JPH0456774A - Plasma reactor - Google Patents
Plasma reactorInfo
- Publication number
- JPH0456774A JPH0456774A JP17080790A JP17080790A JPH0456774A JP H0456774 A JPH0456774 A JP H0456774A JP 17080790 A JP17080790 A JP 17080790A JP 17080790 A JP17080790 A JP 17080790A JP H0456774 A JPH0456774 A JP H0456774A
- Authority
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- Prior art keywords
- plasma
- magnetic field
- electrodes
- reaction vessel
- wafer
- 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.)
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- ing And Chemical Polishing (AREA)
- Drying Of Semiconductors (AREA)
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〕
この発明は、ガス放電によりプラズマを発生させ、発生
させたプラズマを利用して半導体基板表面のエツチング
や薄膜形成等の処理を行うプラズマ反応装置に関する。[Detailed Description of the Invention] [Field of Industrial Application] The present invention relates to a plasma reaction device that generates plasma by gas discharge and uses the generated plasma to perform processing such as etching or forming a thin film on the surface of a semiconductor substrate. Regarding.
ICなどの半導体装置の製造においては、半導体基板(
ウェハ)に薄膜形成、エツチング等の処理が行われるが
、このような半導体基板処理装置の一つとして、ガス放
電によるプラズマを利用したプラズマ反応装置がある。In the manufacture of semiconductor devices such as ICs, semiconductor substrates (
Processes such as thin film formation and etching are performed on wafers, and one type of semiconductor substrate processing apparatus is a plasma reaction apparatus that utilizes plasma generated by gas discharge.
第5図はRIE(反応性イオンエツチング)等に用いら
れる従来のプラズマ反応装置の概略を示す断面図であり
、以下に説明する。FIG. 5 is a sectional view schematically showing a conventional plasma reaction apparatus used for RIE (reactive ion etching), etc., and will be described below.
第5図に示すように、例えば中空円柱状の反応容器1内
の底面に絶縁体2を介して一方の平板電極であるカソー
ド電極3が固定されると共に、反応容器1内の天面に、
接地された他方の平板電極であるアノード電極4が固定
され、画電極3.4が反応容器1内に対向して設けられ
、カソード電極3にウェハ5が装着、保持されている。As shown in FIG. 5, for example, a cathode electrode 3, which is one flat plate electrode, is fixed to the bottom surface of a hollow cylindrical reaction container 1 via an insulator 2, and a cathode electrode 3, which is one of the flat electrodes, is fixed to the bottom surface of the reaction container 1, which has a hollow cylindrical shape, for example.
An anode electrode 4, which is the other grounded flat plate electrode, is fixed, a picture electrode 3.4 is provided facing inside the reaction vessel 1, and a wafer 5 is mounted and held on the cathode electrode 3.
このとき、アノード電極4に複数のガス吹出口6a及び
ガス流路6bが形成され、反応容器1の天面に形成され
たガス導入ロアにガス流路か連通し、ガス導入ロア、ガ
ス流路6b及び各ガス吹出口6aを介して、反応容器1
内にガスが導入され、反応容器1の底面に形成された排
気口8からガスが排気される。At this time, a plurality of gas outlets 6a and gas channels 6b are formed in the anode electrode 4, and the gas channels communicate with a gas introduction lower formed on the top surface of the reaction vessel 1. 6b and each gas outlet 6a, the reaction vessel 1
Gas is introduced into the reaction vessel 1 and exhausted from an exhaust port 8 formed at the bottom of the reaction vessel 1 .
また、高周波電源9の一端がインピーダンス整合器10
を介してカソード電極3に接続されると共に、他端が接
地され、両電極3.4間に高周波電界が形成される。Further, one end of the high frequency power supply 9 is connected to an impedance matching device 10.
It is connected to the cathode electrode 3 via the electrode 3.4, and the other end is grounded, so that a high frequency electric field is formed between the two electrodes 3.4.
