JPH02205020A - Microwave plasma treatment equipment - Google Patents
Microwave plasma treatment equipmentInfo
- Publication number
- JPH02205020A JPH02205020A JP2387689A JP2387689A JPH02205020A JP H02205020 A JPH02205020 A JP H02205020A JP 2387689 A JP2387689 A JP 2387689A JP 2387689 A JP2387689 A JP 2387689A JP H02205020 A JPH02205020 A JP H02205020A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- plasma
- ring
- shaped coils
- microwave
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 238000009832 plasma treatment Methods 0.000 title 1
- 230000005684 electric field Effects 0.000 claims description 2
- 239000000696 magnetic material Substances 0.000 claims 1
- 238000005530 etching Methods 0.000 description 26
- 239000000956 alloy Substances 0.000 description 8
- 229910045601 alloy Inorganic materials 0.000 description 8
- 238000001020 plasma etching Methods 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 150000002500 ions Chemical class 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 239000000463 material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 239000004065 semiconductor Substances 0.000 description 2
- 239000000758 substrate Substances 0.000 description 2
- ZAMOUSCENKQFHK-UHFFFAOYSA-N Chlorine atom Chemical compound [Cl] ZAMOUSCENKQFHK-UHFFFAOYSA-N 0.000 description 1
- 229910052801 chlorine Inorganic materials 0.000 description 1
- 239000000460 chlorine Substances 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 238000005268 plasma chemical vapour deposition Methods 0.000 description 1
- 150000003254 radicals Chemical class 0.000 description 1
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
本発明は、マイクロ波プラズマ処理装置に係り、特に有
磁界型のマイクロ波プラズマ処理装置に関するものであ
る。DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a microwave plasma processing apparatus, and particularly to a magnetic field type microwave plasma processing apparatus.
従来のマイクロ波プラズマ処理装547として半導体素
子基板等の試料をエツチング処理する装置を第4図によ
り説明する。An apparatus for etching a sample such as a semiconductor element substrate as a conventional microwave plasma processing apparatus 547 will be explained with reference to FIG.
第4図で真空排気装置10が連結され、上方に開放端を
有する真空容器加には、一方に開放端を有する放電管I
がこの場合上下方向に気密に構成されている。放電管(
資)の外側には、放電管間を含み導波管旬が配設され、
等波管荀の外側には磁界発生手段、例えば檄状コイル恥
が^さ方向に2段猿装されている。また環状コイルの外
周には磁界シールド板6が配置される。In FIG. 4, a vacuum evacuation device 10 is connected to a vacuum vessel having an open end on the upper side, and a discharge tube I having an open end on one side.
In this case, the structure is airtight in the vertical direction. Discharge tube (
A waveguide tube is installed on the outside of the tube, including between the discharge tubes.
On the outside of the equal-wave tube, magnetic field generating means, for example, a coil-shaped coil, is installed in two stages in the horizontal direction. Further, a magnetic field shield plate 6 is arranged around the outer periphery of the annular coil.
導波貴信はマイクロ波導波管印を介してマイクロ波発生
手段70に連結されている。The waveguide is connected to the microwave generation means 70 via a microwave waveguide.
真空容器囚には放電ガス導入用のノズル21が設けられ
、ノズル4にはガス導管(資)を介して放電ガス供給装
!匍に連結されている。真空容器(9)と放電管加とで
形成された空間100には試料電極110が設けられて
いる。試料電極110には高周波電源120が接続され
、一方アースされた真空容器加にはアース電極130が
設けられている。A nozzle 21 for introducing discharge gas is provided in the vacuum container, and a discharge gas supply device is connected to the nozzle 4 via a gas conduit. It is connected to the sword. A sample electrode 110 is provided in a space 100 formed by the vacuum container (9) and the discharge tube. A high frequency power source 120 is connected to the sample electrode 110, and a ground electrode 130 is provided on the grounded vacuum vessel.
