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JPH0796704B2 - Method for homogenizing low-temperature plasma - Google Patents
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JPH0796704B2 - Method for homogenizing low-temperature plasma - Google Patents

Method for homogenizing low-temperature plasma

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Publication number
JPH0796704B2
JPH0796704B2 JP61270444A JP27044486A JPH0796704B2 JP H0796704 B2 JPH0796704 B2 JP H0796704B2 JP 61270444 A JP61270444 A JP 61270444A JP 27044486 A JP27044486 A JP 27044486A JP H0796704 B2 JPH0796704 B2 JP H0796704B2
Authority
JP
Japan
Prior art keywords
electrode
plasma
cable
power supply
temperature plasma
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 - Fee Related
Application number
JP61270444A
Other languages
Japanese (ja)
Other versions
JPS63125671A (en
Inventor
保友 大口
四郎 堤
正克 高橋
博司 石徹白
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.)
SANDO TECH, INC.
Unitika Ltd
Original Assignee
SANDO TECH, INC.
Unitika Ltd
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 SANDO TECH, INC., Unitika Ltd filed Critical SANDO TECH, INC.
Priority to JP61270444A priority Critical patent/JPH0796704B2/en
Publication of JPS63125671A publication Critical patent/JPS63125671A/en
Publication of JPH0796704B2 publication Critical patent/JPH0796704B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Plasma Technology (AREA)
  • Treatment Of Fiber Materials (AREA)
  • Physical Vapour Deposition (AREA)

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、有機材料、無機材料等の表面処理などで利用
される低温プラズマ処理において、高周波放電により発
生する低温プラズマの均一化方法に関するものである。
TECHNICAL FIELD The present invention relates to a method for homogenizing low-temperature plasma generated by high-frequency discharge in low-temperature plasma processing used for surface treatment of organic materials, inorganic materials, and the like. .

従来の技術 近年、半導体、金属、有機材料、無機材料等の表面処理
や薄膜形成等に低圧力下での高周波放電によるプラズマ
が利用されている。プラズマ処理効果の一つとして、た
とえば布帛等の低温プラズマ雰囲気中での処理により、
糊抜、精練あるいは仕上効果が得られることが知られて
いる。これらの処理のための内部電極型低温プラズマ処
理装置は、たとえば繊維機械学会誌:第38巻、NO.4.198
〜199頁(1985)、特公昭60−31937号、特公昭60−1114
9号、特公昭60−11150号公報などに紹介されている。そ
の基本的構造は第4図に示すとおりである。すなわち第
4図において、真空を保持し得るようにした処理室
(1)内に、高電圧印加電極板(2)とそれに平行に一
定の間隔をおいて対向する接地電極板(3)とを配設
し、前記高電圧印加電極板(2)のほぼ中央に給電点
(2a)を設け、接地電極板(3)のほぼ中央に接地点
(3a)を設け、両電極(2),(3)間に高周波電源装
置(4)から高周波高電圧を印加する。真空シールされ
た入口(5a)から被処理シート状物(b)を供給ローラ
(7a)により送り込み、前記両電極(2),(3)間で
処理し、出口(5b)から巻取ローラ(7b)により巻取
る。なお処理室(1)内へは、空気、酸素等の所定の処
理ガスを給気口(8a)から所定の量を連続して送り込
み、排気口(8b)から連続排気しつつ、所定の圧力を保
つ。これらの装置では、高電圧印加電極板(2)および
接地電極板(3)からなるプラズマ発生電極が真空系の
処理室(1)内に設置されるため、壁を貫通して大気中
から真空中へと高周波電力を供給するための電路(以下
給電部という)(9)が必要である。
2. Description of the Related Art In recent years, plasma by high-frequency discharge under low pressure has been used for surface treatment of semiconductors, metals, organic materials, inorganic materials and the like, thin film formation and the like. As one of the plasma treatment effects, for example, by treating a cloth or the like in a low-temperature plasma atmosphere,
It is known that a desizing, scouring or finishing effect can be obtained. An internal electrode type low temperature plasma processing apparatus for these treatments is disclosed in, for example, Journal of the Textile Machinery Society: Volume 38, NO.4.198.
Pp. 199 (1985), Japanese Patent Publication No. 60-31937, Japanese Patent Publication No. 60-1114
No. 9 and Japanese Patent Publication No. 60-11150. Its basic structure is as shown in FIG. That is, in FIG. 4, a high voltage applying electrode plate (2) and a ground electrode plate (3) facing the high voltage applying electrode plate (2) at a constant interval in parallel to the high voltage applying electrode plate (2) are arranged in a processing chamber (1) capable of holding a vacuum. The high voltage applying electrode plate (2) is provided with a feeding point (2a) substantially at the center thereof, and the ground electrode plate (3) is provided with a grounding point (3a) at the substantially center thereof. During the period 3), a high frequency high voltage is applied from the high frequency power supply device (4). The sheet-like material (b) to be treated is fed by the supply roller (7a) from the vacuum-sealed inlet (5a), processed between the electrodes (2) and (3), and taken up from the outlet (5b) to the take-up roller ( Wind up according to 7b). It should be noted that a predetermined processing gas such as air and oxygen is continuously fed into the processing chamber (1) through a supply port (8a) in a predetermined amount and continuously exhausted through an exhaust port (8b) at a predetermined pressure. Keep In these devices, since the plasma generating electrode composed of the high voltage applying electrode plate (2) and the ground electrode plate (3) is installed in the vacuum processing chamber (1), it penetrates through the wall and is vacuumed from the atmosphere. An electric circuit (hereinafter referred to as a power feeding unit) (9) for supplying high frequency power to the inside is required.

