JPH06188237A - Apparatus for forming plasma - Google Patents
Apparatus for forming plasmaInfo
- Publication number
- JPH06188237A JPH06188237A JP4335784A JP33578492A JPH06188237A JP H06188237 A JPH06188237 A JP H06188237A JP 4335784 A JP4335784 A JP 4335784A JP 33578492 A JP33578492 A JP 33578492A JP H06188237 A JPH06188237 A JP H06188237A
- Authority
- JP
- Japan
- Prior art keywords
- forming apparatus
- conductor line
- plasma forming
- line
- ground conductor
- 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
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- Plasma Technology (AREA)
- Physical Vapour Deposition (AREA)
- Drying Of Semiconductors (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明はプラズマ形成装置に係
り、特に、大口径の半導体基板のエッチングや薄膜堆積
等を行うのに好適なプラズマ形成装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a plasma forming apparatus, and more particularly to a plasma forming apparatus suitable for etching a large diameter semiconductor substrate or depositing a thin film.
【0002】[0002]
【従来の技術】従来、低真空で高密度なプラズマを形成
するために磁場とマイクロ波領域の電磁波により、それ
らの相乗作用でプラズマを形成する装置が用いられてい
た。これを有磁場マイクロ波プラズマと言う。しかし、
この従来装置にはプラズマを形成する放電管部分への電
磁波の照射が不均一になりやすく、特に使用する電磁波
の波長より口径の大きい領域にプラズマを形成しようと
する場合、その領域に均一なプラズマを形成することが
大変困難である。2. Description of the Related Art Conventionally, in order to form a high-density plasma in a low vacuum, an apparatus for forming a plasma by a synergistic effect of a magnetic field and an electromagnetic wave in a microwave region has been used. This is called magnetic field microwave plasma. But,
Irradiation of electromagnetic waves to the discharge tube portion that forms plasma tends to be nonuniform in this conventional device, and especially when trying to form plasma in a region having a diameter larger than the wavelength of the electromagnetic wave used, uniform plasma is generated in that region. Are very difficult to form.
【0003】[0003]
【発明が解決しようとする課題】本発明の目的は、有磁
場マイクロ波プラズマの利点を活かしたまま、従来装置
では困難であった、広い面積での均一なプラズマ形成を
実現することに有る。SUMMARY OF THE INVENTION An object of the present invention is to realize uniform plasma formation over a wide area, which has been difficult with a conventional apparatus, while utilizing the advantages of the magnetic field microwave plasma.
【0004】[0004]
【課題を解決するための手段】上記目的を達成するため
に本発明においては、接地導体基板と前記接地導体基板
と容量結合した導体線路により構成されるマイクロスト
リップ線路を用い、前記マイクロストリップ線路からの
漏れ電磁波を放電管に供給することによりプラズマを形
成させる。To achieve the above object, the present invention uses a microstrip line composed of a ground conductor substrate and a conductor line capacitively coupled to the ground conductor substrate. A leaked electromagnetic wave is supplied to the discharge tube to form plasma.
【0005】[0005]
【作用】マイクロストリップ線路をプラズマ形成領域に
均一に張り巡らせることにより、マイクロストリップ線
路からの漏洩電磁波がプラズマ形成領域に均一に照射さ
れ、広い面積に均一なプラズマを形成することが可能と
なる。By uniformly extending the microstrip line in the plasma formation region, the electromagnetic wave leaked from the microstrip line is uniformly irradiated to the plasma formation region, and uniform plasma can be formed in a wide area.
【0006】[0006]
【実施例】本発明の実施例を図1により説明する。図1
は本発明の基本構成の説明図である。主な構成は電磁石
1とその中心部に設置されている放電管2及び放電管2
に電磁波を供給する電磁波供給部3より構成される。こ
の電磁波供給部3からのマイクロ波領域の電磁波と電磁
石1による磁場との相乗作用により、放電管2中に導入
された原料ガスをプラズマ状態にすることができる。EXAMPLE An example of the present invention will be described with reference to FIG. Figure 1
FIG. 3 is an explanatory diagram of a basic configuration of the present invention. The main components are the electromagnet 1, the discharge tube 2 installed in the center of the electromagnet 1, and the discharge tube 2.
The electromagnetic wave supply unit 3 supplies electromagnetic waves to the. The source gas introduced into the discharge tube 2 can be made into a plasma state by the synergistic action of the electromagnetic wave in the microwave region from the electromagnetic wave supply unit 3 and the magnetic field of the electromagnet 1.
