but - numerically,
The frequency of the high frequency power source is often 13.560 MHz.
上記、第1の従来技術の問題点は、試験の結果、放電電
極上の処理対象物表面に発生する直流電位を一200V
から正側へ制御する場合、13.560MHzの高周波
II源の電力調整範囲は20〜2W程度であるため、電
力調整手段が高分解能で無いと、制御できる直流電位は
、ラフな値になってしまう。また、グロー放電を辛うじ
て維持できる高周波最小出力電力2WUi後まで出力を
下げても、処理対象物表面に発生する直流電位は一70
V程度もあり、これより正側への制御は不可能であった
。The problem with the above-mentioned first conventional technique is that, as a result of testing, the DC potential generated on the surface of the object to be treated on the discharge electrode was -200V.
When controlling from to the positive side, the power adjustment range of the 13.560MHz high frequency II source is about 20 to 2W, so if the power adjustment means does not have high resolution, the controllable DC potential will be a rough value. Put it away. In addition, even if the output is lowered to 2 WUi of the minimum high-frequency output power that can barely maintain glow discharge, the DC potential generated on the surface of the object to be processed is -70
It was also about V, and it was impossible to control it to the positive side beyond this.
なお、第5図に、参考までに、この第1の従来技術によ
り、高周波出力電力(進行波)をO〜20Wまで変化さ
せた時の放電電極直流電位及び処理対象物であるガラス
基板表面の直流電位の関係を示す。For reference, FIG. 5 shows the DC potential of the discharge electrode and the surface of the glass substrate to be processed when the high-frequency output power (travelling wave) is varied from 0 to 20 W using this first conventional technique. Shows the relationship between DC potential.
さらに、上記の試験結果の値は、放電電極と接地側棒と
の表面積割合、グロー放電生成に用いる作動ガスの圧力
、高周波整合装置の整合状態等で大きく変動するため、
放i11!極上の処理対象物表面に発生する直流電位を
検知するモニタ手段が無いと、所望する値に制御できな
い欠点がある2上記、第2の従来技術の問題点は、特開
平1−180970号公報の実施例に記載されているよ
うに、高周波電源の周波数を210MHz 。Furthermore, the values of the above test results vary greatly depending on the surface area ratio of the discharge electrode and the ground side rod, the pressure of the working gas used to generate glow discharge, the matching state of the high frequency matching device, etc.
Hou i11! If there is no monitoring means for detecting the DC potential generated on the surface of the finest object to be processed, there is a drawback that it cannot be controlled to a desired value.2 The problem with the above-mentioned second conventional technique is as described in Japanese Patent Application Laid-Open No. 1-180970. As described in the examples, the frequency of the high frequency power source was 210 MHz.
100MHzに選んでいるが、これらの周波数は、日本
に割当てられた工業用周波数では無いため、工業的に大
出力で用いるためには電波雑音防止手段が必要で、また
、−数的に用いられていない周波数であるため、専用の
高周波電源及び高周波整合装置を製作する必要があり、
性能の割に複雑で高価なものになってしまう欠点がある
。100MHz is selected, but these frequencies are not industrial frequencies assigned to Japan, so radio noise prevention means are required for industrial use at high output, and - Since the frequency is not specified, it is necessary to manufacture a dedicated high frequency power supply and high frequency matching device.
The drawback is that it is complicated and expensive despite its performance.
サラニ、13.560MHz (7)高周波1fili
i!及び整合装置及び高周波フィルタを用いて、その他
は第2の従来技術に従って試験した結果、放*’jl極
上の電気絶縁体の処理対象物表面に発生する直流電位値
の制御範囲は−76〜−122■と非常に狭い範囲でし
か制御できなかった。Sarani, 13.560MHz (7) High frequency 1fili
i! The control range of the DC potential value generated on the surface of the electrical insulator to be processed on the radiation pole is -76 to -. It could only be controlled within a very narrow range of 122■.
なお、第6図に、参考までに、この第2の従来技術によ
り、13.560MHzの高周波電源及び整合装置及び
高周波フィルタを用いて、その他は第2の従来技術に従
って試験した場合の、DCバイアス電源の出力電力を0
〜−300Vまで変化させた時の放電電極直流電位及び
処理対象物であるガラス基板表面の直流電位及びDCバ
イアス電源の出力電流の関係を示す。For reference, FIG. 6 shows the DC bias when tested using a 13.560 MHz high frequency power supply, a matching device, and a high frequency filter, and in accordance with the second prior art. Set the output power of the power supply to 0
The relationship between the DC potential of the discharge electrode, the DC potential of the surface of the glass substrate to be processed, and the output current of the DC bias power supply when changed to -300V is shown.
前記したことからもわかるよう1乙 2の従来技術は、
工業周波数として日本に割当ての無い特殊な周波数帯で
しか、その効果は期待できない欠点がある。As can be seen from the above, the conventional technologies of 1 and 2 are:
The drawback is that it can only be expected to be effective in a special frequency band that has not been allocated to Japan as an industrial frequency.
本発明は前述の如き、高周波tisを用い、電気絶縁性
基板や電気絶縁性薄膜の堆積又はエツチング、アッシン
グ等の薄膜処理を実施する際にグロー放電プラズマ中の
イオンを処理対象物表面に対し加速するのに必要となる
静電結合型放[電極及び、又は電極上の処理対象物表面
に発生する直流電位(セルフバイアス)の制御範囲が実
用的な範囲(−20〜−500V )を網羅し、かつ、
コストパフォーマンスと制御性に優れた高周波放電電極
及び、又は電極上の処理対象物表面に発生する直流電位
制御方法及び装置を提供することにある。As described above, the present invention uses high-frequency TIs to accelerate ions in a glow discharge plasma to the surface of an object to be processed when depositing an electrically insulating substrate or electrically insulating thin film, or performing thin film processing such as etching or ashing. The control range of the capacitively coupled discharge necessary for ,and,
It is an object of the present invention to provide a high frequency discharge electrode with excellent cost performance and controllability, and/or a DC potential control method and device generated on the surface of an object to be treated on the electrode.