上記のごとく第4図に例示する従来の装置において、通
常処理室(1)本体と処理室(1)内の金属類は接地さ
れているため、高周波電圧が印加されている給電部
(9)および高電圧印加電極板(2)と、その周囲の処
理室(1)本体および処理室(1)内の金属類との間で
プラズマが発生し、これにより著しい電力損失が生じる
とともに、処理室(1)本体および付近の絶縁物を過熱
し、あるいは給電部(9)、電極板(2),(3)自身
も過熱するなどで、処理室(1)内の広い範囲にわたっ
て熱的な歪や熱劣化が起こるなどの問題があったが、同
軸ケーブルあるいは平衡型ケーブルなどの外部がシール
ドされたケーブルを給電線として用いて、プラズマ発生
電極の一端部に接続した内部電極型低温プラズマ処理装
置が試みられて、給電線と電極の接続点での反射が小さ
くなり、給電線上に生じる定在波が小さくなって給電線
の局所過熱がなくなり、さらにプラズマが発生電極内に
局在化されて不要なプラズマを発生することがない、な
どの効果が得られている。
As described above, in the conventional apparatus illustrated in FIG. 4, the main body of the normal processing chamber (1) and the metals in the processing chamber (1) are grounded, so that the power feeding section (9) to which the high frequency voltage is applied. Plasma is generated between the high voltage application electrode plate (2) and the surrounding processing chamber (1) body and the metals inside the processing chamber (1), which causes significant power loss and also causes the processing chamber (1) Thermal distortion over a wide range in the processing chamber (1) due to overheating of the main body and the insulating material in the vicinity thereof, or overheating of the power feeding section (9) and the electrode plates (2) and (3) themselves. Although there was a problem such as heat deterioration due to heat and the like, an internal electrode type low temperature plasma processing device connected to one end of the plasma generating electrode by using a cable with external shield such as a coaxial cable or a balanced type cable as a power supply line. Tried and fed The reflection at the connection point between the electrode and the electrode will be small, the standing wave generated on the power supply line will be small, the local overheating of the power supply line will be eliminated, and the plasma will be localized in the generating electrode and generate unnecessary plasma. There is no such effect.