試料電極110には試料140が絶縁材製の試料押え1
50により圧着保持され、空間100は真空排気装[1
0により所定圧力まで減圧排気される。その後空間10
0には放電ガス供給装置f9fJよりガス導管(資)、
ノズル21を経て放電ガスが所定温飯で導入されるとと
もに空間100の圧力は真空排気装置10により所定の
処理圧力に適切に調節される。A sample 140 is attached to the sample electrode 110 using a sample holder 1 made of an insulating material.
50, and the space 100 is equipped with a vacuum exhaust system [1
0, the pressure is reduced to a predetermined pressure. then space 10
0 is a gas conduit (material) from the discharge gas supply device f9fJ,
The discharge gas is introduced at a predetermined temperature through the nozzle 21, and the pressure in the space 100 is appropriately adjusted to a predetermined processing pressure by the evacuation device 10.
一方、空間100にはマイクロ波発生装置70で発生し
たマイクロ波による電界と環状コイル関による磁界とが
印加され放電管(資)内の放電領域に存在する放電ガス
がプラズマ化されるとともに、試料電極110には高周
波電源120より高周波電力が印加され、これにより高
周波バイアスが発生する。On the other hand, an electric field due to microwaves generated by the microwave generator 70 and a magnetic field generated by the ring-shaped coil are applied to the space 100, and the discharge gas present in the discharge area in the discharge tube is turned into plasma, and the sample High frequency power is applied to the electrode 110 from a high frequency power supply 120, thereby generating a high frequency bias.
試料140は高周波電力を適切に調整することによリイ
オンエネルギが制御され高精度にエツチング処理される
。The sample 140 is etched with high precision by controlling the ion energy by appropriately adjusting the high frequency power.
上記マイクロ波プラズマエツチング装置を用いて塩素系
ガスによるM合金膜のエツチング処理を行い、その後の
M残膜を除去する目的でいわゆるオーバーエツチングを
行う際の下地膜、例えば、8i02膜のエツチング結果
の一例を第5因に示す。The M alloy film is etched using a chlorine-based gas using the microwave plasma etching apparatus described above, and the underlying film, for example, the 8i02 film, is etched when performing so-called over-etching for the purpose of removing the remaining M film. An example is shown in the fifth factor.
第5図中の数値は1分間当りの5i02膜のエツチング
速度を示した数値であるが平均エツチング速度8211
17m1n、エブチング均一性±12%程度が得られて
いるが、エツチング速度にかなりばらつきが生じている
。またエツチング速度の低い部分にはM合金膜エツチン
グ時のエツチング残渣の発生が多く見られた。エツチン
グ残漬や下地膜エブチングの不均一はLSI素子の電気
等性のばらつきや不良の要因となり、素子製造上の問題
点となっていた。The values in Figure 5 indicate the etching rate of the 5i02 film per minute, and the average etching rate is 8211.
Although an etching uniformity of approximately ±12% was obtained, there was considerable variation in the etching speed. Furthermore, in areas where the etching rate was low, a large amount of etching residue was observed during etching of the M alloy film. Etching residue and non-uniform etching of the underlying film cause variations in electrical properties and defects in LSI devices, which pose problems in device manufacturing.
なお、この種の装置として関連するものには、例えば、
特開昭60−103618号、特開昭60−15462
0号、特開昭60−158629号等が挙げられる。Note that related devices of this type include, for example,
JP-A-60-103618, JP-A-60-15462
No. 0, JP-A-60-158629, and the like.
上記従来技術では、磁界シールド板を改良して高磁界を
達成しプラズマをさら1こ高密度、均一化することにつ
いて配慮されておらず、このため、試料を高速、均一性
良くプラズマ処理する上で問題を有している。In the above conventional technology, no consideration is given to improving the magnetic field shield plate to achieve a high magnetic field and making the plasma even more dense and uniform. I have a problem with this.
久′
本発明の目的は、試料を高速、均−性良畷プ六マ処理で
きるマイクロ波プラズマ処理装置を提供することにある
。An object of the present invention is to provide a microwave plasma processing apparatus capable of processing a sample at high speed and with good uniformity.