[課題を解決するための手段]
本発明においては、前記課題を解決するために、高周波
グロー放電を利用する薄膜処理装置において、高周波電
力を供給する電極にローパスフィルタ(低域通過型濾波
器)を介し、電力消費手段(摺動抵抗器、電子負荷装置
等)を接続し、抵抗値又は直流分流入電流を調整するよ
うにした。[Means for Solving the Problems] In the present invention, in order to solve the above problems, in a thin film processing apparatus that utilizes high-frequency glow discharge, a low-pass filter (low-pass filter) is provided to an electrode that supplies high-frequency power. A power consumption means (sliding resistor, electronic load device, etc.) is connected through the connector to adjust the resistance value or DC inflow current.
[作用]
高周波グロー放電を利用する薄膜処理装置において、高
周波電力を供給する電極にローパスフィルタを介し、電
力消費手段、例えば摺動抵抗器を接続し、その抵抗値の
最大値のところで高周波グロー放電を開始する。この時
、静電結合型放電電極又は電極上の処理対象物表面に発
生する直流電位が所望する制御範囲の負側の絶対値の最
大値に成る様、高周波出力電力を設定する。その後、抵
抗値が減少する方向へ調整すると高周波グロー放電プラ
ズマ中のイオンと電子の移動度の差により生じる放t1
i極及び電極上の処理対象物表面に発生する直流電位の
値は、負側の絶対値の最大値より正側に変化する。これ
は、抵抗値の減少に伴い、電極からローパスフィルタを
介し、直流分の電流のみが増大するためである。また、
電極上の処理対象物表面に発生する直流電位も、負側の
絶対値の最大値より正側に変化する。これは、処理対象
物の形状と誘電率で決まる静電容量に対し、高周波電流
がこれに流れる事で、交流分電位差が、処理対象物表面
と電極の間で保たれるために、電極の直流分電位に追従
できる。さらに、抵抗値を0Ωにすると、電極直流電位
はO[V]に、電極上の処理対象物表面の直流電位は一
25V程度に制御可能で、この状態においても高周波グ
ロー放電プラズマの密度は、電極に投入する高周波電力
及び電力消費手段の最大インピーダンス(抵抗値)にも
よるが、通常、抵抗値最大時の70%程度を維持してい
る。したがって、本発明を薄膜堆積装置に適応すれば、
高イオン密度でかっ、低エネルギのイオンアシスト成膜
(イオンで堆積中の薄膜粒子を叩きながら成膜する技術
)が可能である。[Operation] In a thin film processing device that uses high-frequency glow discharge, a power consumption means, such as a sliding resistor, is connected to the electrode to which high-frequency power is supplied via a low-pass filter, and the high-frequency glow discharge occurs at the maximum resistance value of the power consumption means, such as a sliding resistor. Start. At this time, the high frequency output power is set so that the DC potential generated on the surface of the capacitively coupled discharge electrode or the object to be processed on the electrode reaches the maximum absolute value on the negative side of the desired control range. After that, when the resistance value is adjusted in the direction of decreasing, the radiation t1 caused by the difference in mobility between ions and electrons in the high-frequency glow discharge plasma
The value of the DC potential generated on the i-electrode and the surface of the object to be processed on the electrode changes from the maximum negative absolute value to the positive side. This is because as the resistance value decreases, only the direct current component increases from the electrode through the low-pass filter. Also,
The DC potential generated on the surface of the object to be processed on the electrode also changes from the maximum negative absolute value to the positive side. This is due to the electrostatic capacitance determined by the shape and dielectric constant of the object to be processed, and when the high-frequency current flows through this, an AC potential difference is maintained between the surface of the object to be processed and the electrode. Can follow DC component potential. Furthermore, when the resistance value is set to 0Ω, the electrode DC potential can be controlled to O[V], and the DC potential of the surface of the object to be treated on the electrode can be controlled to about -25V, and even in this state, the density of the high-frequency glow discharge plasma is Although it depends on the high frequency power input to the electrode and the maximum impedance (resistance value) of the power consumption means, the resistance value is usually maintained at about 70% of the maximum resistance value. Therefore, if the present invention is applied to a thin film deposition apparatus,
High ion density and low energy ion-assisted film formation (a technology in which thin film particles are formed while being bombarded with ions) is possible.
[実施例]
本発明を薄膜堆積装置の−っであるスパッタリング装置
に適用した実施例を第1図および第2図により、また、
電力消費手段の自動側!ll装置を具備した実施例を第
3図により、以下説明する。[Example] An example in which the present invention is applied to a sputtering apparatus, which is a thin film deposition apparatus, is shown in FIGS. 1 and 2, and
Automatic side of power consumption means! An embodiment equipped with the II device will be described below with reference to FIG.