さらに、反応容器1の外側には1組のミラー磁場発生用
コイルlla、llbが対向位置に配設されると共に、
ミラー磁場を回転させるために、複数組のミラー磁場発
生用コイルが、反応容器1の中心軸を基準として一定角
度ごとに配設され、一定周期で各組のミラー磁場発生用
コイルに順次に切換通電することにより、一定の方向に
ミラー磁場を回転し、プラズマの偏在を防止している。Furthermore, a pair of mirror magnetic field generating coils lla and llb are disposed at opposing positions on the outside of the reaction vessel 1, and
In order to rotate the mirror magnetic field, multiple sets of mirror magnetic field generating coils are arranged at fixed angles with respect to the central axis of the reaction vessel 1, and each set of mirror magnetic field generating coils is sequentially switched at a fixed period. By applying electricity, the mirror magnetic field is rotated in a fixed direction to prevent uneven distribution of plasma.
そして、このような構成の装置によりウェハ5に薄膜形
成やエツチングを行う場合、排気口8より反応容器1内
の不要ガスか十分に排気されたのち、ガス導入ロア、ガ
ス流路6b及び各ガス吹出口6aを介して反応容器1内
に反応性ガスを導入しつつ、その一部が排気口8より排
気され、反応容器1の内部の圧力が所定の値に保たれる
。When forming a thin film or etching on the wafer 5 using an apparatus having such a configuration, the unnecessary gas in the reaction vessel 1 is sufficiently exhausted through the exhaust port 8, and then the gas introduction lower, the gas flow path 6b, and each gas are removed. While the reactive gas is introduced into the reaction vessel 1 through the blow-off port 6a, a portion of the reactive gas is exhausted through the exhaust port 8, and the pressure inside the reaction vessel 1 is maintained at a predetermined value.
つぎに、電源9により13.56MHzの高周波電力が
カソード電極3に与えられると共に、コイルlla、l
lbに通電されてミラー磁場か発生され、反応容器1内
において、両電極3.4間の高周波電界と、これに直交
する磁力線を持つミラー磁場とによるマグネトロン放電
が開始され、高密度のガスプラズマか発生され、この高
密度ガスプラズマの反応によって、ウェハ5の表面に薄
膜形成やエツチング等が行われる。Next, a high frequency power of 13.56 MHz is applied to the cathode electrode 3 by the power source 9, and the coils lla and l
lb is energized to generate a mirror magnetic field, and magnetron discharge is started in the reaction vessel 1 due to the high-frequency electric field between both electrodes 3.4 and the mirror magnetic field having lines of magnetic force perpendicular to this, and a high-density gas plasma is generated. By the reaction of this high-density gas plasma, thin film formation, etching, etc. are performed on the surface of the wafer 5.
ここで用いられる反応性ガスの種類、圧力や高周波電源
8による電力等は、ウエノ\の処理工程の種類に応じて
適宜選択される。The type of reactive gas used here, the pressure, the electric power from the high frequency power source 8, etc. are appropriately selected depending on the type of Ueno treatment process.
ところで、このようなプラズマ反応装置の場合、前述し
たように、複数組(2〜3組)のミラー磁場発生用コイ
ルによってミラー磁場を回転することによって、ExB
(Eは電界、Bは磁場)ドリフトによるプラズマの偏
在を防止し、プラズマ密度の均一化を図っているが、こ
の場合、プラズマ密度は時間的に均一化されるものの、
任意の時刻におけるプラズマ密度は不均一になり、プラ
ズマ中のウェハ5の電位及びウェハ5の表面電位の分布
は、例えば第6図に示すようになる。By the way, in the case of such a plasma reactor, as mentioned above, by rotating the mirror magnetic field using multiple sets (2 to 3 sets) of mirror magnetic field generating coils, ExB
(E is electric field, B is magnetic field) In order to prevent uneven distribution of plasma due to drift and make the plasma density uniform, in this case, although the plasma density is made uniform over time,
The plasma density at any given time becomes non-uniform, and the potential of the wafer 5 in the plasma and the distribution of the surface potential of the wafer 5 become as shown in FIG. 6, for example.
たたし、第6図中の横軸は、ウェハ5の中心点を基準と
したときの距離であり、縦軸は電位■の絶対値であり、
1点鎖線はウェハ5の電位、実線はウェハ5の表面の局
所電位をそれぞれ表わし、X印は測定点を示す。However, the horizontal axis in FIG. 6 is the distance with respect to the center point of the wafer 5, and the vertical axis is the absolute value of the potential ■.
