JP2001210495A - Plasma treatment device and plasma treatment method - Google Patents

Plasma treatment device and plasma treatment method

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Publication number
JP2001210495A
JP2001210495A JP2000019404A JP2000019404A JP2001210495A JP 2001210495 A JP2001210495 A JP 2001210495A JP 2000019404 A JP2000019404 A JP 2000019404A JP 2000019404 A JP2000019404 A JP 2000019404A JP 2001210495 A JP2001210495 A JP 2001210495A
Authority
JP
Japan
Prior art keywords
substrate
electrode
frequency
mounting surface
processed
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.)
Pending
Application number
JP2000019404A
Other languages
Japanese (ja)
Inventor
Mitsuhiro Yoshinaga
光宏 吉永
Shiyuushin Amano
修臣 天野
Masaki Suzuki
正樹 鈴木
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co 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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP2000019404A priority Critical patent/JP2001210495A/en
Publication of JP2001210495A publication Critical patent/JP2001210495A/en
Pending legal-status Critical Current

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  • Plasma Technology (AREA)
  • Chemical Vapour Deposition (AREA)
  • ing And Chemical Polishing (AREA)
  • Drying Of Semiconductors (AREA)

Abstract

PROBLEM TO BE SOLVED: To reduce the potential difference at a base board placing surface of an electrode which places the treated base board, and to enable the treated base board to treat a plasma evenly. SOLUTION: A lower electrode 5 placing the treated base board 4 is formed in conical shape that the opposite side against the base board placing surface 5a reduces the diameter, and a high-frequency impressing part 5b is connected to the apex part of the one. By the above, as the distance from the high-frequency impressing part 5b becomes nearly even at the whole part of the base board placing surface 5a, a high-frequency 11 reaches the whole part of the base board placing surface 5a almost simultaneously, accordingly, the phase shift and the potential difference caused by the phase shift between center part and peripheral part of the base board placing surface 5a is reduced.

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、半導体や液晶表示
素子(LCD)の製造に用いられるドライエッチング装
置、スパッタ装置、CVD装置などのプラズマ処理装置
およびプラズマ処理方法に関し、特にドライエッチング
処理で基板上における均一性の向上を図ることができる
プラズマ処理装置およびプラズマ処理方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a plasma processing apparatus and a plasma processing method such as a dry etching apparatus, a sputtering apparatus, and a CVD apparatus used for manufacturing a semiconductor or a liquid crystal display device (LCD). The present invention relates to a plasma processing apparatus and a plasma processing method capable of improving the above uniformity.

【0002】[0002]

【従来の技術】近年、半導体や液晶基板の製造工程にお
いて高集積化、大口径化が進行し、さらなる微細パター
ンでのプラズマ処理への技術的要求がますます高まって
来ている。この技術的要求とは、半導体エッチング工程
を例に取ると、エッチング・マスクや下地材料層に対す
る高選択性、良好な形状制御性、実用的なエッチング速
度、低ダメージ性、良好な再現性の達成である。これら
の条件をウエハ全面についてクリアすることがデバイス
の歩留まり向上や性能の向上に繋がる。これにはウエハ
全面に渡ってプラズマ処理を均一に実施する必要があ
り、そのために従来よりさまざまな方法が取られてき
た。
2. Description of the Related Art In recent years, in the manufacturing process of semiconductors and liquid crystal substrates, high integration and large diameter have been progressing, and technical requirements for plasma processing with further finer patterns have been increasing more and more. The technical requirements are, for example, in the case of a semiconductor etching process, achieving high selectivity to an etching mask and an underlying material layer, good shape controllability, a practical etching rate, low damageability, and good reproducibility. It is. Clearing these conditions on the entire surface of the wafer leads to an improvement in device yield and performance. For this purpose, it is necessary to perform the plasma processing uniformly over the entire surface of the wafer, and various methods have been conventionally used for that purpose.