第1図〜第3図において、】は13.560MHzの基
板電極用高周波S源装置、2は1i源側と負荷側のイン
ピーダンス整合を行う基板電極用高周波整合装置、3は
基板4を載置し水冷または加熱され所定の温度を保つ基
板用高周波放電電極、4は基板、5は成膜物質より成る
ターゲット、6はターゲット5を載置し水冷機構を有す
るターゲット用電極、loは高周波電力が印加される基
板用1i極3より直流成分のみを通しつるローパスフィ
ルタ(低域通過型濾波器)、11は必要に応じて用いら
れる高周波ノイズをカットするノイズフィルタ、12は
必要に応じて用いられる高周波輻射ノイズを遮閉するシ
ールド板、13は高周波グロー放電プラズマ中のイオン
と電子の移動度の差により生じる基板用数twit極3
及び電極上の基板4表面に発生する直流電位(セルフバ
イアス)を制御する電力消費手段の一つである摺動抵抗
器、14は必要に応じて用いられる電力消費手段13に
流入する直流成分の電流を検出する電流モニタ手段、1
5は必要に応じて用いられる基板用電極3の直流成分の
電位を検出する電圧モニタ手段、21は13.560M
Hzのターゲット電極用高周波電源装置、22は電源側
と負荷側のインピーダンス整合を行うターゲット電極用
高周波整合装置、23はターゲット5を載置し水冷機構
を有するターゲット用高周波放w′rIi極、24は高
周波電力が印加されるターゲット用電極23より直流成
分のみを通しうるローパスフィルタ(低域通過型濾波器
)、25は必要に応じて用いられる高周波ノイズをカッ
トするノイズフィルタ、26は必要に応じて用いられる
高周波輻射ノイズを遮閉するシールド板、27はターゲ
ット用放電電極23及び電極上のターゲット5表面に発
生する直流電位を制御する電力消費手段の一つである摺
動抵抗器、28は必要に応じて用いられる電力消費手段
27に流入する直流成分の電流を検出する電流モニタ手
段、29は必要に応じて用いられるターゲット用電極2
3の直流成分の電位を検出する電圧七二夕手段、30は
真空容器、32はターゲット5およびターゲット用電極
23の内部を冷却する水配管、33はターゲット用電極
23を真空容器30に連結するための真空シール機能お
よび電気絶縁機能を有する絶縁体、34は必要に応じて
用いられるプラズマポテンシャルを調整するために設け
られたアノードリング、35は真空容器外の電源からア
ノードリンク34へ給電するための電流導入端子、36
は真空容器30に対してアノードリンク34を電気的に
絶縁し固定するための絶縁体、38は基板用アースシー
ルド、39は基板用電極3と基板用アースシールド38
を連結するための真空シール機能および電気絶縁機能を
有する絶縁体、40はスパッタガスを導入する質量流量
制御弁、41は真空容器30の内部を排気する排気装置
、50はスパッタ用高圧電源、51は必要に応じてアノ
ードリングに給電する電源、60は高周波放電電極又は
電極上の処理対象物表面に発生する直流電位を設定した
値に自動制御する制御装置、61は電力消費手段の一つ
である摺動抵抗器の位置又は値を検出するセンサを示す
。In Figures 1 to 3, ] is a 13.560 MHz high frequency S source device for substrate electrodes, 2 is a high frequency matching device for substrate electrodes that performs impedance matching between the 1i source side and the load side, and 3 is a substrate 4 mounted. 4 is a substrate, 5 is a target made of a film-forming material, 6 is a target electrode on which the target 5 is placed and has a water cooling mechanism, lo is a high-frequency discharge electrode for a substrate that is water-cooled or heated to maintain a predetermined temperature; A low-pass filter (low-pass filter) that passes only the DC component from the applied substrate 1i pole 3; 11 is a noise filter that cuts high-frequency noise; 12 is used as necessary; A shield plate 13 blocks out high frequency radiation noise, and 13 is the number of substrate poles 3 caused by the difference in mobility between ions and electrons in high frequency glow discharge plasma.
and a sliding resistor 14, which is one of the power consumption means for controlling the DC potential (self-bias) generated on the surface of the substrate 4 on the electrode; Current monitor means for detecting current, 1
5 is a voltage monitor means for detecting the potential of the DC component of the substrate electrode 3, which is used as necessary; 21 is 13.560M;
22 is a high frequency matching device for target electrodes that performs impedance matching between the power supply side and the load side; 23 is a high frequency radiation w'rIi pole for the target on which the target 5 is mounted and has a water cooling mechanism; 24 25 is a low-pass filter (low-pass filter) that can pass only the DC component from the target electrode 23 to which high-frequency power is applied; 25 is a noise filter that cuts high-frequency noise; 26 is used as necessary; 27 is a sliding resistor which is one of the power consumption means for controlling the direct current potential generated on the target discharge electrode 23 and the surface of the target 5 on the electrode; A current monitor means for detecting the DC component current flowing into the power consumption means 27, which is used as necessary, and 29 is a target electrode 2, which is used as necessary.
3 voltage Tanabata means for detecting the potential of the DC component; 30 a vacuum container; 32 a water pipe for cooling the inside of the target 5 and the target electrode 23; 33 connecting the target electrode 23 to the vacuum container 30; 34 is an anode ring provided to adjust the plasma potential used as necessary; 35 is for supplying power to the anode link 34 from a power source outside the vacuum vessel. current introduction terminal, 36
38 is an insulator for electrically insulating and fixing the anode link 34 to the vacuum container 30; 38 is a board ground shield; 39 is a board electrode 3 and a board ground shield 38;
40 is a mass flow control valve for introducing sputtering gas, 41 is an exhaust device for evacuating the inside of vacuum container 30, 50 is a high-voltage power source for sputtering, 51 60 is a control device that automatically controls the DC potential generated on the surface of the high-frequency discharge electrode or the object to be processed on the electrode to a set value; and 61 is one of the power consumption means. A sensor is shown for detecting the position or value of a sliding resistor.
以上の構成要素からなる第1図は本発明の第1の実施例
で、スパッタリング装置の基板電極側に本発明を適用し
たものであり、装置全体は、以下のように動作する。FIG. 1, which consists of the above-mentioned components, shows a first embodiment of the present invention, in which the present invention is applied to the substrate electrode side of a sputtering apparatus, and the entire apparatus operates as follows.