発明が解決しようとする問題点 このような低温プラズ処理装置では、プラズマ発生電極
間で発生するプラズマが、給電側とその反対側で強度で
異なり、処理効果も不均一となるという問題が認められ
る。特に布帛やフィルム等の処理の場合、大面積あるい
は大容量のプラズマが要求され、工業規模では装置が大
型になるが、均一で大規模なプラズマを高周波放電で発
生することは、周波数が高くなり、波長が短くなるとと
もに、あるいは装置が大型になるとともに困難になって
くる。
Problems to be Solved by the Invention In such a low-temperature plasma processing apparatus, there is a problem in that the plasma generated between the plasma generating electrodes differs in intensity between the power supply side and the opposite side, and the processing effect becomes nonuniform. . Particularly in the case of processing fabrics and films, a large area or a large volume of plasma is required, and the device becomes large on an industrial scale, but generating a uniform and large-scale plasma by high-frequency discharge increases the frequency. However, it becomes difficult as the wavelength becomes shorter or the device becomes larger.

上記のような、外部がシールドされた給電線を、一端縁
部へ接続したプラズマ発生電極面上の高周波の動きを考
えると、給電線が接続される電極の端縁部(以下給電端
部という。)から高周波の進行(進行波)が始まるが、
反対側の端縁部(以下終端部という。)では電路が開放
されているため、到達した高周波は反射され逆方向に進
む。この反射波と進行波が電極面上で合成され、定在波
が生じる。電極の終端部は電気的には開放端であるため
電流は流れ得ず、電流の有する磁界のエネルギーは全て
電界のエネルギーに変り、したがって電圧は進行波の2
倍の値となり、給電端部に向って電圧が降下する。した
がって電極終端部で発生するプラズマが最大で、給電端
部に向って弱くなり、プラズマ強度に勾配が生じる。こ
の勾配が生じることは、電極の終端部開放の場合避けら
れない現象である。
Considering the movement of the high frequency on the surface of the plasma generating electrode in which the externally shielded power supply line is connected to one end edge as described above, the edge part of the electrode to which the power supply line is connected (hereinafter referred to as the power supply end part). High-frequency wave (traveling wave) starts from.
Since the electric path is open at the edge portion on the opposite side (hereinafter referred to as the terminal portion), the high frequency waves that have arrived are reflected and travel in the opposite direction. The reflected wave and the traveling wave are combined on the electrode surface to generate a standing wave. Since the terminal end of the electrode is electrically open, no current can flow, and the energy of the magnetic field possessed by the current changes to the energy of the electric field.
The value is doubled, and the voltage drops toward the feeding end. Therefore, the maximum plasma generated at the electrode terminal end becomes weaker toward the power supply end, and a gradient occurs in the plasma intensity. The occurrence of this gradient is an unavoidable phenomenon when the terminal end of the electrode is opened.

本発明は、上記のような問題を解決するものであって、
大規模なプラズマ発生電極を用いた低温プラズマ発生装
置でも、均一な低温プラズマを発生することができる低
温プラズマの均一化方法を提供しようとするものであ
る。
The present invention is to solve the above problems,
It is an object of the present invention to provide a low-temperature plasma homogenizing method capable of generating a uniform low-temperature plasma even in a low-temperature plasma generator using a large-scale plasma generating electrode.

なお本発明において、大規模なプラズマ発生電極とは、
電極の幅および長さが高周波の波長(λ)のおよそ1/50
以上のものをいう。また均一とは、不均一さが実用上差
支えない位に小さいという意味である。
In the present invention, the large-scale plasma generating electrode means
The width and length of the electrode is approximately 1/50 of the high frequency wavelength (λ)
The above is said. Further, “uniform” means that the non-uniformity is so small that it is practically acceptable.

問題点を解決するための手段 上記の問題点を解決するため本発明の低温プラズマの均
一化方法は、外部がシールドされた給電線をプラズマ発
生電極の一端縁部に接続した内部電極高周波放電型低温
プラズマ処理装置において、前記プラズマ発生電極の給
電線との接続点の反対側の端縁部に、一端側を短絡した
外部がシールドされた長さがケーブル上波長の1/4以下
のケーブルの他端側を接続することを特徴とするもので
ある。
Means for Solving the Problems In order to solve the above-mentioned problems, a method for homogenizing low temperature plasma according to the present invention is a high frequency discharge type internal electrode in which an externally shielded feed line is connected to one edge of a plasma generating electrode. In the low-temperature plasma processing apparatus, the edge portion on the opposite side of the connection point with the power supply line of the plasma generating electrode, the length of the external shielded one end side is 1/4 or less of the wavelength on the cable The other end is connected.