【0003】従来のプラズマ処理装置には、図3に示す
ようなエッチング装置がある。このエッチング装置で
は、真空容器21内の上部に上部電極22を配設し、こ
の上部電極22の下方に被処理基板23を載置する下部
電極24を配設しており、真空排気ポンプ25により真
空排気し、上部電極22に形成したガス流路22a,ガ
ス吹出口22bを通じて反応ガス26を導入しつつ所定
圧力に制御している。そしてその状態において、下部電
極24の高周波印加部24aにコンデンサ27を介し高
周波電源28より高周波電力を印加して真空容器21内
にプラズマを励起し、プラズマ中に存在するラジカル・
イオンによって被処理基板23をエッチングしている。
As a conventional plasma processing apparatus, there is an etching apparatus as shown in FIG. In this etching apparatus, an upper electrode 22 is provided in an upper portion of a vacuum vessel 21, and a lower electrode 24 on which a substrate 23 is placed is provided below the upper electrode 22. The system is evacuated and controlled to a predetermined pressure while introducing a reaction gas 26 through a gas passage 22 a and a gas outlet 22 b formed in the upper electrode 22. Then, in this state, high-frequency power is applied from a high-frequency power supply 28 to the high-frequency application section 24a of the lower electrode 24 via the capacitor 27 to excite plasma in the vacuum vessel 21, and radicals existing in the plasma are excited.
The substrate 23 to be processed is etched by the ions.

【0004】[0004]

【発明が解決しようとする課題】ところが、上記したエ
ッチング装置を始めとする従来のプラズマ処理装置で
は、図示したように、被処理基板23を載置する下部電
極24は基板載置面24bの面積に比べて厚みが小さ
く、全面に渡ってほぼ平坦な円盤型または平板の形状を
しており、その下面の中央部またはその近傍に高周波印
加部24aが設定されていて、被処理基板23に入射す
るイオンのエネルギーが被処理基板23の中央部と外周
部で異なる点について考慮されていなかった。
However, in a conventional plasma processing apparatus such as the above-described etching apparatus, as shown in the drawing, the lower electrode 24 on which the substrate 23 to be processed is mounted has an area of the substrate mounting surface 24b. The high-frequency applying portion 24a is set at the center of the lower surface or in the vicinity thereof, and is incident on the substrate 23 to be processed. No consideration was given to the fact that the energy of the ions to be processed differs between the central portion and the outer peripheral portion of the substrate 23 to be processed.

【0005】つまり、このような下部電極24では、高
周波印加部24aから基板載置面24bの中央部までの
距離L11と外周部までの距離L12との差は、電極厚
み一定と仮定すると、基板載置面24bが大口径化する
につれ大きくなる。そのため、基板載置面24b上に到
達する高周波は、同一時間で見れば、高周波印加部24
aからの距離に応じて異なり、基板載置面24bの中央
部と外周部で位相がずれ、その結果、基板載置面24b
の中央部で電位が低く外周部で電位が高くなる傾向が見
られる。これは、他の部分からの高周波により干渉を起
こしているからであり、また下部電極24の大きさによ
っては電極上で定在波が生じているからであると思われ
る。そして、この基板載置面24b上の電位差が原因
で、被処理基板23上に到達するイオンのエネルギーが
不均一になる。この傾向は下部電極24が大きくなるほ
ど顕著である。
That is, in such a lower electrode 24, assuming that the difference between the distance L11 from the high-frequency applying portion 24a to the center of the substrate mounting surface 24b and the distance L12 from the outer peripheral portion is constant, the electrode thickness is constant. It becomes larger as the mounting surface 24b becomes larger in diameter. Therefore, the high-frequency wave reaching the substrate mounting surface 24b is viewed at the same time, and the high-frequency
The phase differs between the central portion and the outer peripheral portion of the substrate mounting surface 24b, and as a result, the substrate mounting surface 24b
Tend to be lower at the center and higher at the outer periphery. This is considered to be because interference is caused by high frequencies from other parts, and a standing wave is generated on the electrode depending on the size of the lower electrode 24. Then, due to the potential difference on the substrate mounting surface 24b, the energy of ions reaching the substrate 23 to be processed becomes non-uniform. This tendency becomes more remarkable as the size of the lower electrode 24 increases.