【0007】図2は電磁波供給部3の詳しい説明図であ
る。電磁波供給部3は円筒状の銅で形成され、端部の一
方が開放もう一方が銅の平板(以下、接地導体基板5と
する)で閉じた構造になっている。その内部には渦巻状
導体線路6が接地導体基板5に一定の間隔をおき、設置
されている。この渦巻状導体線路6の中心部は抵抗負荷
7を介し接地導体基板5に終端されている。また渦巻状
導体線路6の始点には外部からマイクロ波領域の電磁波
が給電されている。FIG. 2 is a detailed explanatory view of the electromagnetic wave supply section 3. The electromagnetic wave supply unit 3 is formed of copper in a cylindrical shape, and has a structure in which one end is open and the other is closed by a flat plate of copper (hereinafter referred to as a ground conductor substrate 5). Spiral conductor lines 6 are installed inside the ground conductor substrate 5 at regular intervals. The central portion of the spiral conductor line 6 is terminated to the ground conductor substrate 5 via the resistance load 7. Further, an electromagnetic wave in the microwave region is fed from the outside to the starting point of the spiral conductor line 6.
【0008】ここで、渦巻状導体線路6を接地導体基板
5に一定間隔で近接させる方法としては、例えば微小な
絶縁物製スペーサを渦巻状導体線路6と接地導体基板5
の間に設置する等の手段がある。Here, as a method of bringing the spiral conductor line 6 close to the ground conductor substrate 5 at a constant interval, for example, a minute insulator spacer is used to form the spiral conductor line 6 and the ground conductor substrate 5.
There is a means such as installing between.
【0009】図3により図2で記された電磁波供給部3
の動作を説明する。図3は接地導体基板5上の渦巻上導
体線路6の一部を示し、さらに渦巻状導体線路6と接地
導体基板5間を電磁波が伝搬するときの電磁波の様子を
表している。接地導体基板5と渦巻状導体線路6の間の
誘電率をε1とし、空気中の誘電率をε0とする。この
時、ε1≫ε0ならば渦巻状導体線路5に給電された電磁
波の電界は接地導体基板5と渦巻状導体線路6の間に集
中し、図3(a)に示すようになる。この様な状態では
電磁波はあまり空気中に放出されることなく、渦巻状導
体線路6に沿って接地導体基板5の間を伝搬していく。
次にε1=ε0の場合の電磁波の様子を図3(b)に示
す。この図から分かるように、ε1=ε0では電磁波の電
界が接地導体基板5と渦巻状導体線路6の間に集中する
ことができず、かなりの割合の電磁波を空間に放出す
る。つまり、電磁波の電送路としては非常に効率の悪い
状態を作り出すわけである。図3(b)の様な状態の接
地導体基板5と渦巻状導体線路6を構成を実現すれば、
渦巻状導体線路6を伝搬する電磁波は、渦巻状導体線路
6に沿って一定の割合で空間に放出される。よって、渦
巻状導体線路6を張り巡らせた接地導体基板5の平面方
向に比較的均一な電磁波を放射することが可能となる。The electromagnetic wave supply unit 3 shown in FIG. 2 according to FIG.
The operation of will be described. FIG. 3 shows a part of the spiral conductor line 6 on the ground conductor substrate 5, and shows a state of the electromagnetic wave when the electromagnetic wave propagates between the spiral conductor line 6 and the ground conductor substrate 5. Let ε 1 be the permittivity between the ground conductor substrate 5 and the spiral conductor line 6, and let ε 0 be the permittivity in air. At this time, if ε 1 >> ε 0 , the electric field of the electromagnetic wave fed to the spiral conductor line 5 is concentrated between the ground conductor substrate 5 and the spiral conductor line 6, and becomes as shown in FIG. In such a state, the electromagnetic wave is not so much released into the air and propagates along the spiral conductor line 6 between the ground conductor substrates 5.
Next, the state of the electromagnetic wave when ε 1 = ε 0 is shown in FIG. As can be seen from this figure, when ε 1 = ε 0 , the electric field of the electromagnetic wave cannot be concentrated between the ground conductor substrate 5 and the spiral conductor line 6, and a considerable proportion of the electromagnetic wave is emitted into the space. In other words, it creates a very inefficient state as an electromagnetic wave transmission path. If the ground conductor substrate 5 and the spiral conductor line 6 in the state as shown in FIG. 3B are realized,
The electromagnetic waves propagating in the spiral conductor line 6 are emitted into the space along the spiral conductor line 6 at a constant rate. Therefore, it is possible to radiate a relatively uniform electromagnetic wave in the plane direction of the ground conductor substrate 5 having the spiral conductor line 6 stretched around.