基板4を基板用高周波電極3に載!した後、排気装置4
1により、真空容器30の内部を所定のバックグラウン
ド(高真空)まで排気すると同時に、基板用高層$電極
3を温度制御して基板4を所定の温度に保つ。その後、
スパッタ用のアルゴンガスを質量流量制御弁40より導
入し、所定のガス圧力に調整する。ターゲット5に電気
的に接続されたターゲット用電極6t\スパツタ用高圧
電源50から電力を供給すると、ターゲット5上に図示
していないがスパッタリング用の高密度なプラズマが発
生し、この高密度プラズマ中のアルゴンガスイオンは陰
極降下(カソードフォール)により加速されターゲット
5に衝突し、ターゲット原子をたたき出す。Place the substrate 4 on the high frequency electrode 3 for substrate! After that, exhaust device 4
1, the inside of the vacuum container 30 is evacuated to a predetermined background (high vacuum), and at the same time, the temperature of the high-rise substrate electrode 3 is controlled to maintain the substrate 4 at a predetermined temperature. after that,
Argon gas for sputtering is introduced through the mass flow control valve 40 and adjusted to a predetermined gas pressure. When power is supplied from the target electrode 6t electrically connected to the target 5\sputtering high-voltage power source 50, high-density plasma for sputtering (not shown) is generated on the target 5, and in this high-density plasma The argon gas ions are accelerated by cathode fall and collide with the target 5, knocking out target atoms.
この時、摺動抵抗器13の抵抗値が最大になる位置に合
わせ、高周波整合装置2で整合をとりながら基板電極用
高周波電源1の出力電力を増し、基板用放電電極3又は
電極上の基板4表面に発生する直流電位が所望する負側
の絶対値より若干大きい値に成る所に出力電力を合わせ
る。その後、電圧モニタ手段15を参照するか、又は、
図示していないが処理対象物である基板表面の電位をモ
ニタする手段を参照するか、又は、事前に調査しておい
た基板表面電位と相関のある電力消費手段に流入する電
流を検出する電流モニタ手段14を参照し、摺動抵抗器
13の抵抗値を減少させ、所望する値に正確に制御する
。At this time, adjust the resistance value of the sliding resistor 13 to the maximum position, increase the output power of the high frequency power source 1 for substrate electrodes while performing matching with the high frequency matching device 2, and increase the output power of the high frequency power source 1 for substrate electrodes or the substrate on the discharge electrode 3 for substrates. 4 Adjust the output power to a point where the direct current potential generated on the surface becomes a value slightly larger than the desired absolute value on the negative side. Then refer to the voltage monitoring means 15, or
A current that refers to a means (not shown) that monitors the potential of the surface of the substrate that is the object to be processed, or detects a current that flows into a power consumption means that is correlated with the substrate surface potential that has been investigated in advance. Referring to the monitoring means 14, the resistance value of the sliding resistor 13 is decreased and accurately controlled to a desired value.
上記のスパッタ操作により、たたき出されたターゲット
原子が基板4表面上に堆積すると同時に、上記の基板バ
イアス操作により制御した直流成分の基板表面電位とプ
ラズマポテンシャル(プラズマ電位)との電位差により
加速された基板4近傍のプラズマ中のアルゴンガスイオ
ン及びターゲット原子の中で正にイオン化されたものが
基板4表面に衝突し、イオンアシスト成膜機能(イオン
により基板に堆積する薄膜粒子にマイグレーションを与
え、緻密度、膜応力、結晶性等の膜質制御を可能とする
技術)を果たす。このイオンアシスト成膜技術において
重要な制御因子は、基板4に照射するイオンの加速エネ
ルギとイオンの個数(正確にはスパッタされたターゲッ
ト粒子の内で基板に堆積する粒子と基板に照射するイオ
ンの個数の比¥A)であり、基板4に照射するイオンの
加速エネルギとイオンの個数との独立制御性が優れてい
る程、幅広い新機能薄膜に対応できる。例えば、基板4
に照射するイオンの個数を多くし、加速エネルギを低く
して成膜する場合には、上記、基板電極用高周波電源工
の出力電力を大としでイオン個数に直接関係のある基板
4近傍のプラズマ密度を大きくし、摺動抵抗器13の抵
抗値を小とすれば良い。また、イオンの個数を正確に所
望する値に制御する場合は、図示していないがイオンの
個数を検出するイオンモニタ、例えばラングミアブロー
ブ等を基板4近傍に設置し、この値を参詔しながら高周
波St源の出力を」η整すれば良い。By the above sputtering operation, the ejected target atoms are deposited on the surface of the substrate 4, and at the same time, they are accelerated by the potential difference between the substrate surface potential of the DC component and the plasma potential (plasma potential) controlled by the above substrate bias operation. Positively ionized argon gas ions and target atoms in the plasma near the substrate 4 collide with the surface of the substrate 4, resulting in an ion-assisted film formation function (ions give migration to the thin film particles deposited on the substrate, forming a dense film). technology that enables control of film quality such as film strength, film stress, and crystallinity). Important control factors in this ion-assisted film formation technology are the acceleration energy of the ions irradiated onto the substrate 4 and the number of ions (more precisely, the number of sputtered target particles deposited on the substrate and the number of ions irradiated onto the substrate). The ratio of the number of ions is A), and the better the independent controllability of the acceleration energy of ions irradiated to the substrate 4 and the number of ions, the more it can be applied to a wide range of new functional thin films. For example, board 4
When forming a film by increasing the number of ions irradiated and lowering the acceleration energy, the output power of the above-mentioned high-frequency power source for substrate electrodes is increased to increase the plasma concentration near the substrate 4, which is directly related to the number of ions. The density may be increased and the resistance value of the sliding resistor 13 may be reduced. In addition, in order to accurately control the number of ions to a desired value, an ion monitor (not shown) that detects the number of ions, such as a Langmire probe, is installed near the substrate 4, and this value is measured. However, the output of the high frequency St source may be adjusted by "η".
すなわち、放電電極に供給する高周波電力によって処理
対象物近傍のイオン個数を制御し、放電電極にローパス
フィルタを介し接続された電力消費手段の調整により処
理対象物に入射するイオンの加速エネルギを決める負の
バイアスを独立制御できる。In other words, the number of ions near the object to be treated is controlled by high-frequency power supplied to the discharge electrode, and the acceleration energy of the ions incident on the object to be treated is determined by adjusting the power consumption means connected to the discharge electrode via a low-pass filter. bias can be controlled independently.