【0006】そのため、均一なプラズマを生成しても、
プラズマ処理速度は被処理基板23面内で不均一になる
という問題があった。本発明は上記問題を解決するもの
で、被処理基板を載置する電極の基板載置面での電位差
を低減することができ、被処理基板を均一にプラズマ処
理できるプラズマ処理装置およびプラズマ処理方法を提
供することを目的とするものである。
Therefore, even if uniform plasma is generated,
There is a problem that the plasma processing speed is not uniform in the surface of the substrate 23 to be processed. SUMMARY OF THE INVENTION The present invention solves the above-described problems, and can reduce a potential difference between an electrode on which a substrate to be processed is mounted on a substrate mounting surface, and can uniformly perform plasma processing on the substrate to be processed and a plasma processing method. The purpose is to provide.

【0007】[0007]

【課題を解決するための手段】本発明は上記目的を達成
するために、高周波印加点から基板載置面までの距離が
基板載置面の全面において均一になるように電極形状を
コーン状またはそれに近い形にしたものであり、それに
より基板載置面に内周部であるか外周部であるかに関わ
らず同一位相の高周波が到達するよう構成したものであ
る。
According to the present invention, in order to achieve the above object, the shape of the electrode is cone-shaped or cone-shaped so that the distance from the high-frequency application point to the substrate mounting surface is uniform over the entire surface of the substrate mounting surface. This is a shape close to that, whereby the high frequency of the same phase reaches the substrate mounting surface regardless of whether it is the inner peripheral portion or the outer peripheral portion.

【0008】[0008]

【発明の実施の形態】請求項1記載の発明は、真空容器
の内部に被処理基板を載置する電極を配設し、前記電極
と対向電極との間に印加する高周波電力によりプラズマ
を発生させ被処理基板を処理するプラズマ処理装置にお
いて、前記電極は、基板載置面に背反する側が縮径した
コーン状に形成し、その頂部に高周波電力が印加される
高周波印加部を設けたことを特徴とする。
According to the first aspect of the present invention, an electrode for mounting a substrate to be processed is disposed inside a vacuum vessel, and plasma is generated by high-frequency power applied between the electrode and a counter electrode. In the plasma processing apparatus for processing the substrate to be processed, the electrode is formed in a cone shape having a diameter reduced on a side opposite to the substrate mounting surface, and a high-frequency application unit to which high-frequency power is applied is provided at the top. Features.

【0009】上記構成により、高周波印加部からの距離
が基板載置面の全面において均一に近づくため、高周波
は基板載置面の全面においてほぼ同等な時間に到達する
ことになり、基板載置面の中央部と外周部とにおける高
周波の位相のずれ、それに起因する電位差を小さくする
ことができ、プラズマ処理を均一に行うことが可能にな
る。コーン状としては、円錐状、三角錐状、四角錐状
や、それに近い形状など、種々可能である。
According to the above configuration, since the distance from the high-frequency application section uniformly approaches the entire surface of the substrate mounting surface, the high-frequency waves arrive at substantially the same time over the entire surface of the substrate mounting surface. Of the high-frequency phase between the central portion and the outer peripheral portion, and the potential difference resulting therefrom can be reduced, and the plasma processing can be performed uniformly. As the cone shape, various shapes such as a conical shape, a triangular pyramid shape, a quadrangular pyramid shape, and a shape close thereto are possible.

【0010】請求項2記載の発明は、請求項1記載の構
成において、コーン状の電極の内部に誘電率不均一部を
形成したことを特徴とする。上記構成により、高周波は
誘電率不均一部で速度や向きを変えて基板載置面に到達
することになり、基板載置面の中央部と外周部とにおけ
る高周波の位相のずれがより小さくなる。
According to a second aspect of the present invention, in the configuration of the first aspect, a non-uniform dielectric constant portion is formed inside the cone-shaped electrode. With the above configuration, the high frequency wave reaches the substrate mounting surface by changing the speed and direction at the non-uniform dielectric constant portion, and the phase shift of the high frequency in the central portion and the outer peripheral portion of the substrate mounting surface becomes smaller. .