作 用 本発明の上記構成の低圧力高周波放電において、外部が
シールドされた同軸ケーブルまたは平衡型ケーブルの一
端側を短絡し(以下短絡ケーブルという。)、その他端
側をプラズマ発生電極の終端部に接続すると、プラズマ
発生電極上の電流と電圧の分布を最適化することができ
る。すなわちケーブル短絡端の電圧は零で、電極の終端
部および給電端部に向って電圧が上昇する。電極面上の
電圧定在波は、電極終端部開放時の定在波と短絡ケーブ
ルによる定在波の二者を合成したものであるから、その
合成された定在波の波腹が電極の中央もしくはその付近
に位置するようにすると、プラズマの発生の勾配が解消
されることになる。そのためには、電極終端部に接続す
る短絡ケーブルの長さをケーブル上波長の1/4以内の範
囲で調整することにより、電極面上の定在波の波腹の位
置を、プラズマの発生が均一となる点(ほぼ電極の中央
部)に設定すればよい。
Operation In the low-pressure high-frequency discharge having the above-described structure of the present invention, one end of a coaxial cable or a balanced cable whose outside is shielded is short-circuited (hereinafter referred to as a short-circuit cable), and the other end is a terminal portion of the plasma generating electrode. Once connected, the distribution of current and voltage on the plasma generating electrode can be optimized. That is, the voltage at the cable short-circuit end is zero, and the voltage increases toward the terminal end of the electrode and the power supply end. The voltage standing wave on the electrode surface is a combination of the standing wave when the terminal end of the electrode is open and the standing wave due to the short-circuit cable. If it is located at or near the center, the gradient of plasma generation will be eliminated. To this end, by adjusting the length of the short-circuit cable connected to the terminal end of the electrode within the range of 1/4 of the wavelength on the cable, the position of the antinode of the standing wave on the electrode surface can be controlled so that plasma is It may be set at a uniform point (approximately the center of the electrode).