第2図は本発明の第2の実施例で、スパッタリング装置
のターゲット電極側に本発明を適用したものであり、以
下のように動作する。FIG. 2 shows a second embodiment of the present invention, in which the present invention is applied to the target electrode side of a sputtering device, and operates as follows.
基板4を基板用電極3に載置した後、排気装置41によ
り、真空容器30の内部を所定のバックグラウンドまで
排気すると同時に、基板用電極3を温度制御して基板4
を所定の温度に保つ。その後、スパッタ用のアルゴンガ
スな質量流量制御弁40より導入し、所定のガス圧力に
調整する。この時、摺動抵抗器27の抵抗値が最大にな
る位置に合わせ、ターゲット5に電気的に接続されたタ
ーゲット用高周波電極23へ高周波整合装置22で整合
をとりながらターゲット電極用高周波電源21の出力電
力を供給すると、ターゲット5上に図示していないがス
パッタリング用のプラズマが発生し、このプラズマ中の
アルゴンガスイオンはターゲット表面に発生した負の直
流電位により加速されターゲット5に衝突し、ターゲッ
ト原子をたたき出す。ターゲット明放at極23又は電
極上のターゲット5表面に発生する直流電位を。After placing the substrate 4 on the substrate electrode 3, the exhaust device 41 evacuates the inside of the vacuum container 30 to a predetermined background level, and at the same time controls the temperature of the substrate electrode 3 to remove the substrate 4.
to maintain the specified temperature. Thereafter, argon gas for sputtering is introduced through the mass flow control valve 40 and adjusted to a predetermined gas pressure. At this time, the high-frequency power source 21 for the target electrode is adjusted to the position where the resistance value of the sliding resistor 27 is maximum, and the high-frequency power source 21 for the target electrode is matched with the high-frequency electrode 23 for the target electrically connected to the target 5 using the high-frequency matching device 22. When output power is supplied, sputtering plasma (not shown) is generated on the target 5, and the argon gas ions in this plasma are accelerated by the negative DC potential generated on the target surface and collide with the target 5. Knock out atoms. A DC potential generated on the target open-emitting at pole 23 or on the surface of the target 5 on the electrode.
摺動抵抗器27の抵抗値を調整することで所望する値に
正確に制御する。抵抗値の調整に際しては、前記、第1
の実施例と同様に、電圧モニタ手段29を参照するか、
又は、図示していないが処理対象物であるターゲット表
面の電位をモニタする手段を参照するか、又は、事前に
調査しておいたターゲット表面電位と相関のある電力消
費手段に流入する電流を検出する電流モニタ手段28を
参照しながら行っても良い。上記のターゲット5表面に
発生する直流電位を制御すれば、スパッタ率が変化し成
膜速度が若干調整できることはもとより、たたき出され
たターゲット原子の持つ運動エネルギの制御が可能で、
基板4に堆積する過程でダメージを嫌う成膜にも対応で
きる。By adjusting the resistance value of the sliding resistor 27, it is accurately controlled to a desired value. When adjusting the resistance value, the first
Referring to the voltage monitoring means 29 as in the embodiment of
Alternatively, refer to a means (not shown) for monitoring the potential on the surface of the target that is the object to be processed, or detect the current flowing into the power consumption means that is correlated with the target surface potential investigated in advance. This may be done while referring to the current monitoring means 28. By controlling the DC potential generated on the surface of the target 5, it is possible to change the sputtering rate and slightly adjust the film formation rate, and also to control the kinetic energy of the ejected target atoms.
It can also be applied to film formation in which damage is avoided during the process of depositing on the substrate 4.
第3図は本発明の第3の実施例で、抵抗値又は、及び、
直流分流入電流又は、及び5高周波放電電極に発生する
直流分の電位をモニタする信号をもとに、所望する(設
定した)高周波放電電極又は電極上の処理対象物表面に
発生する直流電位に成る様、電力消費手段(摺動抵抗器
、電子負荷装置等〕を自動制御する制御装置を具備した
ものを示し、以下のように動作する。FIG. 3 shows a third embodiment of the present invention, in which the resistance value or
Based on the signal that monitors the DC component inflow current or the DC component potential generated in the high-frequency discharge electrode 5, the DC potential generated on the desired (set) high-frequency discharge electrode or the surface of the object to be treated on the electrode is adjusted. The device is equipped with a control device that automatically controls the power consumption means (sliding resistor, electronic load device, etc.) so as to achieve the desired results, and operates as follows.
高周波放電電極又は、及び、電極上の処理対象物表面に
発生する直流電位と各種モニタ信号である抵抗値、直流
分流入電流、高周波放電電極に発生する直流分電位の総
て又は、一部との相関をあらかじめ求め(古典制御理論
では伝達関数、現代制御理論では状態方程式を求め)、
制御装置60のプログラムを行う。摺動抵抗器の抵抗値
を例えば、駆動用アクチュエータの回転角度より検出す
る抵抗値検出センサ61の信号、電力消費手段に流入す
る直流成分電流を検出する電流モニタ手段14の信号、
放電電極の直流成分電位を検出する電圧モニタ手段15
の信号の総て又は一部の信号により、制御装置6oは設
定された値に成る様に電力消費手段13の駆動用アクチ
ュエータに信号を与え、自動制御を行う。なお、上記の
各種モニタ信号以外の例えば、高周波電源の出力電力、
高周波1を源の出力電圧波高値、ガス圧力、1!極間距
離等の信号を追加利用しても良く、第3図に限定するも
のでは無い。All or part of the DC potential generated on the high-frequency discharge electrode or the surface of the object to be processed on the electrode, the resistance value that is various monitor signals, the DC inflow current, and the DC potential generated on the high-frequency discharge electrode. Find the correlation in advance (determine the transfer function in classical control theory, and find the state equation in modern control theory),
Program the control device 60. For example, a signal from the resistance value detection sensor 61 that detects the resistance value of the sliding resistor from the rotation angle of the drive actuator, a signal from the current monitor means 14 that detects the DC component current flowing into the power consumption means,
Voltage monitor means 15 for detecting the DC component potential of the discharge electrode
The control device 6o automatically controls the drive actuator of the power consumption means 13 by giving a signal to the drive actuator of the power consumption means 13 so that the set value is achieved based on all or some of the signals. In addition to the various monitor signals mentioned above, for example, the output power of a high frequency power supply,
High frequency 1 is the output voltage peak value of the source, gas pressure, 1! Signals such as the distance between poles may be additionally used, and the present invention is not limited to that shown in FIG. 3.