【0010】以上の原理を用いれば、使用する電磁波の
波長よりかなり広い面にも、渦巻状導体線路6を張り巡
らせる面積を大きくすることで比較的均一な電磁波を照
射することが可能となる。ただし、渦巻状導体線路6の
給電点から導入された電磁波は渦巻状導体線路の終端部
ではかなり減衰しているので渦巻状の外郭から電磁波を
供給した場合には中心部分での放射電磁波量が少なくな
る場合がある。よって、そのような場合には渦巻状中心
部分の巻数の密度を多くしてやる必要がある。By using the above principle, it is possible to irradiate a relatively uniform electromagnetic wave on a surface considerably wider than the wavelength of the electromagnetic wave to be used by enlarging the area over which the spiral conductor line 6 extends. However, since the electromagnetic wave introduced from the feeding point of the spiral conductor line 6 is considerably attenuated at the terminal end of the spiral conductor line, when the electromagnetic wave is supplied from the spiral outer shell, the amount of electromagnetic waves radiated in the central portion is increased. It may decrease. Therefore, in such a case, it is necessary to increase the density of the number of turns in the spiral center portion.
【0011】図2に示すように電磁波の給電点の他端で
ある終端部は抵抗負荷7により終端されている。この抵
抗負荷7の大きさは渦巻状導体線路6のインピーダンス
を考慮し、電磁波の放射効率または放射均一性が最適と
なるように設定する。その際、抵抗負荷7での電力消費
が大きくなった場合には抵抗負荷を水冷あるいは空冷に
より冷却する機構を付加する。また、抵抗負荷を付加す
る代わりに、終端部を開放し、容量結合によって、接地
導体基板に終端しても同等の効果がある。As shown in FIG. 2, the terminal end, which is the other end of the electromagnetic wave feeding point, is terminated by the resistive load 7. The size of the resistance load 7 is set in consideration of the impedance of the spiral conductor line 6 so that the radiation efficiency or radiation uniformity of electromagnetic waves is optimized. At that time, when the power consumption of the resistive load 7 becomes large, a mechanism for cooling the resistive load by water cooling or air cooling is added. Further, instead of adding a resistance load, the same effect can be obtained by terminating the end portion and opening the end portion to the ground conductor substrate by capacitive coupling.
【0012】このようにして広い面積にわたって均一な
プラズマを形成することが可能となる。半導体の製造工
程であるプラズマを応用したエッチングや膜体積装置に
本発明を適用することで、従来では困難であった大口径
試料の均一加工が可能となる。In this way, it is possible to form a uniform plasma over a wide area. By applying the present invention to the etching and the film volume apparatus that apply plasma, which is a semiconductor manufacturing process, it is possible to uniformly process a large-diameter sample, which has been difficult in the past.
【0013】図4および図5は図2で記された導体線路
を渦巻状とは異なる構造に配置した場合の説明図であ
る。まず、図4の場合は接地導体基板5に導体線路9を
矩形波状に配置した場合の説明図である。この図4の構
成においても渦巻状の配置と同様広い面積にわたって、
均一な電磁波の放射が可能となる。また図5の場合は導
体線路12を単一のループ状に配置した場合の説明図で
ある。図5の場合はループの中心部分とループを配置し
た部分で電磁波強度に強弱ができる可能性があるが、簡
単な構成で大面積に比較的均一な電磁波を供給できる点
に利点がある。FIGS. 4 and 5 are explanatory views when the conductor line shown in FIG. 2 is arranged in a structure different from the spiral shape. First, in the case of FIG. 4, it is an explanatory view in the case where the conductor lines 9 are arranged in a rectangular wave shape on the ground conductor substrate 5. Even in the configuration of FIG. 4, over a wide area like the spiral arrangement,
Radiation of uniform electromagnetic waves is possible. Further, FIG. 5 is an explanatory diagram in the case where the conductor lines 12 are arranged in a single loop shape. In the case of FIG. 5, there is a possibility that the intensity of the electromagnetic wave can be increased or decreased in the central portion of the loop and the portion where the loop is arranged, but there is an advantage in that a relatively uniform electromagnetic wave can be supplied to a large area with a simple configuration.
【0014】図6は本発明を半導体の製造装置以外に応
用した場合の実施例を示している。これは気体を封入し
た平面状の石英管15に本発明による電磁波供給源を用
い、石英管内部をプラズマ状態にする装置構成である。
図6に示す構成により、石英管内部に広い面積にわたり
均一なプラズマが形成される。これにより、石英管から
の発光を平面光源として利用することができる。FIG. 6 shows an embodiment in which the present invention is applied to a device other than a semiconductor manufacturing apparatus. This is a device configuration in which the electromagnetic wave supply source according to the present invention is used in a flat quartz tube 15 in which a gas is enclosed and the inside of the quartz tube is put into a plasma state.