実施例 本発明の実施例について説明する。第1図は本発明を実
施するプラズマ発生電極を用いたシート状物処理の低温
プラズマ処理装置の一例を示す。第1図(A),(B)
において、真空を保持し得るようにした処理室(11)内
に、垂直状に立設した高電圧印加電極板(12)の両側
に、一定間隔を隔てて前記高電圧印加電極(12)より面
積が大きい接地電極板(13a),(13b)を平行に対向し
て配置したプラズマ発生電極(14)が配設され、高周波
電源装置(15)から送られる高周波電力が整合器(16)
から外部が接地シールドされた同軸ケーブル(または平
衡型ケーブル)からなる給電線(17)を経て前記プラズ
マ発生電極(14)へ給電される。その給電線(17)は、
第2図にも示すごとくプラズマ発生電極(14)の一端縁
部(給電端部)(14a)に接続されている。すなわち外
部がシールドされた同軸ケーブルからなる給電線(17)
の外部導体、すなわちシールド側導体(17a),(17b)
がそれぞれ対応する接地電極板(13a),(13b)に、ま
た内部導体(17c)が高電圧印加電極板(12)に、いず
れも最短距路で接続されている。さらにプラズマ発生電
極(14)の給電線(17)との接続点を設けた給電端部
(14a)の反対側の端縁部(終端部)(14b)に、同軸ケ
ーブル(18)を、一端側(18a)を短絡してその他端側
(18b)で接続している。その接続の態様は給電線(1
7)の場合と全く同様である。次に処理室(11)内は、
被処理シート状物(19)を真空シールされた入口(20
a)から供給ローラ(21a)により送込み、ガイドローラ
(22a),(22b),(22c),(22d),(22e),(22
f),(22g)を経て両電極(12),(13a)間および(1
2),(13b)間を通過させて、同じく真空シールされた
出口(20b)から巻取ローラ(21b)により引出して巻取
るよう配備する。また処理室(11)は排気口(23a)か
ら排気し、所定の圧力を保ちつつ空気、酸素、窒素等の
処理ガスを吸気口(23b)から連続供給する。
Example An example of the present invention will be described. FIG. 1 shows an example of a low temperature plasma processing apparatus for processing a sheet-like material using a plasma generating electrode according to the present invention. Figure 1 (A), (B)
In a processing chamber (11) capable of holding a vacuum, both sides of a high voltage applying electrode plate (12) standing upright are separated from the high voltage applying electrode (12) at regular intervals. A plasma generating electrode (14) in which ground electrode plates (13a) and (13b) having a large area are arranged in parallel and opposite to each other is provided, and high frequency power sent from the high frequency power supply device (15) is matched by a matching box (16).
Is supplied to the plasma generating electrode (14) through a power supply line (17) composed of a coaxial cable (or a balanced type cable) the outside of which is grounded and shielded. The feeder line (17)
As shown in FIG. 2, the plasma generating electrode (14) is connected to one end edge (feed end) (14a). That is, the feeder line (17) consisting of a coaxial cable with the outside shielded.
Outer conductor, ie shield side conductor (17a), (17b)
Are connected to the corresponding ground electrode plates (13a) and (13b), respectively, and the internal conductor (17c) is connected to the high voltage applying electrode plate (12) by the shortest path. Further, connect the coaxial cable (18) to one end at the edge (termination) (14b) opposite to the feeding end (14a) where the connection point of the plasma generating electrode (14) with the feeding line (17) is provided. The side (18a) is short-circuited and the other end side (18b) is connected. The connection mode is the power supply line (1
This is exactly the same as in 7). Next, in the processing room (11),
Vacuum-sealed inlet (20) for the sheet (19) to be treated
It is fed from a) by a supply roller (21a), and guide rollers (22a), (22b), (22c), (22d), (22e), (22).
f), (22g), and between both electrodes (12), (13a) and (1
2) and (13b) are passed through, and the outlet (20b), which is also vacuum-sealed, is pulled out by the winding roller (21b) and wound up. Further, the processing chamber (11) is evacuated from the exhaust port (23a) and continuously supplies a processing gas such as air, oxygen and nitrogen from the intake port (23b) while maintaining a predetermined pressure.

上記の低温プラズマ処理装置を使用してポリエステル加
工糸織物を下記の条件で低温プラズマ処理した。
Using the above-mentioned low-temperature plasma treatment device, the polyester textured yarn fabric was subjected to low-temperature plasma treatment under the following conditions.

(条件)被処理布帛…ポリエステル加工糸織物(経15
0D,110本/吋;緯150D×2,55本/吋) 処理ガス……酸素 処理ガス流量…4/min 真空度…0.5Torr 処理速度…100cm/min 高周波電源装置周波数…13.56MHz 高周波電源装置自由空間波長…22m 高周波電源装置出力…2KW 電極寸法(接地電極)…長さ900mm,幅2000mm 電極間隔…60mm 短絡同軸ケーブル長さ…1000mm また比較例として、第1図の装置を短絡した同軸ケーブ
ル(18)を接続しない状態で用いて、上記実施例と同一
布帛を同一プラズマ処理条件で処理した。
(Conditions) Treated fabric: Polyester processed yarn fabric (War 15
0 D , 110 lines / inch; Weft 150 D × 2,55 lines / inch) Processing gas …… Oxygen Processing gas flow rate ・ ・ ・ 4 / min Vacuum degree ・ ・ ・ 0.5 Torr Processing speed ・ ・ ・ 100cm / min High frequency power supply frequency ・ ・ ・ 13.56MHz High frequency Power supply device Free space wavelength: 22 m High frequency power supply output: 2 KW Electrode dimensions (ground electrode): Length 900 mm, width 2000 mm Electrode spacing: 60 mm Short-circuited coaxial cable length: 1000 mm As a comparative example, the device of Fig. 1 was short-circuited. The same fabric as the above example was treated under the same plasma treatment conditions using the coaxial cable (18) without being connected.