なお、本発明の実施例である第1図〜第3図において、
基板搬送手段、基板移動手段、基板回転手段、リアクテ
ィブスパッタ用ガス導入手段シャッタ、ビューボート、
真空計等は図示していないが、必要に応じて使用が可能
である。また、電力消費手段として、摺動抵抗器を示し
たが、例えば、電子負荷装置等も使用可能で、第1図〜
第3図に示す構成に限定するものではない。In addition, in FIGS. 1 to 3 which are examples of the present invention,
Substrate transport means, substrate movement means, substrate rotation means, reactive sputtering gas introduction means shutter, view boat,
Although a vacuum gauge and the like are not shown, they can be used if necessary. In addition, although a sliding resistor is shown as a power consumption means, for example, an electronic load device or the like can also be used.
The configuration is not limited to the configuration shown in FIG. 3.
さらに、第1図〜第2図では、本発明を薄膜形成装置の
一つであるスパッタリング装置のそれぞれ一方の電極に
適用した例を示したが、これに限定するものでは無く、
必要に応じて基板電極及びターゲット電極双方に適用す
る事が可能で、また、スパッタリング装置に限定するも
のでは無く、プラズマCVD (プラズマを利用した化
学蒸着法)。Furthermore, although FIGS. 1 and 2 show an example in which the present invention is applied to one electrode of a sputtering device, which is one type of thin film forming device, the present invention is not limited to this.
It can be applied to both substrate electrodes and target electrodes as needed, and is not limited to sputtering equipment; plasma CVD (chemical vapor deposition method using plasma).
エツチング装置、アッシング装置等の高周波グロー放電
を利用する薄膜処理技術の中で、特に高周波電源を用い
、静電結合型放電電極及び、又は電極上の処理対象物表
面に発生する直流電位を所望する値に成る様、強制的に
制御し薄膜形成又は薄膜処理を行う方法及び装置に適用
できる。Among thin film processing technologies that utilize high-frequency glow discharge such as etching equipment and ashing equipment, it is particularly desirable to use a high-frequency power source and generate a DC potential on the surface of a capacitively coupled discharge electrode and/or the object to be processed on the electrode. It can be applied to a method and apparatus that performs thin film formation or thin film processing by forcibly controlling so that the value is the same.
第4図は、本発明の実施例である第1図に示すものにつ
いて、電力消費手段の一つである摺動抵抗器の抵抗値を
調整して放電電極の直流成分の電位をO〜−300Vま
で変化させた時の放電電極直流電位及び処理対象物であ
るガラス基板表面の直流電位及び摺動抵抗器に流入する
直流成分の電流値の関係を示したものである。主要条件
は放電ガス圧力を20m torr (アルゴン)、電
極間距離が60mm、電極寸法をφ144mm、真空容
器内側寸法を$250X240Hmm、13.560M
Hzの高周波出力電力(進行波)を120W−定にして
、実験した。FIG. 4 shows an example of the present invention shown in FIG. 1, in which the resistance value of the sliding resistor, which is one of the power consumption means, is adjusted to adjust the potential of the DC component of the discharge electrode from O to -. The figure shows the relationship between the DC potential of the discharge electrode, the DC potential of the surface of the glass substrate to be processed, and the current value of the DC component flowing into the sliding resistor when the voltage is varied up to 300V. The main conditions are: discharge gas pressure of 20 m torr (argon), distance between electrodes of 60 mm, electrode dimensions of φ144 mm, vacuum vessel inner dimensions of $250 x 240 H mm, 13.560 M.
The experiment was conducted with the Hz high frequency output power (traveling wave) constant at 120W.
本発明の試験結果である第4図と従来技術の試験結果で
ある第6図を比較すると明らかな様に、第6図では放電
電極上の電気絶縁体の処理対象物であるガラス基板表面
に発生する直流電位の制御範囲は−76〜−122■と
非常に狭い範囲であるのに対し、第4図では放′R,電
極上のガラス基板表面に発生する直流電位の制御範囲が
−25〜−290Vと広範囲で、しかも、電位のモニタ
が容易な放電電極電位に約±20Vの差で追従している
。また、図示していないが、高周波電源の出力電力(進
行波)を200W一定とし、その他の条件を同一にする
とガラス基板表面に発生する直流電位の制御範囲が−2
7〜−510Vにさらに広がる。さらに、高周波電源の
出力電力(進行波)を400W一定とし、抵抗値をOΩ
に調整すると放電電極の直流電位はO[V]に、ガラス
基板表面に発生する直流電位は一29Vになり、この時
のガラス基板に入射するイオンの個数は、約1.2X1
016個/seeである。As is clear from a comparison between FIG. 4, which shows the test results of the present invention, and FIG. 6, which shows the test results of the prior art, in FIG. The control range of the generated DC potential is very narrow, from -76 to -122mm, whereas in Figure 4, the control range of the DC potential generated on the surface of the glass substrate on the electrode is -25mm. It has a wide range of ~-290V and follows the discharge electrode potential, which is easy to monitor, with a difference of about ±20V. Although not shown, if the output power (traveling wave) of the high-frequency power source is constant at 200 W and other conditions are the same, the control range of the DC potential generated on the surface of the glass substrate is -2
It further spreads from 7 to -510V. Furthermore, the output power (traveling wave) of the high frequency power supply was set to be constant at 400W, and the resistance value was set to OΩ.