【0011】請求項3記載の発明は、請求項2記載の構
成において、誘電率不均一部が空隙部であることを特徴
とする。上記構成により、高周波は誘電率不均一部で速
度や向きを変えて基板載置面に到達することになる。
According to a third aspect of the present invention, in the configuration of the second aspect, the non-uniform dielectric constant portion is a void portion. According to the above configuration, the high frequency wave reaches the substrate mounting surface while changing the speed and direction at the portion having the non-uniform dielectric constant.

【0012】請求項4記載の発明は、真空容器の内部に
配設したコーン状の電極の基板載置面に被処理基板を載
置し、反応ガスを供給しつつ、前記電極の頂部に設けた
高周波印加部に高周波電力を印加して基板載置面まで伝
播させ、対向電極との間で発生するプラズマにより被処
理基板を処理することを特徴とする。
According to a fourth aspect of the present invention, a substrate to be processed is mounted on a substrate mounting surface of a cone-shaped electrode provided inside a vacuum vessel, and is provided on the top of the electrode while supplying a reaction gas. And applying the high-frequency power to the high-frequency applying unit and transmitting the high-frequency power to the substrate mounting surface, and processing the substrate to be processed by the plasma generated between the high-frequency applying unit and the counter electrode.

【0013】上記構成により、高周波は高周波印加部か
ら基板載置面の各位置までほぼ均一な距離を伝播して同
等な時間に到達することになり、基板載置面の中央部と
外周部とにおける高周波の位相のずれ、それに起因する
電位差を小さくすることができ、プラズマ処理を均一に
行うことが可能になる。
With the above structure, the high-frequency wave propagates over a substantially uniform distance from the high-frequency applying section to each position on the substrate mounting surface and arrives at the same time, so that the central portion and the outer peripheral portion of the substrate mounting surface are separated from each other. , The potential difference caused by the phase shift of the high frequency can be reduced, and the plasma processing can be performed uniformly.

【0014】以下、本発明の実施の形態を図面を参照し
ながら具体的に説明する。 (実施の形態1)本発明の実施の形態1におけるプラズ
マ処理装置としてドライエッチング工程のRIE(反応
性イオンエッチング)装置を説明する。
Hereinafter, embodiments of the present invention will be specifically described with reference to the drawings. (Embodiment 1) An RIE (reactive ion etching) apparatus in a dry etching step will be described as a plasma processing apparatus according to Embodiment 1 of the present invention.

【0015】図1において、1は真空容器、2は真空容
器1内を真空排気する真空排気ポンプである。3は真空
容器1の内部に設置された上部電極であり、4は半導体
用シリコンウエハや液晶基板などの被処理基板であり、
5は上部電極3に対向して絶縁板6に載置された下部電
極である。
In FIG. 1, reference numeral 1 denotes a vacuum container, and 2 denotes a vacuum pump for evacuating the vacuum container 1. Reference numeral 3 denotes an upper electrode provided inside the vacuum vessel 1, reference numeral 4 denotes a substrate to be processed such as a semiconductor silicon wafer or a liquid crystal substrate,
Reference numeral 5 denotes a lower electrode placed on the insulating plate 6 so as to face the upper electrode 3.

【0016】上部電極3は、内部にガス流路3aを有し
下面に複数のガス吹出口3bを有しており、ガス供給口
3cにおいて外部のガス供給源(図示せず)に連通して
いる。7は上部電極3のためのアースである。
The upper electrode 3 has a gas passage 3a inside and a plurality of gas outlets 3b on the lower surface, and communicates with an external gas supply source (not shown) at a gas supply port 3c. I have. 7 is a ground for the upper electrode 3.

【0017】下部電極5はセラミックなどで製作されて
いて、基板設置面5aに静電吸着電極を備え、基板載置
面5aに背反する側が縮径したほぼ円錐台状をなし、そ
の頂部中央の高周波印加部5bにコンデンサ8などの整
合機を介して高周波電源9が接続している。
The lower electrode 5 is made of ceramic or the like, is provided with an electrostatic chucking electrode on the substrate mounting surface 5a, has a substantially truncated conical shape with a reduced diameter on the side opposite to the substrate mounting surface 5a, and has a central top portion. A high-frequency power supply 9 is connected to the high-frequency application unit 5b via a matching device such as a capacitor 8.