The one-dot chain line represents the potential of the wafer 5, the solid line represents the local potential on the surface of the wafer 5, and the X marks represent measurement points.
従来の場合、第6図に示すように任意の時刻におけるウ
ェハ5の電位及びウェハ5の表面の局所電位に差が生じ
、ウェハ5の中心から離れるに従って電位の差は大きく
なっており、ウェハ5の表面に形成されている半導体デ
バイスに電界が加わり、特に薄い絶縁膜の場合には破損
し、形成デバイスの損傷を招くという問題点があった。In the conventional case, as shown in FIG. 6, a difference occurs between the potential of the wafer 5 at any given time and the local potential of the surface of the wafer 5, and the difference in potential increases as the distance from the center of the wafer 5 increases. There is a problem in that an electric field is applied to a semiconductor device formed on the surface of the insulating film, causing damage to the formed device, especially in the case of a thin insulating film.
この発明は、上記のような問題点を解消するためになさ
れたもので、マグネトロン放電による高密度プラズマを
維持し、かつ均一性に優れ、形成デバイスに与える損傷
の少ないプラズマ反応装置が得られるようにすることを
目的とする。This invention was made in order to solve the above-mentioned problems, and it is possible to obtain a plasma reactor that maintains high-density plasma by magnetron discharge, has excellent uniformity, and causes less damage to forming devices. The purpose is to
この発明に係るプラズマ反応装置は、反応容器内に2個
の平板電極が平行に対向して設けられ、前記両電極間で
導入ガスの放電によるプラズマを発生するプラズマ反応
装置において、前記容器内の磁束密度が前記両電極間に
おいて極小となる極小磁場を発生する磁場発生手段を設
けたことを特徴としている。A plasma reactor according to the present invention is a plasma reactor in which two flat plate electrodes are provided in a reaction vessel in parallel and facing each other, and plasma is generated by discharge of an introduced gas between the two electrodes. The present invention is characterized in that a magnetic field generating means is provided for generating a minimal magnetic field in which the magnetic flux density becomes minimal between the two electrodes.
この発明においては、磁場発生手段により両電極間にお
いて磁束密度が極小となる極小磁場を発生したため、反
応容器の内壁近傍では磁束密度が大きくなり、両電極間
で発生したプラズマの反応容器の内壁方向への拡散が抑
制され、両電極間に高密度のプラズマが安定に保持され
、しかも両電極間のプラズマの密度がほぼ均一で軸対称
になり、従来のようにウェハとウニ八表面との電位に差
が生じることがなく、ウェハに形成されるデバイスが損
傷を受けることが防止される。In this invention, since the magnetic field generation means generates a minimal magnetic field in which the magnetic flux density is minimal between the two electrodes, the magnetic flux density increases near the inner wall of the reaction vessel, and the plasma generated between the two electrodes is directed toward the inner wall of the reaction vessel. This suppresses the diffusion of high-density plasma between the two electrodes, and the density of the plasma between the two electrodes becomes almost uniform and axially symmetrical. This prevents damage to the devices formed on the wafer.
第1図はこの発明のプラズマ反応装置の−実施例の概略
図である。FIG. 1 is a schematic diagram of an embodiment of the plasma reactor of the present invention.
第1図において、第5図と相違するのは、ミラー磁場発
生用コイルlla、llbに代え、反応容器1内に極小
磁場を発生する磁場発生手段としての多重カスプ磁場発
生用コイル12を、反応容器1の外側に設けたことであ
る。1 is different from FIG. 5 in that, instead of the mirror magnetic field generating coils lla and llb, a multiple cusp magnetic field generating coil 12 is used as a magnetic field generating means for generating a minimal magnetic field in the reaction vessel 1. This is because it is provided on the outside of the container 1.
このとき、多重カスプ磁場発生用コイル12は、中空円
柱状の反応容器1の母船に平行な8個の電流路を備えて
おり、これらの電流路が反応容器1の中心軸を基準とし
て一定角度ごとに配置されている。At this time, the multiple cusp magnetic field generation coil 12 is equipped with eight current paths parallel to the mother vessel of the hollow cylindrical reaction vessel 1, and these current paths are arranged at a constant angle with respect to the central axis of the reaction vessel 1. are arranged for each.
