JP2706022B2 - ECR plasma processing method - Google Patents
ECR plasma processing methodInfo
- Publication number
- JP2706022B2 JP2706022B2 JP4270485A JP27048592A JP2706022B2 JP 2706022 B2 JP2706022 B2 JP 2706022B2 JP 4270485 A JP4270485 A JP 4270485A JP 27048592 A JP27048592 A JP 27048592A JP 2706022 B2 JP2706022 B2 JP 2706022B2
- Authority
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- Prior art keywords
- magnetic field
- plasma processing
- processing method
- microwave
- coil
- Prior art date
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- Expired - Lifetime
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- Coating By Spraying Or Casting (AREA)
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Description
【0001】[0001]
【産業上の利用分野】本発明は、ECRプラズマエッチ
ングおよびコーティング加工方法に関する。The present invention relates to an ECR plasma etching and coating method.
【0002】[0002]
【従来の技術】従来のECRプラズマ加工方法は、マイ
クロ波の進行方向と平行に一定磁界0.0875Tを与
えて電子の円運動を生じさせ、その角振動数ωCとマイ
クロ波の角振動数ωとが一致するECR現象を利用し
て、電子により試料全面の処理を行う方法である。2. Description of the Related Art In a conventional ECR plasma processing method, a constant magnetic field of 0.0875 T is applied in parallel with the direction of propagation of a microwave to generate circular motion of electrons, and its angular frequency ω C and angular frequency of the microwave This is a method in which the entire surface of the sample is processed by electrons using the ECR phenomenon in which ω coincides.
【0003】[0003]
【発明が解決しようとする課題】従来のECRプラズマ
加工方法では、マイクロ波の角振動数ωと電子の円運動
による角振動数ωCとが一致したECR現象によってイ
オン散乱しているため、加工点が広い面となり目的の部
分のみの精密なプラズマ加工ができなかった。そのた
め、部分処理の時はマスクを使用しなければならなかっ
た。しかしながら、図4に示すように、マスクを使用し
ても、イオン散乱のため試料の加工部分はθ°だけ先拡
がりとなり、しかも加工底面は中心が浅く周辺が深いう
ねりをもつものとなる。又、イオン散乱を少なくするた
めにイオンを集束するには、イオンの質量は電子の質量
の1758倍も大きく、可成りの電磁力が必要である。In THE INVENTION Problems to be Solved by conventional ECR plasma processing method, since the ion scattering by ECR phenomenon and angular frequency omega C by circular motion of the angular frequency omega and the electronic microwave match, processed The point was a wide surface, and precise plasma processing of only the target portion could not be performed. Therefore, at the time of partial processing, a mask had to be used. However, as shown in FIG. 4, even when a mask is used, the processed portion of the sample spreads by θ ° due to ion scattering, and the processed bottom surface has a shallow center and a deep undulation at the periphery. In order to focus ions to reduce ion scattering, the mass of the ions is 1758 times larger than the mass of the electrons, and a considerable electromagnetic force is required.
【0004】そこで本発明は、ECRプラズマ処理によ
る極小部分の加工や被覆を正確に高速に、効率良く実施
することを目的とするものである。Accordingly, an object of the present invention is to perform processing and coating of an extremely small portion by ECR plasma processing accurately, quickly, and efficiently.
【0005】[0005]
【課題を解決するための手段】本発明は、マイクロ波の
進行方向と平行に、又は垂直に、又は垂直にそして平行
に磁界を与えて生じる電子サイクロトロン共鳴(EC
R)現象を利用したECRプラズマ処理方法において、
磁力線が回転し、その回転径が被加工体に近くなるにし
たがって小さくなるような漏斗型の中心をもった磁力線
回転コイルにパルス電圧を印加することによって磁力線
を回転させ、プラズマ中のイオンを漏斗型に沿って集束
し、イオン流を絞って被加工体面に当てて加工すること
を特徴とするECRプラズマ処理方法である。磁束の回
転は、例えば図2に示すイオン集束用のパルス磁界発生
コイルを用いて発生させる。すなわち、ヨーク11に複
数のコイル12を巻回し中心部を漏斗型に形成したもの
で、これにパルス電流を与えることにより、個々のコイ
ル12間に回転磁束(図中点線と矢印で示す)を発生さ
せる。この回転磁束の中心にイオン流を通すことによっ
て、イオン流が漏斗型に沿って中心部に集束される。し
たがってこのパルス磁界発生コイルの中心を試料面に当
てて、パルス幅のピーク電圧や休止時間を変えること
で、1.7T以上のパルス磁界を与え、パルス幅は0.
01〜500msのパルス電流をコイルに通電して回転
磁束を発生させるとイオンが集束されて精密な加工がで
きる。SUMMARY OF THE INVENTION The present invention relates to an electron cyclotron resonance (EC) generated by applying a magnetic field in a direction parallel to, or perpendicular to, or perpendicular to and parallel to the traveling direction of microwaves.