When the DC potential of the discharge electrode is adjusted to O[V], the DC potential generated on the surface of the glass substrate becomes -29V, and the number of ions incident on the glass substrate at this time is approximately 1.2X1.
016 pieces/see.
[発明の効果]
本発明によれば、高周波グロー放電を利用する薄膜処理
装置において、高周波電力を供給する静電結合型放電電
極又は電極上の処理対象物表面に発生する直流電位を広
範囲に制御可能で、処理対象物表面に入射するイオン個
数を非常に多くした状態でかつイオンの加速エネルギを
30eV程度の小さな値に成る様な、電極上の処理対象
物表面の直流電位に制御できる。したがって、本発明を
薄膜堆積装置に適応ずれば、高イオン密度でかつ、低エ
ネルギのイオンアシスト成膜(イオンで堆積中の薄膜粒
子を叩きながら成膜する技術)が可能になる。また、電
気絶縁性基板や電気絶縁性薄膜のエツチング、アッシン
グ等の薄膜処理に適用すれば、低ダメージの処理が可能
となる。しかも、本発明の技術は、日本に割当てられた
工業用周波数で、グロー放電プラズマ生成に適し、−数
的に多用されている周波数が13.560MHzの高周
波電源及び高周波整合装置を用いて十分な機能を果たす
。[Effects of the Invention] According to the present invention, in a thin film processing apparatus that utilizes high-frequency glow discharge, the DC potential generated on the surface of a capacitively coupled discharge electrode or the object to be processed on the electrode that supplies high-frequency power can be controlled over a wide range. It is possible to control the direct current potential of the surface of the object to be processed on the electrode so that the number of ions incident on the surface of the object to be processed is greatly increased and the acceleration energy of the ions is a small value of about 30 eV. Therefore, if the present invention is applied to a thin film deposition apparatus, ion-assisted film formation (a technique for forming a film while hitting the thin film particles being deposited with ions) with high ion density and low energy becomes possible. Further, if applied to thin film processing such as etching and ashing of electrically insulating substrates and electrically insulating thin films, it becomes possible to perform processing with low damage. In addition, the technology of the present invention is suitable for generating glow discharge plasma at the industrial frequency assigned to Japan, and uses a high frequency power source and a high frequency matching device whose frequency is 13.560 MHz, which is numerically frequently used. fulfill a function.
第1図は本発明の第1の実施例で、薄膜形成装置の一つ
であるスパッタリング装置の基板電極側に適用した場合
の構成を示す装置全体の断面概略図、第2図は本発明の
第2の実施例で、同スパッタリング装置のターゲット電
極側に適用した場合の構成を示す装置全体の断面概略図
、第3図は本発明の第3の実施例で、抵抗値又は、及び
、直流分流入電流又は、及び、高周波放電電極に発生す
る直流分の電位をモニタする信号をもとに、所望する(
設定した)高周波放電電極又は電極上の処理対象物表面
に発生する直流電位になるように、電力消費手段(摺動
抵抗器、1i子負荷装置等)を自動制御する制御装置を
具備した場合を説明する主要構成要素を示す概略図、第
4図は、本発明の第1の実施例である第1図に示すもの
について、電力消費手段の一つである摺動抵抗器の抵抗
値を調整して放電電極の直流成分の電位をO〜−300
Vまで変化させた時の放電電極直流電位及び処理対象物
であるガラス基板表面の直流電位及び摺動抵抗器に流入
する直流成分の電流値の関係を示す線図、第5図は第1
の従来技術により、高周波出力電力(進行波)をO〜2
0Wまで変化させた時の放電電極直流電位及び処理対象
物であるガラス基板表面の直流電位の関係を示す線図、
第6図は第2の従来技術により、13.560MHzの
高周波電源及び整合装置及び高周波フィルタを用いて、
その他は第2の従来技術に従って試験した場合の、DC
バイアス電源の出力電圧を0〜−300Vまで変化させ
た時の放電電極直流電位及び処理対象物であるガラス基
板表面の直流電位及びDCバイアス電源の出力電流の関
係を示す線図である。
l・・・基板電極用高周波電源装置、
2・・・基板電極用高周波整合製雪、
3・・・基板用高周波数1i電極、
4・・・基板、 5・・・ターゲット、
6・・・ターゲット用電極、
10.24・・・ローパスフィルタ、
11.25・・・ノイズフィルタ、
12.26・・・シールド扱、
13.27・・・摺動抵抗器、
14.28・・・電流モニタ手段、
15.29・・・電圧モニタ手段、
21・・・ターゲット電極用高周波電源装置、22・・
・ターゲット電極用高周波整合装置、23・・・ターゲ
ット用高周波放電電極、30・・・真空容器、 3
2・・・水配管、33.36.39・・・絶縁体、
34・・・アノードリング、35・・・電流導入端子、
38・・・基板用アースシールド、
40・・・質量流量制御弁、41・・・排気装置、50
・・・スパッタ用高圧電源、
51・・・アノードバイアス電源、
60・・・自動制御装置、
61・・・電力消費手段の値を検出するセンサ。
特許出願人 宇部興産株式会社
第2図
第1図
第3図
第5図
試験条件;
真空容器
:φ250 X 24L)?−
第4図
試験条件:
第6図
試験条件;
高周波室カニ5W(進行波)一定FIG. 1 shows a first embodiment of the present invention, and is a schematic cross-sectional view of the entire device when applied to the substrate electrode side of a sputtering device, which is one of the thin film forming devices. The second embodiment is a schematic cross-sectional view of the entire device showing the configuration when applied to the target electrode side of the same sputtering device, and FIG. 3 is a third embodiment of the present invention. The desired (
The case is equipped with a control device that automatically controls the power consumption means (sliding resistor, 1I load device, etc.) so that the DC potential generated on the surface of the high-frequency discharge electrode or the object to be processed on the electrode is set. FIG. 4 is a schematic diagram showing the main components to be explained, and the resistance value of the sliding resistor, which is one of the power consumption means, is adjusted for the first embodiment of the present invention shown in FIG. and set the potential of the DC component of the discharge electrode to O~-300.