【0018】上記構成における作用を説明する。被処理
基板4を下部電極5の基板設置面5aに載せて静電吸着
させる。次いで、真空ポンプ2により真空容器1内の空
気を排気し、ガス供給源より供給される反応ガス(エッ
チングガス)10をガス供給口3c,ガス流路3a,ガ
ス吹出口3bを通じて真空容器1内に導入しつつ、所定
圧力に制御する。その後に、下部電極5の高周波印加部
5bにコンデンサ8を介して高周波電源9より高周波電
力を印加し、真空容器1内にプラズマを励起し、プラズ
マ中に存在するラジカル・イオンによって被処理基板4
をエッチングする。
The operation of the above configuration will be described. The target substrate 4 is placed on the substrate setting surface 5a of the lower electrode 5 and electrostatically attracted. Next, the air in the vacuum vessel 1 is exhausted by the vacuum pump 2, and the reaction gas (etching gas) 10 supplied from the gas supply source is supplied to the inside of the vacuum vessel 1 through the gas supply port 3c, the gas passage 3a, and the gas outlet 3b. While controlling to a predetermined pressure. Thereafter, high-frequency power is applied from a high-frequency power source 9 to a high-frequency application unit 5b of the lower electrode 5 via a capacitor 8 to excite plasma in the vacuum chamber 1, and radicals and ions present in the plasma cause the substrate 4 to be processed.
Is etched.

【0019】その際に、高周波電源9より高周波印加部
5bを印加ポイントとして下部電極5に印加された高周
波11は、下部電極5の内部や表面を伝わって基板載置
面5aに到達する。
At this time, the high frequency 11 applied to the lower electrode 5 from the high frequency power supply 9 with the high frequency applying section 5b as an application point reaches the substrate mounting surface 5a through the inside and the surface of the lower electrode 5.

【0020】この時、高周波印加部5bから基板載置面
5aまでの距離は、下部電極7が円錐台状であることに
よって、例えば中央部まではL1となり外周部まではL
2となり、両者L1,L2間の差は従来の円盤状の下部
電極に比べて少ない。このため、従来の円盤状の下部電
極とは異なって、基板載置面5aの全面にほぼ同位相の
高周波が伝達されることになり、基板載置面5a上の電
位は均一性が増し、また他の位置からの高周波の干渉や
定在波の影響は低減する。
At this time, since the lower electrode 7 has a truncated cone shape, the distance from the high-frequency application unit 5b to the substrate mounting surface 5a is, for example, L1 up to the center and L1 up to the outer periphery.
2 and the difference between the two electrodes L1 and L2 is smaller than that of the conventional disk-shaped lower electrode. For this reason, unlike the conventional disc-shaped lower electrode, high-frequency waves having substantially the same phase are transmitted to the entire surface of the substrate mounting surface 5a, and the potential on the substrate mounting surface 5a increases in uniformity. Further, the influence of high-frequency interference and standing waves from other positions is reduced.

【0021】その結果、被処理基板4に到達するイオン
エネルギーの均一性は向上し、被処理基板4は均一にプ
ラズマ処理される。 (実施の形態2)本発明の実施の形態2におけるプラズ
マ処理装置は、図2に示すように、上記実施の形態1で
説明したRIE装置において、下部電極5の内部に断面
が菱形の空隙部12を形成したものである。
As a result, the uniformity of the ion energy reaching the target substrate 4 is improved, and the target substrate 4 is uniformly plasma-processed. (Embodiment 2) As shown in FIG. 2, the plasma processing apparatus according to Embodiment 2 of the present invention is the same as the RIE apparatus described in Embodiment 1 except that the lower electrode 5 has a diamond-shaped void inside. 12 is formed.

【0022】この構成によれば、高周波11は空隙部1
2を廻り込んで基板載置面5aに到達するので、高周波
印加部5bから基板載置面5aまでの距離は、基板載置
面5aの全面においてより均一に近づき、基板載置面5
aの全面にほぼ同位相の高周波が伝達される。
According to this configuration, the high frequency 11 is applied to the gap 1
2 and arrives at the substrate mounting surface 5a, the distance from the high-frequency application section 5b to the substrate mounting surface 5a becomes more uniform over the entire surface of the substrate mounting surface 5a.
A high frequency wave having substantially the same phase is transmitted to the entire surface of a.