R) In an ECR plasma processing method using a phenomenon,
Magnetic field lines is rotated, the rotation diameter rotates the result lines of magnetic force applying becomes smaller like about the pulse voltage to the magnetic field lines rotating coil having funnel according closer to the object to be processed, ions in the plasma This is an ECR plasma processing method characterized by converging along a funnel shape, narrowing an ion flow, and processing the ion beam against a surface of a workpiece. The rotation of the magnetic flux is generated using, for example, a pulse magnetic field generating coil for ion focusing shown in FIG. That is, a plurality of coils 12 are wound around the yoke 11 to form a central portion in a funnel shape, and a pulse current is applied to the yoke 11 so that a rotating magnetic flux (indicated by a dotted line and an arrow in the drawing) is generated between the individual coils 12. generate. By passing the ion current through the center of the rotating magnetic flux, the ion current is focused on the center along the funnel shape. Therefore, it is necessary to change the peak voltage of the pulse width and the pause time by applying the center of this pulse magnetic field generating coil to the sample surface.
In the above, a pulse magnetic field of 1.7 T or more is applied, and the pulse width is set to 0.1.
When a pulse current of 01 to 500 ms is applied to the coil to generate a rotating magnetic flux, the ions are focused and precise processing can be performed.
【0006】すなわち、パルスτon時の瞬時には直流磁
界の数百倍以上の回転磁束が生じるため、イオンは集束
されてその中心をまっ直に進み、被加工材表面に達する
ため、極小部分の加工や被覆が正確に高速になり、パル
ス幅を小さくすることにより、イオン加速が大きくなり
効率を良くすることができる。That is, at the moment of the pulse τ on, a rotating magnetic flux of several hundred times or more of the DC magnetic field is generated, so that the ions are focused and travel straight along the center thereof, reach the surface of the workpiece, and have a very small portion. Accurately high-speed processing and coating, and reducing the pulse width, increase the ion acceleration and improve the efficiency.
【0007】本発明は又、マイクロ波の進行方向に平行
な磁界を発生させるコイル、又はマイクロ波の進行方向
に垂直な磁界を発生させるコイルにもパルス電圧を印加
すると、従来の一定磁界を越える磁界を生じ、プラズマ
閉じ込め効果も良くなり、イオン旋回曲率と速度の減少
とイオン温度の低下によって高異方性処理による正確で
高速な低損傷加工を施すことができる。[0007] The present invention is also directed to a structure which is parallel to the traveling direction of microwaves.
Coil that generates a strong magnetic field, or the traveling direction of the microwave
When a pulse voltage is also applied to a coil that generates a magnetic field perpendicular to the magnetic field, a magnetic field exceeding the conventional constant magnetic field is generated, the plasma confinement effect is improved, and a high anisotropy is caused by a decrease in the ion rotation curvature and velocity and a decrease in the ion temperature. Accurate, high-speed, low-damage processing by processing can be performed.
【0008】[0008]
【実施例】実施例を図面に基づいて説明する。An embodiment will be described with reference to the drawings.
【0009】図1において、1は被加工材で、2はイオ
ン集束用パルス磁界発生コイルで中心部は漏斗型に形成
してある。3はマイクロ波の進行方向に平行なパルス磁
界を発生させるコイル、5はイオン源においてマイクロ
波の進行方向に垂直なパルス磁界を発生させるコイル、
4はヨーク、6はイオン源であり、7は冷却水排水口、
8は2.45GHzのマイクロ波の進行方向を示す。9
は反応ガス導入口で、10は冷却水導入口である。図2
における11は、図1のA−A’断面のヨークで、12
はコイルである。In FIG. 1, reference numeral 1 denotes a workpiece, 2 denotes a pulse magnetic field generating coil for ion focusing, and a center portion is formed in a funnel shape. 3 is a coil for generating a pulse magnetic field parallel to the direction in which the microwave travels, 5 is a coil for generating a pulse magnetic field in the ion source perpendicular to the direction in which the microwave travels,
4 is a yoke, 6 is an ion source, 7 is a cooling water drain,
8 indicates the traveling direction of the microwave of 2.45 GHz. 9
Is a reaction gas inlet, and 10 is a cooling water inlet. FIG.
Reference numeral 11 denotes a yoke having a section taken along the line AA ′ in FIG.
Is a coil.
【0010】次に具体的な加工例について説明する。Next, a specific processing example will be described.
【0011】例えばSiO2を被加工材とした場合、エ
ッチングガスとして、CF4+20%H2を流し、0.0
5Torrの雰囲気中で高電離プラズマを生成させるた
め、マイクロ波の進行方向と平行方向に一定磁界0.0
875Tとなる磁界を与え、イオン濃度を高め、さらに
イオン濃度を低温化のため、プラズマ安定化の閉じ込め
磁場として垂直方向に一定磁界0.0875Tの磁界を
与えた。そして図2のイオン集束用パルス磁界発生コイ
ルにパルス電流を流し、平均磁界1.7Tの磁界を与え
ることでイオンの集束を計った。For example, when SiO 2 is used as a workpiece, CF 4 + 20% H 2 is flowed as an etching gas,
In order to generate highly ionized plasma in an atmosphere of 5 Torr, a constant magnetic field of 0.0 is applied in a direction parallel to the microwave traveling direction.