With the configuration shown in FIG. 6, uniform plasma is formed inside the quartz tube over a wide area. Thereby, the light emitted from the quartz tube can be used as a flat light source.
【0015】[0015]
【発明の効果】本発明により、広い面積に均一に電磁波
を供給することが可能となった。これにより、電磁波と
磁場の相乗作用でプラズマを形成する装置で大面積に均
一なプラズマを形成することが可能となる。このプラズ
マ形成装置を半導体装置の加工に応用することにより、
大口径(例えば、直径8インチ以上)のシリコンウエハ
を全面にわたり均一に加工することができる。According to the present invention, it becomes possible to uniformly supply an electromagnetic wave to a wide area. As a result, it becomes possible to form a uniform plasma over a large area in an apparatus that forms plasma by the synergistic effect of electromagnetic waves and magnetic fields. By applying this plasma forming device to the processing of semiconductor devices,
A silicon wafer having a large diameter (for example, a diameter of 8 inches or more) can be uniformly processed over the entire surface.
【図1】本発明の基本構成の説明図。FIG. 1 is an explanatory diagram of a basic configuration of the present invention.
【図2】本発明の主たる部分の詳しい説明図。FIG. 2 is a detailed explanatory diagram of a main part of the present invention.
【図3】本発明の主たる部分の動作原理の説明図。FIG. 3 is an explanatory diagram of an operation principle of a main part of the present invention.
【図4】本発明の主たる部分の他の応用例の説明図。FIG. 4 is an explanatory diagram of another application example of the main part of the present invention.
【図5】本発明の主たる部分の他の応用例の説明図。FIG. 5 is an explanatory diagram of another application example of the main part of the present invention.
【図6】本発明の主たる部分を応用した他の実施例の説
明図。FIG. 6 is an explanatory diagram of another embodiment to which the main part of the present invention is applied.
5…接地導体基板、9…導体線路、10…電磁波の給電
点、11…終端部。5 ... Ground conductor board, 9 ... Conductor line, 10 ... Electromagnetic wave feeding point, 11 ... Termination part.
Claims (18)
ズマ状態にするプラズマ形成装置において、プラズマ形
成領域を構成する放電管を有し、前記放電管に前記マイ
クロ波領域の電磁波を照射する手段として、接地導体基
板と前記接地導体基板と容量結合した導体線路で構成し
たマイクロストリップ線路を用い、前記導体線路からの
漏洩電磁波を前記放電管に供給することを特徴とするプ
ラズマ形成装置。1. A plasma forming apparatus for bringing a gas into a plasma state by an electromagnetic wave in a microwave region, comprising a discharge tube constituting a plasma forming region, and irradiating the discharge tube with the electromagnetic wave in the microwave region, A plasma forming apparatus, characterized in that a microstrip line composed of a ground conductor substrate and a conductor line capacitively coupled to the ground conductor substrate is used to supply the electromagnetic wave leaking from the conductor line to the discharge tube.
に磁場を印加する手段を設けたプラズマ形成装置。2. The plasma forming apparatus according to claim 1, further comprising means for applying a magnetic field to the plasma forming region.
地導体基板の平面を均一に覆うように張り巡らされてい
るプラズマ形成装置。3. The plasma forming apparatus according to claim 1, wherein the conductor line is stretched around the ground conductor substrate so as to uniformly cover the plane thereof.
を前記接地導体基板平面を均一に覆うように渦巻状に張
り巡らせてなるプラズマ形成装置。4. The plasma forming apparatus according to claim 1 or 3, wherein the conductor line is spirally wound so as to uniformly cover the ground conductor substrate plane.
を前記接地導体基板平面を均一に覆うように方形波状に
張り巡らせてなるプラズマ形成装置。5. The plasma forming apparatus according to claim 1, wherein the conductor line is stretched in a square wave shape so as to uniformly cover the ground conductor substrate plane.
記導体線路の間が真空であるプラズマ形成装置。6. The plasma forming apparatus according to claim 1, wherein there is a vacuum between the ground conductor substrate and the conductor line.
記導体線路の間が空気であるプラズマ形成装置。7. The plasma forming apparatus according to claim 1, wherein air is present between the ground conductor substrate and the conductor line.
ら前記マイクロ波領域の電磁波を供給し、他端を抵抗負
荷により終端するプラズマ形成装置。8. The plasma forming apparatus according to claim 1, wherein the electromagnetic wave in the microwave region is supplied from one end of the conductor line and the other end is terminated by a resistance load.