【0023】その結果、被処理基板4に到達するイオン
エネルギーの均一性はより向上し、被処理基板4は更に
均一にプラズマ処理される。なお、上記においてはRI
E装置を例にとって説明したが、スパッタ装置、CVD
(化学的気相成長)装置など、その他のプラズマ処理装
置でも、上記したような電極を用いることで同様の効果
が得られる。被処理基板4が上下方向に設置される場合
も、上記したような形状の電極を用いることで同様の効
果が得られる。
As a result, the uniformity of the ion energy reaching the substrate 4 to be processed is further improved, and the substrate 4 to be processed is more uniformly plasma-processed. In the above, RI
The E apparatus has been described as an example.
The same effect can be obtained in other plasma processing apparatuses such as a (chemical vapor deposition) apparatus by using the above-described electrodes. Even when the substrate 4 to be processed is installed in the vertical direction, the same effect can be obtained by using the electrodes having the above-described shapes.

【0024】また、基板載置面5aの全面にほぼ同位相
の高周波が伝達されるように、空隙部12の形状を紡錘
型など、種々変更してもよく、空隙部12に相当する部
分に、その外周部分とは誘電率が異なる材料を配置して
もよい。たとえば、空隙部12に相当する部分にセラミ
ックや流体(水、エチレングリコールなど)を配置し、
外周部分をアルミニウムとすることが可能である。
The shape of the gap 12 may be variously changed, such as a spindle type, so that high-frequency waves having substantially the same phase are transmitted to the entire surface of the substrate mounting surface 5a. Alternatively, a material having a different dielectric constant from the outer peripheral portion may be arranged. For example, a ceramic or a fluid (water, ethylene glycol, or the like) is arranged in a portion corresponding to the gap portion 12,
The outer periphery can be aluminum.

【0025】[0025]

【発明の効果】本発明によれば、以上の説明から明らか
なように、被処理基板を載置する電極をコーン状に形成
しその頂部に高周波印加部を設けることにより、高周波
印加部から伝達する高周波による電位を基板載置面の全
面において従来よりも均一化し、被処理基板の全面に均
一なエネルギーを入射させることができ、均一にプラズ
マ処理を行える。
According to the present invention, as is apparent from the above description, the electrode on which the substrate to be processed is mounted is formed in a cone shape, and the high frequency application section is provided on the top thereof, so that the transmission from the high frequency application section is achieved. Thus, the potential due to the high frequency is made more uniform over the entire surface of the substrate mounting surface than before, so that uniform energy can be incident on the entire surface of the substrate to be processed, and plasma processing can be performed uniformly.

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

【図1】本発明の実施の形態1におけるプラズマ処理装
置の概略構成を示す縦断面図である。
FIG. 1 is a longitudinal sectional view illustrating a schematic configuration of a plasma processing apparatus according to a first embodiment of the present invention.

【図2】本発明の実施の形態2におけるプラズマ処理装
置の概略構成を示す縦断面図である。
FIG. 2 is a longitudinal sectional view illustrating a schematic configuration of a plasma processing apparatus according to a second embodiment of the present invention.

【図3】従来のプラズマ処理装置の概略構成を示す縦断
面図である。
FIG. 3 is a longitudinal sectional view showing a schematic configuration of a conventional plasma processing apparatus.

【符号の説明】[Explanation of symbols]

1 真空容器 2 真空排気ポンプ 3 上部電極 4 被処理基板 5 下部電極 5a 基板設置面 5b 高周波印加部 9 高周波電源 10 反応ガス 11 高周波 12 空隙部 DESCRIPTION OF SYMBOLS 1 Vacuum container 2 Vacuum pump 3 Upper electrode 4 Substrate to be processed 5 Lower electrode 5a Substrate installation surface 5b High frequency application part 9 High frequency power supply 10 Reaction gas 11 High frequency 12 Void