また、第1図には示されていないが、反応容器1内には
第5図に示す両電極3.4が配設されている。Although not shown in FIG. 1, both electrodes 3.4 shown in FIG. 5 are disposed within the reaction vessel 1. As shown in FIG.
ところで、第3図は第1図中のx−x’線における断面
の概略図であり、コイル12に第1図中の矢印方向に電
流を通流することによって、反応容器1内に第3図中の
矢印に示すような磁力線が発生し、反応容器1のほぼ中
心において磁束密度が極小となる極小磁場が形成される
。By the way, FIG. 3 is a schematic cross-sectional view taken along the line xx' in FIG. 1, and by passing a current through the coil 12 in the direction of the arrow in FIG. Lines of magnetic force as shown by the arrows in the figure are generated, and a minimal magnetic field is formed in which the magnetic flux density is minimal at approximately the center of the reaction vessel 1.
このような極小磁場により、反応容器1内で発生したプ
ラズマは、第3図中の磁力線で囲まれた内側部分に閉じ
込められ、磁力線によって反応容器1の内壁方向へのプ
ラズマ拡散が抑制されるため、磁力線で囲まれた内側部
分におけるプラズマは高密度でかつ均一になる。Due to such a minimal magnetic field, the plasma generated in the reaction vessel 1 is confined in the inner part surrounded by the magnetic lines of force in Fig. 3, and the plasma diffusion toward the inner wall of the reaction vessel 1 is suppressed by the magnetic lines of force. , the plasma in the inner part surrounded by magnetic field lines becomes dense and uniform.
従って、反応容器1の中央の磁束密度はほぼゼロとなり
、画電極3,4間のプラズマ発生領域における磁束密度
が極小で、反応容器1の内壁に近づくに連れて磁束密度
が大きくなるため、両電極間3.4で発生したプラズマ
の反応容器1の内壁方向への拡散を抑制することができ
、両電極3゜4間に高密度のプラズマを安定に保持する
ことができる。Therefore, the magnetic flux density at the center of the reaction vessel 1 is almost zero, the magnetic flux density in the plasma generation region between the picture electrodes 3 and 4 is minimal, and the magnetic flux density increases as it approaches the inner wall of the reaction vessel 1. Diffusion of plasma generated between the electrodes 3.4 toward the inner wall of the reaction vessel 1 can be suppressed, and high-density plasma can be stably maintained between the electrodes 3.4.
さらに、両電極3.4間のプラズマの密度がほぼ均一で
軸対称になるため、第4図に示すように、カソード電極
3に固定されたウェハ5の電位とウェハ5の表面の電位
はほぼ等しくなり、従来のようにウェハ5の電位とウェ
ハ5の表面の局所電位に差が生じることがなく、ウェハ
5に形成されるデバイスの損傷を防止することができ、
検証によっても薄い絶縁膜の絶縁耐圧不良は全く検出さ
れなかった。Furthermore, since the plasma density between the two electrodes 3.4 is almost uniform and axially symmetrical, the potential of the wafer 5 fixed to the cathode electrode 3 and the potential of the surface of the wafer 5 are approximately equal, as shown in FIG. Therefore, there is no difference between the potential of the wafer 5 and the local potential of the surface of the wafer 5 as in the conventional case, and damage to the devices formed on the wafer 5 can be prevented.
Even through verification, no breakdown voltage failure of the thin insulating film was detected.
ただし、第6図と同様に、第4図中の横軸はウェハ5の
中心点を基準としたときの距離であり、縦軸は電位Vの
絶対値であり、1点鎖線はウェハ5の電位であり、X印
はウェハ5の表面の電位測定点における電位である。However, similar to FIG. 6, the horizontal axis in FIG. The X mark is the potential at the potential measurement point on the surface of the wafer 5.
なお、上記実施例では、極小磁場を発生する磁場発生手
段として、多重カスプ磁場発生用コイル12を用いたが
、特にこれに限定されるものではなく、例えばベースボ
ールコイルや2個のベースボールコイルを90″ずらし
て対向した引用コイルなどを用いてもよいのは言うまで
もない。In the above embodiment, the multiple cusp magnetic field generating coil 12 was used as the magnetic field generating means for generating the minimum magnetic field, but the invention is not limited to this, and for example, a baseball coil or two baseball coils may be used. Needless to say, it is also possible to use opposing coils that are shifted by 90''.