上記実施例および比較例で得た処理織物の吸水性をJISL
−1096(バイレック法)により織物の幅方向に測定し
た。その結果は第3図に示すとおりであり、第1図の装
置を使用した実施例の場合、織物の幅方向に均一で、か
つすぐれた吸水性能が付与された。これに対し、短絡し
た同軸ケーブルを接続しない比較例の場合、織物の吸水
性能は幅方向に不均一で、プラズマ発生電極の給電線を
接続した給電端部に対応する端(耳)部が最も低く、反
対側端部に向って高くなっており、好ましくなかった。
これらの結果からも明らかなごとく、実施例ではプラズ
マ発生状態が極めて均一かつ高効率であり、均一なプラ
ズマ処理を行なうことができた。
The water absorption of the treated fabrics obtained in the above examples and comparative examples is JIS L
It was measured in the width direction of the fabric by -1096 (Bayrec method). The results are shown in FIG. 3, and in the case of the example using the apparatus of FIG. 1, uniform and excellent water absorption performance was imparted in the width direction of the fabric. On the other hand, in the case of the comparative example in which the short-circuited coaxial cable is not connected, the water absorption performance of the fabric is uneven in the width direction, and the end (ear) corresponding to the power supply end to which the power supply line of the plasma generation electrode is connected is the most It was low and increased toward the opposite end, which was not preferable.
As is clear from these results, in the example, the plasma generation state was extremely uniform and highly efficient, and uniform plasma treatment could be performed.

本発明において、上記のごとく低温プラズマ処理装置
の、プラズマ発生電極に対して給電線との接続点の反対
側の終端部に、短絡ケーブルを接続することにより、プ
ラズマ発生電極で発生するプラズマが均一化されるが、
その程度は上記のごとく電極面上の合成された定在波の
波腹の位置によって変り、電極のできるだけ中央付近に
位置させることにより、均一化がより向上する。それ
は、他の条件が同一の場合接続する短絡ケーブルの長さ
をケーブル上波長の1/4以内の範囲で調整することによ
り達成することができる。第1図で示す実施例では短絡
ケーブルは1本接続しているが、必要に応じて複数本接
続してもよい。
In the present invention, as described above, in the low temperature plasma processing apparatus, by connecting the short-circuit cable to the terminal end on the side opposite to the connection point with the power supply line with respect to the plasma generation electrode, the plasma generated at the plasma generation electrode is made uniform. Will be
The degree thereof varies depending on the position of the antinode of the combined standing wave on the electrode surface as described above, and the homogenization is further improved by positioning the electrode as close to the center as possible. This can be achieved by adjusting the length of the short-circuit cable to be connected under other conditions being the same, within a range of 1/4 of the wavelength on the cable. Although one short-circuit cable is connected in the embodiment shown in FIG. 1, a plurality of short-circuit cables may be connected if necessary.

なお本発明の片側短絡ケーブルに代えて、片側開放で長
さがケーブル上波長の1/4〜1/2のケーブル、あるいは集
中定数のインダクタンスを用いることができる。
Instead of the one-sided short-circuited cable of the present invention, it is possible to use a cable that is open on one side and has a length of 1/4 to 1/2 of the wavelength on the cable or a lumped constant inductance.