上記目的は、高密度で均一なプラズマは二つの環状コイ
ル外部の上、下面に磁界シールド板を配設しプラズマ発
生領域に作用する磁界強度を高めるとともに、磁界を発
生するためのコイル電流値を適正化する手段を具備した
ものとすることにより達成される。The above purpose is to create a high-density, uniform plasma by installing magnetic field shield plates on the top and bottom surfaces of the two annular coils to increase the magnetic field strength that acts on the plasma generation area, and to increase the coil current value for generating the magnetic field. This can be achieved by providing a means for making it appropriate.
本発明は高密度で均一なプラズマを得るために二組の環
状コイル外部の上、下面に磁界シールド板を適切に配置
し、かつ環状コイル電流値を適切に制御することにより
達成される。The present invention is achieved by appropriately arranging magnetic field shield plates on the upper and lower surfaces of the outside of two sets of annular coils and appropriately controlling the annular coil current value in order to obtain high-density and uniform plasma.
高密度プラズマは従来、コイルの上下面から発散してい
た磁界を磁界シールド板を挿入し磁力線の通過面積をほ
ぼマイクロ波導波管径および放電管径と同程度とし磁束
密度を増加して、★動的にプラズマ発生領域に作用する
磁界強度を高めることによって達成される。High-density plasma is created by inserting a magnetic field shield plate to replace the magnetic field that was conventionally emitted from the top and bottom surfaces of the coil, making the area through which the lines of magnetic force pass approximately the same as the diameter of the microwave waveguide and discharge tube, increasing the magnetic flux density. This is achieved by dynamically increasing the magnetic field strength acting on the plasma generation region.
一方、均一なプラズマは二つの環状コイルの電流値を適
切に設定することにより達成される。On the other hand, uniform plasma can be achieved by appropriately setting the current values of the two annular coils.
本発明の一実施例を第1図、@2図および第3図により
説明する。なお、本実施例のようなマイクロ波プラズマ
エツチング装置における半導体素子基板等の試料の処理
操作は従来技術と同様であるため説明を省略する。また
第1図の装置構成で第4図に示した従来装置と同一部材
は同一符号で示し、説明を省略する。An embodiment of the present invention will be explained with reference to FIGS. 1, 2, and 3. It should be noted that the processing operations for samples such as semiconductor element substrates in the microwave plasma etching apparatus of this embodiment are the same as those in the prior art, and therefore the explanation thereof will be omitted. Further, the same members in the apparatus configuration of FIG. 1 as those of the conventional apparatus shown in FIG. 4 are designated by the same reference numerals, and the explanation thereof will be omitted.
第1図で環状フィルにより発生する磁界の外部への発散
を防止するため磁場シールド板46.47を二つの環状
コイル(資)の上、下面に挿入する。磁界シールド板4
6.47の開口径をほぼマイクロ波導波管ωおよび放電
管加の開口径と同程度とすることにより環状コイル上面
、下面での磁力線通過面積を従来より小さくでき、実効
的にプラズマ発生領域に作用するコイル中心軸上の磁界
強度を増加することができる。In FIG. 1, magnetic field shield plates 46 and 47 are inserted on the upper and lower surfaces of the two annular coils to prevent the magnetic field generated by the annular fill from dispersing to the outside. Magnetic field shield plate 4
By making the aperture diameter of 6.47 approximately the same as the aperture diameter of the microwave waveguide ω and the discharge tube, the area through which the lines of magnetic force pass on the top and bottom surfaces of the annular coil can be made smaller than before, effectively allowing the plasma generation region to The magnetic field strength on the acting coil central axis can be increased.
第2図に環状コイル父の電流値を上コイル25A。Figure 2 shows the current value of the circular coil father at the upper coil 25A.