Figure 5 is a diagram showing the relationship between the DC potential of the discharge electrode, the DC potential of the surface of the glass substrate to be processed, and the current value of the DC component flowing into the sliding resistor when changed to V.
With conventional technology, high frequency output power (traveling wave) can be reduced to
A diagram showing the relationship between the DC potential of the discharge electrode and the DC potential of the surface of the glass substrate to be processed when changed to 0W,
FIG. 6 shows a second conventional technique using a 13.560 MHz high frequency power supply, a matching device, and a high frequency filter.
Others are DC when tested according to the second prior art.
FIG. 3 is a diagram showing the relationship between the DC potential of the discharge electrode, the DC potential of the surface of the glass substrate to be processed, and the output current of the DC bias power supply when the output voltage of the bias power supply is varied from 0 to -300V. l... High frequency power supply device for substrate electrodes, 2... High frequency matching snowmaking for substrate electrodes, 3... High frequency 1i electrodes for substrates, 4... Substrate, 5... Target,
6... Target electrode, 10.24... Low pass filter, 11.25... Noise filter, 12.26... Shield treatment, 13.27... Sliding resistor, 14.28. ...Current monitor means, 15.29...Voltage monitor means, 21...High frequency power supply device for target electrode, 22...
- High frequency matching device for target electrode, 23... High frequency discharge electrode for target, 30... Vacuum container, 3
2... Water piping, 33.36.39... Insulator, 34... Anode ring, 35... Current introduction terminal,
38... Earth shield for substrate, 40... Mass flow control valve, 41... Exhaust device, 50
... High voltage power supply for sputtering, 51 ... Anode bias power supply, 60 ... Automatic control device, 61 ... Sensor for detecting the value of power consumption means. Patent applicant: Ube Industries, Ltd. Figure 2 Figure 1 Figure 3 Figure 5 Test conditions; Vacuum container: φ250 x 24L)? - Figure 4 test conditions: Figure 6 test conditions; High frequency chamber crab 5W (traveling wave) constant
Claims (2)
て、高周波電力を供給する電極にローパスフィルタを介
し、電力消費手段を接続し、抵抗値や直流分流入電流を
調整することにより、高周波放電電極及び、又は電極上
の処理対象物表面に発生する直流分の電位を強制的に制
御することを特徴とする薄膜処理装置の直流電位制御方
法。(1) In a thin film processing device that utilizes high-frequency glow discharge, the high-frequency discharge electrode and , or a DC potential control method for a thin film processing apparatus, comprising forcibly controlling a DC potential generated on the surface of an object to be processed on an electrode.
て、高周波電力を供給する電極にローパスフィルタを介
し、電力消費手段を接続し、このローパスフィルタに抵
抗値を調整可能な摺動抵抗器を接続し、かつ、直流分流
入電流を調整可能な高周波電力制御装置を接続して設け
たことを特徴とする薄膜処理装置の直流電位制御装置。(2) In a thin film processing device that uses high-frequency glow discharge, a power consumption means is connected to the electrode that supplies high-frequency power via a low-pass filter, and a sliding resistor whose resistance value can be adjusted is connected to this low-pass filter. A DC potential control device for a thin film processing apparatus, characterized in that the DC potential control device is connected to and provided with a high frequency power control device capable of adjusting a DC component inflow current.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11015490A JPH049465A (en) | 1990-04-27 | 1990-04-27 | Method and device for controlling dc potential in thin film forming device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP11015490A JPH049465A (en) | 1990-04-27 | 1990-04-27 | Method and device for controlling dc potential in thin film forming device |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH049465A true JPH049465A (en) | 1992-01-14 |
Family
ID=14528424
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP11015490A Pending JPH049465A (en) | 1990-04-27 | 1990-04-27 | Method and device for controlling dc potential in thin film forming device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH049465A (en) |
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006137966A (en) * | 2004-11-10 | 2006-06-01 | Matsushita Electric Ind Co Ltd | Sputtering apparatus and sputtering method |
| JP2007096051A (en) * | 2005-09-29 | 2007-04-12 | Samco Inc | Cathode-coupling plasma cvd equipment and thin film manufacturing method by it |
| JP2008041795A (en) * | 2006-08-03 | 2008-02-21 | Tokyo Electron Ltd | Plasma treatment device and plasma treatment method |
| JP2009231417A (en) * | 2008-03-21 | 2009-10-08 | Fujifilm Corp | Manufacturing method for piezoelectric-body film, film forming device, and piezoelectric-body film |
| JP2019024090A (en) * | 2013-11-06 | 2019-02-14 | アプライド マテリアルズ インコーポレイテッドApplied Materials,Incorporated | Particle generation suppressing device by DC bias modulation |
-
1990
- 1990-04-27 JP JP11015490A patent/JPH049465A/en active Pending
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2006137966A (en) * | 2004-11-10 | 2006-06-01 | Matsushita Electric Ind Co Ltd | Sputtering apparatus and sputtering method |
| JP2007096051A (en) * | 2005-09-29 | 2007-04-12 | Samco Inc | Cathode-coupling plasma cvd equipment and thin film manufacturing method by it |
| JP2008041795A (en) * | 2006-08-03 | 2008-02-21 | Tokyo Electron Ltd | Plasma treatment device and plasma treatment method |
| JP2009231417A (en) * | 2008-03-21 | 2009-10-08 | Fujifilm Corp | Manufacturing method for piezoelectric-body film, film forming device, and piezoelectric-body film |
| JP2019024090A (en) * | 2013-11-06 | 2019-02-14 | アプライド マテリアルズ インコーポレイテッドApplied Materials,Incorporated | Particle generation suppressing device by DC bias modulation |
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