発明の効果 本発明によれば、外部がシールドされた給電線をプラズ
マ発生電極の一端縁部に接続した内部電極高周波放電型
低温プラズマ処理装置において、プラズマ発生電極の給
電線の接続点の反対側に、一端を短絡した同軸ケーブル
あるいは平衡型ケーブル等の外部をシールドされた長さ
がケーブル上波長の1/4以内のケーブルを他端側に接続
することにより、プラズマ発生電極上に極めて均一なプ
ラズマを高効率で得ることができ、極めて均一な処理を
行なうことができる。
EFFECTS OF THE INVENTION According to the present invention, in the internal electrode high frequency discharge type low temperature plasma processing apparatus in which the externally shielded power supply line is connected to the one end edge of the plasma generation electrode, the side opposite to the connection point of the power generation line of the plasma generation electrode. In addition, by connecting a cable with a shielded length such as a coaxial cable or a balanced type cable with one end short-circuited within 1/4 of the wavelength on the cable to the other end side, it is possible to achieve a very uniform distribution on the plasma generating electrode. Plasma can be obtained with high efficiency, and extremely uniform treatment can be performed.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の実施例で用いる低温プラズマ処理装置
を示し、(A)は概略側面図、(B)は(A)のI−I
線断面図、第2図は第1図のプラズマ発生電極の要部の
平面図、第3図は低温プラズマ処理織物の吸水性能値を
示す線図、第4図は従来装置を示し、(A)は概略側面
図、(B)は概略正面図、(C)は概略平面図である。 (11)……処理室、(12)……高電圧印加電極板、(13
a),(13b)……接地電極板、(14)……プラズマ発生
電極、(15)……高周波電源装置、(17)……給電線、
(18)……短絡ケーブル。
FIG. 1 shows a low temperature plasma processing apparatus used in an embodiment of the present invention, (A) is a schematic side view, and (B) is II of (A).
2 is a plan view of the main part of the plasma generating electrode of FIG. 1, FIG. 3 is a diagram showing the water absorption performance value of the low temperature plasma treated fabric, and FIG. ) Is a schematic side view, (B) is a schematic front view, and (C) is a schematic plan view. (11) …… Processing chamber, (12) …… High voltage application electrode plate, (13
a), (13b) …… ground electrode plate, (14) …… plasma generating electrode, (15) …… high frequency power supply, (17) …… feeding line,
(18) …… Short-circuit cable.

───────────────────────────────────────────────────── フロントページの続き (72)発明者 大口 保友 兵庫県姫路市北新在家3丁目1−16 (72)発明者 堤 四郎 大阪府豊中市上新田1丁目24番地 G− 208 (72)発明者 高橋 正克 京都府宇治市宇治小桜23 ユニチカ株式会 社中央研究所内 (72)発明者 石徹白 博司 和歌山県和歌山市和歌浦東2丁目1−18 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Inventor Yasutomo Oguchi, 3-16, Kitashinke, Himeji-shi, Hyogo (72) Inventor Shiro Tsutsumi, 24-24 Kaminita, Toyonaka, Osaka G-208 (72) Inventor Masakatsu Takahashi 23 Uji-kozakura, Uji-shi, Kyoto Unit Central Research Institute, Unitika Ltd. (72) Inventor Hiroshi Ishitohaku 2-18 Wakaura East, Wakayama City, Wakayama Prefecture

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】外部がシールドされた給電線をプラズマ発
生電極の一端縁部に接続した内部電極高周波放電型低温
プラズマ処理装置において、前記プラズマ発生電極の給
電線との接続点の反対側の端縁部に、一端側を短絡した
外部がシールドされた長さがケーブル上波長の1/4以下
のケーブルの他端側を接続することを特徴とする低温プ
ラズマの均一化方法。
1. An internal electrode high frequency discharge type low temperature plasma processing apparatus in which an externally shielded power supply line is connected to one edge of a plasma generation electrode, the end of the plasma generation electrode opposite to the connection point with the power supply line. A method for homogenizing low-temperature plasma, characterized in that the other end of a cable having an externally shielded length with one end short-circuited and having a length of 1/4 or less of the wavelength on the cable is connected to the edge portion.
JP61270444A 1986-11-13 1986-11-13 Method for homogenizing low-temperature plasma Expired - Fee Related JPH0796704B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61270444A JPH0796704B2 (en) 1986-11-13 1986-11-13 Method for homogenizing low-temperature plasma

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61270444A JPH0796704B2 (en) 1986-11-13 1986-11-13 Method for homogenizing low-temperature plasma

Publications (2)

Publication Number Publication Date
JPS63125671A JPS63125671A (en) 1988-05-28
JPH0796704B2 true JPH0796704B2 (en) 1995-10-18

Family

ID=17486370

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61270444A Expired - Fee Related JPH0796704B2 (en) 1986-11-13 1986-11-13 Method for homogenizing low-temperature plasma

Country Status (1)

Country Link
JP (1) JPH0796704B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102005002674B4 (en) * 2005-01-11 2012-10-04 Forschungs- Und Applikationslabor Plasmatechnik Gmbh Dresden Apparatus for plasma-chemical vapor deposition on substrates in a vacuum

Also Published As

Publication number Publication date
JPS63125671A (en) 1988-05-28

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