下コイル15Aとしたときのコイル中心軸上の垂直方向
の磁界強度分布aを従来例での分布すとともに示す。本
発明によればプラズマ発生域に従来に比較して高い磁界
強度が得られるため従来よりさらに高密度プラズマを得
ることができる。一方、プラズマの均一性は二つの環状
コイルの電流値を適切に設定することによりて得られる
。The magnetic field strength distribution a in the vertical direction on the coil center axis when the lower coil 15A is used is shown together with the distribution in the conventional example. According to the present invention, since a higher magnetic field strength can be obtained in the plasma generation region than in the past, higher density plasma can be obtained than in the past. On the other hand, plasma uniformity can be obtained by appropriately setting the current values of the two annular coils.
第3図に′!J1図で示した構成の装置を用いてM合金
膜のエツチング処理を行い、その後M残膜を除去する目
的でMのオーバエツチングを行う際の下地5i02膜の
エツチング速度分布を示す。結果として平均エツチング
速度901ul/mln 、エツチング均一性±6−程
度が得られ、従来より下地膜のエツチング均一性がはる
かに向上した。In Figure 3'! The etching rate distribution of the underlying 5i02 film is shown when the M alloy film is etched using the apparatus configured as shown in Figure J1, and then M overetching is performed for the purpose of removing the remaining M film. As a result, an average etching rate of 901 ul/mln and an etching uniformity of about ±6 were obtained, and the etching uniformity of the base film was much improved compared to the conventional method.
また高密度で均一なプラズマを形成することでプラズマ
中のイオン量が増加し、従来たびたび発生し、問題とな
っていたM合金膜中のCu成分に起因するエツチング残
渣も素子の電気特性上問題ないレベルまで十分に低減す
ることができた。In addition, by forming a high-density and uniform plasma, the amount of ions in the plasma increases, and the etching residue caused by the Cu component in the M alloy film, which has often occurred and caused problems in the past, is a problem in terms of the electrical characteristics of the device. We were able to sufficiently reduce this to a level of zero.
なお、下地膜のエツチング速度が増加するため、M合金
膜とのエツチング速度比、いわゆる選択比(1’−1t
/ 8 i 02 )の低下が懸念されるが、プラズマ
密度の増加にともなってラジカル種も増大しM合金膜の
エツチング速度も増加したため、従来と同等な値が得ら
れた。Note that since the etching rate of the underlying film increases, the etching rate ratio with respect to the M alloy film, the so-called selectivity (1'-1t
/8 i 02 ), but as the plasma density increased, the number of radical species increased and the etching rate of the M alloy film also increased, so a value equivalent to the conventional value was obtained.
本実施例によればM合金膜を残漬な畷均−にエツチング
できるのでLSI素子の電気特性の安定した製品ができ
、製品収率の高いエツチング装置が得られる。According to this embodiment, since the M alloy film can be etched evenly with no residue, a product with stable electrical characteristics of an LSI element can be obtained, and an etching apparatus with a high product yield can be obtained.
なお、本実施例ではM合金膜のエツチングに適用した場
合を示したが、被エツチング材やエツチング条件を変更
することにより種々のエツチングに適用できることは言
うまでもない。Although this embodiment shows the case where the present invention is applied to etching an M alloy film, it goes without saying that the present invention can be applied to various types of etching by changing the material to be etched and the etching conditions.
また、例えば、試料をプラズマCVD処理等成膜処理す
る場合においても、その処理装置が、有磁界型のマイク
ロ波プラズマ処理装置であれば、有効に適用できる。Further, for example, even when a sample is subjected to a film forming process such as a plasma CVD process, the present invention can be effectively applied if the processing apparatus is a magnetic field type microwave plasma processing apparatus.
本発明によれば高密度で均一なプラズマが得られるので
、試料を高速、均一性良くプラズマ処理できる効果があ
る。According to the present invention, since high-density and uniform plasma can be obtained, there is an effect that a sample can be plasma-treated at high speed and with good uniformity.