───────────────────────────────────────────────────── フロントページの続き (51)Int.Cl.7 識別記号 FI テーマコート゛(参考) H01L 21/31 H01L 21/302 C (72)発明者 鈴木 正樹 大阪府門真市大字門真1006番地 松下電器 産業株式会社内 Fターム(参考) 4K030 CA04 CA06 DA04 FA03 KA15 LA15 LA18 4K057 DA16 DA20 DD03 DM03 DM06 DM08 DN01 5F004 AA01 BA04 BA06 BB29 BD04 BD05 5F045 AA08 BB02 DP02 EH04 EH08 EH13 ──────────────────────────────────────────────────続 き Continued on the front page (51) Int.Cl. 7 Identification symbol FI Theme coat ゛ (Reference) H01L 21/31 H01L 21/302 C (72) Inventor Masaki Suzuki 1006 Ojidoma, Kazuma, Osaka Matsushita Electric Industrial Incorporated F term (reference) 4K030 CA04 CA06 DA04 FA03 KA15 LA15 LA18 4K057 DA16 DA20 DD03 DM03 DM06 DM08 DN01 5F004 AA01 BA04 BA06 BB29 BD04 BD05 5F045 AA08 BB02 DP02 EH04 EH08 EH13

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 真空容器の内部に被処理基板を載置する
電極を配設し、前記電極と対向電極との間に印加する高
周波電力によりプラズマを発生させ被処理基板を処理す
るプラズマ処理装置において、 前記電極は、基板載置面に背反する側が縮径したコーン
状に形成し、その頂部に高周波電力が印加される高周波
印加部を設けたことを特徴とするプラズマ処理装置。
1. A plasma processing apparatus in which an electrode for mounting a substrate to be processed is disposed inside a vacuum vessel, and plasma is generated by high-frequency power applied between the electrode and a counter electrode to process the substrate to be processed. 3. The plasma processing apparatus according to claim 1, wherein the electrode is formed in a cone shape having a reduced diameter on a side opposite to the substrate mounting surface, and a high-frequency application unit to which high-frequency power is applied is provided at the top.
【請求項2】 コーン状の電極の内部に誘電率不均一部
を形成したことを特徴とする請求項1記載のプラズマ処
理装置。
2. The plasma processing apparatus according to claim 1, wherein a non-uniform dielectric constant portion is formed inside the cone-shaped electrode.
【請求項3】 誘電率不均一部が空隙部であることを特
徴とする請求項2記載のプラズマ処理装置。
3. The plasma processing apparatus according to claim 2, wherein the non-uniform dielectric constant portion is a void.
【請求項4】 真空容器の内部に配設したコーン状の電
極の基板載置面に被処理基板を載置し、反応ガスを供給
しつつ、前記電極の頂部に設けた高周波印加部に高周波
電力を印加して基板載置面まで伝播させ、対向電極との
間で発生するプラズマにより被処理基板を処理すること
を特徴とするプラズマ処理方法。
4. A substrate to be processed is mounted on a substrate mounting surface of a cone-shaped electrode provided inside a vacuum vessel, and a high-frequency application section provided on the top of the electrode is supplied with a reactive gas while supplying a reactive gas. A plasma processing method, comprising applying electric power to propagate to a substrate mounting surface, and processing a substrate to be processed by plasma generated between the substrate and a counter electrode.
JP2000019404A 2000-01-28 2000-01-28 Plasma treatment device and plasma treatment method Pending JP2001210495A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000019404A JP2001210495A (en) 2000-01-28 2000-01-28 Plasma treatment device and plasma treatment method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000019404A JP2001210495A (en) 2000-01-28 2000-01-28 Plasma treatment device and plasma treatment method

Publications (1)

Publication Number Publication Date
JP2001210495A true JP2001210495A (en) 2001-08-03

Family

ID=18546099

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000019404A Pending JP2001210495A (en) 2000-01-28 2000-01-28 Plasma treatment device and plasma treatment method

Country Status (1)

Country Link
JP (1) JP2001210495A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2018170183A (en) * 2017-03-30 2018-11-01 富士フイルム株式会社 Plasma generator

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2018170183A (en) * 2017-03-30 2018-11-01 富士フイルム株式会社 Plasma generator

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