ら前記マイクロ波領域の電磁波を供給し、他端を開放
し、終端するプラズマ形成装置。9. The plasma forming apparatus according to claim 1, wherein electromagnetic waves in the microwave region are supplied from one end of the conductor line, and the other end is opened and terminated.
よび前記導体線路を銅により形成するプラズマ形成装
置。10. The plasma forming apparatus according to claim 1, wherein the ground conductor substrate and the conductor line are made of copper.
前記導体線路の間隔を前記導体線路の全線路間において
一定に保つ手段を有してなるプラズマ形成装置。11. The plasma forming apparatus according to claim 1, further comprising means for keeping a distance between the ground conductor substrate and the conductor line constant between all lines of the conductor line.
と前記導体線路の間隔を前記導体線路の全線路間におい
て一定に保つ手段として、前記接地導体基板と前記導体
線路の間に一定間隔毎に微小な絶縁物製のスペーサを配
置してなるプラズマ形成装置。12. The means according to claim 11, wherein the ground conductor substrate and the conductor line are kept at a constant distance between all the conductor lines, and the ground conductor substrate and the conductor line are spaced at regular intervals. A plasma forming apparatus in which spacers made of minute insulators are arranged.
形状が、一端が閉じた円筒状であり、その閉じた平面上
に前記導体線路を配置し、前記円筒状の接地導体基板を
その開放部から前記放電管全体を包み込むように配置し
てなるプラズマ形成装置。13. The ground conductor substrate according to claim 1, wherein the ground conductor substrate has a cylindrical shape with one end closed, the conductor line is arranged on the closed plane, and the cylindrical ground conductor substrate is opened. Forming apparatus arranged so as to enclose the entire discharge tube from a part.
前記導体線路の間を比誘電率が1に近い物質で構成する
プラズマ形成装置。14. The plasma forming apparatus according to claim 1, wherein a material having a relative permittivity close to 1 is provided between the ground conductor substrate and the conductor line.
状に形成する場合、前記導体線路の終端部分の巻数密度
を給電側の巻数密度より多くするプラズマ形成装置。15. The plasma forming apparatus according to claim 4, wherein, when the conductor line is formed in a spiral shape, the winding number density at the terminal end of the conductor line is made higher than the winding number density on the power feeding side.
する手段を有するプラズマ形成装置。16. The plasma forming apparatus according to claim 8, further comprising means for cooling the resistive load.
のループ状にし、導体線路の一方から電磁波を供給し、
他端を抵抗負荷で終端する構造であるプラズマ形成装
置。17. The conductor line according to claim 1, wherein the conductor line has a single loop shape, and an electromagnetic wave is supplied from one of the conductor lines.
A plasma forming apparatus having a structure in which the other end is terminated by a resistive load.
入した石英管にマイクロ波領域の電磁波を照射する手段
により電磁波を照射し、石英管内をプラズマ状態にする
プラズマ形成装置。18. A plasma forming apparatus according to claim 3, wherein the quartz tube filled with gas is irradiated with electromagnetic waves by means for irradiating electromagnetic waves in the microwave region to bring the inside of the quartz tube into a plasma state.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4335784A JPH06188237A (en) | 1992-12-16 | 1992-12-16 | Apparatus for forming plasma |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP4335784A JPH06188237A (en) | 1992-12-16 | 1992-12-16 | Apparatus for forming plasma |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06188237A true JPH06188237A (en) | 1994-07-08 |
Family
ID=18292412
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP4335784A Pending JPH06188237A (en) | 1992-12-16 | 1992-12-16 | Apparatus for forming plasma |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06188237A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100289239B1 (en) * | 1997-03-27 | 2001-07-12 | 모리시타 요이찌 | Method and apparatus for plasma processing |
US6713968B2 (en) | 2000-09-06 | 2004-03-30 | Tokyo Electron Limited | Plasma processing apparatus |
US7395779B2 (en) | 2000-07-11 | 2008-07-08 | Tokyo Electron Limited | Plasma processing apparatus |
-
1992
- 1992-12-16 JP JP4335784A patent/JPH06188237A/en active Pending
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100289239B1 (en) * | 1997-03-27 | 2001-07-12 | 모리시타 요이찌 | Method and apparatus for plasma processing |
US7395779B2 (en) | 2000-07-11 | 2008-07-08 | Tokyo Electron Limited | Plasma processing apparatus |
US6713968B2 (en) | 2000-09-06 | 2004-03-30 | Tokyo Electron Limited | Plasma processing apparatus |
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