第1図は本発明の一実施例を示すマイクロ波プラズマエ
ツチング!IIの縦断面図、582図は第1図に示す装
置を用いた場合と従来例との効果の比較を示す磁界分布
図、第3図は9161図に示す装置を用いた8i02膜
のエツチング速度分布図、@4図は従来例を示すマイク
ロ波プラズマエブチング装置の縦断面図、第5図は従来
装置を用いて8i02換をエツチングした場合のエツチ
ング速度分布図である。Figure 1 shows an example of microwave plasma etching according to the present invention! 582 is a magnetic field distribution diagram showing a comparison of the effect when using the apparatus shown in Fig. 1 and the conventional example, and Fig. 3 is the etching rate of 8i02 film using the apparatus shown in Fig. 9161. Distribution diagram, Figure @4 is a vertical cross-sectional view of a conventional microwave plasma etching apparatus, and FIG. 5 is an etching rate distribution diagram when etching 8i02 using the conventional apparatus.
Claims (1)
れ、かつ外部磁界が印加される放電領域内に放電ガスを
導入してマイクロ波放電をおこし、発出するプラズマを
用いて試料表面の処理を行う装置において、前記外部磁
界を発生する手段に磁性体による磁界シールド板を設け
ることを特徴とするマイクロ波プラズマ処理装置。 2、前記外部磁界発生用手段に磁界シールド板を設け、
該磁界シールド板の開口面積を上部磁界シールド板より
下部磁界シールド板の方を大きくした第1請求項に記載
のマイクロ波プラズマ処理装置。 3、前記上部磁界シールド板の開口径をマイクロ波導波
管径と略等しく、前記下部磁場シールド板の開口径を放
電管径と略等しくした第2請求項に記載のマイクロ波プ
ラズマ処理装置。[Claims] 1. A microwave electric field is applied by a microwave generator, and a discharge gas is introduced into a discharge region to which an external magnetic field is applied to generate a microwave discharge, and the emitted plasma is used to generate a sample. A microwave plasma processing apparatus for surface processing, characterized in that the means for generating the external magnetic field is provided with a magnetic field shield plate made of a magnetic material. 2. Providing a magnetic field shield plate on the external magnetic field generating means,
The microwave plasma processing apparatus according to claim 1, wherein the opening area of the lower magnetic field shielding plate is larger than that of the upper magnetic field shielding plate. 3. The microwave plasma processing apparatus according to claim 2, wherein the opening diameter of the upper magnetic field shield plate is approximately equal to the microwave waveguide diameter, and the opening diameter of the lower magnetic field shield plate is approximately equal to the discharge tube diameter.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1023876A JP2776866B2 (en) | 1989-02-03 | 1989-02-03 | Microwave plasma processing equipment |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1023876A JP2776866B2 (en) | 1989-02-03 | 1989-02-03 | Microwave plasma processing equipment |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH02205020A true JPH02205020A (en) | 1990-08-14 |
JP2776866B2 JP2776866B2 (en) | 1998-07-16 |
Family
ID=12122652
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1023876A Expired - Fee Related JP2776866B2 (en) | 1989-02-03 | 1989-02-03 | Microwave plasma processing equipment |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2776866B2 (en) |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63219128A (en) * | 1987-03-06 | 1988-09-12 | Matsushita Electric Ind Co Ltd | Treatment apparatus |
JPS63273320A (en) * | 1987-05-01 | 1988-11-10 | Mitsubishi Electric Corp | Plasma treatment apparatus |
JPH0282030U (en) * | 1988-12-15 | 1990-06-25 |
-
1989
- 1989-02-03 JP JP1023876A patent/JP2776866B2/en not_active Expired - Fee Related
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS63219128A (en) * | 1987-03-06 | 1988-09-12 | Matsushita Electric Ind Co Ltd | Treatment apparatus |
JPS63273320A (en) * | 1987-05-01 | 1988-11-10 | Mitsubishi Electric Corp | Plasma treatment apparatus |
JPH0282030U (en) * | 1988-12-15 | 1990-06-25 |
Also Published As
Publication number | Publication date |
---|---|
JP2776866B2 (en) | 1998-07-16 |
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