以上のように、この発明のプラズマ反応装置によれば、
この発明においては、磁場発生手段により両電極間にお
いて磁束密度が極小となる極小磁場を発生したため、両
電極間で発生したプラズマの反応容器の内壁方向への拡
散を抑制することができ、両電極間に高密度のプラズマ
を安定に保持でき、しかも両電極間のプラズマの密度が
ほぼ均一で軸対称になり、従来のようにウェハとウェハ
表面との電位に差を生じることがなく、ウェハに形成さ
れるデバイスの損傷を防止することができ、ガス放電に
よるプラズマを利用したエツチングや薄膜形成において
極めて有利である。As described above, according to the plasma reactor of the present invention,
In this invention, since the magnetic field generating means generates a minimal magnetic field in which the magnetic flux density is minimal between the two electrodes, it is possible to suppress the diffusion of the plasma generated between the two electrodes toward the inner wall of the reaction vessel, and the plasma generated between the two electrodes can be suppressed. High-density plasma can be stably maintained between the two electrodes, and the density of the plasma between the two electrodes is almost uniform and axially symmetrical, which eliminates the difference in potential between the wafer and the wafer surface as in conventional methods, and the wafer It is possible to prevent damage to the formed device and is extremely advantageous in etching and thin film formation using plasma generated by gas discharge.
第1図はこの発明のプラズマ反応装置の一実施例の概略
図、第2図は第1図の一部の斜視図、第3図は第1図の
動作説明図、第4図は第1図の装置を用いたときのウェ
ハ電位及びウェハ表面の局所電位の分布図、第5図は従
来のプラズマ反応装置の概略図、第6図は第5図の装置
を用いたときのウェハ電位及びウェハ表面の局所電位の
分布図である。
図において、1は反応容器、3はカソード電極、4はア
ノード電極、12は多重カスプ磁場発生用コイルである
。
なお、各図中同一符号は同一または相当部分を示す。FIG. 1 is a schematic diagram of an embodiment of the plasma reactor of the present invention, FIG. 2 is a perspective view of a part of FIG. 1, FIG. 3 is an explanatory diagram of the operation of FIG. A distribution diagram of the wafer potential and local potential on the wafer surface when using the device shown in the figure, FIG. 5 is a schematic diagram of a conventional plasma reaction device, and FIG. FIG. 3 is a distribution diagram of local potential on the wafer surface. In the figure, 1 is a reaction vessel, 3 is a cathode electrode, 4 is an anode electrode, and 12 is a multi-cusp magnetic field generating coil. Note that the same reference numerals in each figure indicate the same or corresponding parts.
Claims (1)
けられ、前記両電極間で導入ガスの放電によるプラズマ
を発生するプラズマ反応装置において、 前記容器内の磁束密度が前記両電極間において極小とな
る極小磁場を発生する磁場発生手段を設けたことを特徴
とするプラズマ反応装置。(1) In a plasma reaction device in which two flat plate electrodes are provided in a reaction vessel in parallel and facing each other, and plasma is generated by discharge of introduced gas between the two electrodes, the magnetic flux density in the vessel is equal to the electrodes. 1. A plasma reactor characterized in that a magnetic field generating means is provided for generating a minimal magnetic field that becomes minimal between the plasma reactors.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17080790A JPH0456774A (en) | 1990-06-25 | 1990-06-25 | Plasma reactor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17080790A JPH0456774A (en) | 1990-06-25 | 1990-06-25 | Plasma reactor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH0456774A true JPH0456774A (en) | 1992-02-24 |
Family
ID=15911706
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17080790A Pending JPH0456774A (en) | 1990-06-25 | 1990-06-25 | Plasma reactor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0456774A (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005197456A (en) * | 2004-01-07 | 2005-07-21 | Komatsu Ltd | Light source device and exposure apparatus using the same |
-
1990
- 1990-06-25 JP JP17080790A patent/JPH0456774A/en active Pending
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2005197456A (en) * | 2004-01-07 | 2005-07-21 | Komatsu Ltd | Light source device and exposure apparatus using the same |
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