A magnetic field of 875T was applied to increase the ion concentration and further reduce the ion concentration. A constant magnetic field of 0.0875T was applied in the vertical direction as a confinement magnetic field for plasma stabilization. Then, a pulse current was applied to the ion focusing pulse magnetic field generating coil shown in FIG. 2 to apply a magnetic field having an average magnetic field of 1.7 T to measure ions.
【0012】その結果、最高0.4μm/minの高速
エッチングを行うことができた。これは従来方法の8倍
のエッチング速度である。又、回り込み角は、従来の1
4°に対して最低0.8°であり、マスクなしで極めて
優れた部分処理が得られた。この時パルス幅条件と結果
を表1に示す。As a result, high-speed etching at a maximum of 0.4 μm / min could be performed. This is eight times the etching rate of the conventional method. Also, the wraparound angle is the conventional 1
At least 0.8 ° for 4 °, and extremely excellent partial treatment was obtained without a mask. Table 1 shows the pulse width conditions and the results at this time.
【0013】[0013]
【表1】 [Table 1]
【0014】又、被加工材としてAl2O3についても加
工したところ、表2に示す如くイオン集束の効果が得ら
れ、マスク無し加工が可能であることが判った。When Al 2 O 3 was also processed as a workpiece, it was found that the effect of ion focusing was obtained as shown in Table 2, and that processing without a mask was possible.
【0015】[0015]
【表2】 [Table 2]
【0016】次にSiを被加工材として、Alの薄膜抵
抗体コーティングを行った。ガスとしてAl(C2H5)
2を流し、1Torrの雰囲気中でコーティング処理を
行った。高電離プラズマ生成のためと異方性効果を高め
るための磁界は平均0.0875Tとした。Next, a thin film resistor coating of Al was performed using Si as a workpiece. Al (C 2 H 5 ) as gas
2 and the coating treatment was performed in an atmosphere of 1 Torr. The magnetic field for generating highly ionized plasma and for enhancing the anisotropic effect was 0.0875T on average.
【0017】イオン集束用磁界として平均1.7Tの磁
界を与えてコーティングを行った。その結果を表3に示
す。例えばτon0.005msの場合、被覆速度は3.
4μm/min、面粗度は0.08μHmax、厚み差は
0.026μm/mm2であり均一である。The coating was performed by applying an average magnetic field of 1.7 T as a magnetic field for ion focusing. Table 3 shows the results. For example, in the case of τ on 0.005 ms, the coating speed is 3.
4 [mu] m / min, surface roughness is 0.08μH max, the thickness difference is uniform was 0.026 / mm 2.
【0018】[0018]
【表3】 [Table 3]
【0019】次にSiO2を被加工材とし、エッチング
ガスとしてCF4+20%H2を流し、0.05Torr
の雰囲気中で高電離プラズマを生成させるため、マイク
ロ波の進行方向と平行方向に磁界を与えた場合の試験結
果を表4に示す。又、マイクロ波の進行方向と垂直方向
に磁界を与えた場合の試験結果を表5にそれぞれ示す。Next, using SiO 2 as a work material, flowing CF 4 + 20% H 2 as an etching gas, and applying 0.05 Torr
Table 4 shows the test results when a magnetic field was applied in a direction parallel to the traveling direction of the microwaves in order to generate highly ionized plasma in the atmosphere described above. Table 5 shows the test results when a magnetic field was applied in the direction perpendicular to the direction in which the microwaves traveled.
【0020】[0020]
【表4】 [Table 4]
【0021】[0021]
【表5】 [Table 5]
【0022】又、前記表1,2,3に対応して、平行コ
イルと垂直コイルにパルスの平均磁界0.0875Tを
連続的に印加した場合の試験結果を表6、表7、表8に
示す。According to Tables 1, 2 and 3, an average pulse magnetic field of 0.0875T is applied to the parallel coil and the vertical coil.
Tables 6, 7, and 8 show the test results when the voltage was continuously applied.
【0023】[0023]
【表6】 [Table 6]
【0024】[0024]
【表7】 [Table 7]
【0025】[0025]
【表8】 [Table 8]
【0026】[0026]
【発明の効果】本発明によれば、イオン集束用コイルに
パルス電流を流し、パルス磁界を与えることにより、イ
オンを集速して高速化し、マスクなしでの異方性エッチ
ング並びにコーティング処理を行うことができる。した
がって、高密度基板に高異方性ECRプラズマ処理を施
すことができる。According to the present invention, by applying a pulse current to the ion focusing coil and applying a pulse magnetic field, the ions are focused and speeded up, and anisotropic etching and coating without a mask are performed. be able to. Therefore, a highly anisotropic ECR plasma treatment can be performed on a high-density substrate.
【図1】本発明の実施例の説明図である。FIG. 1 is an explanatory diagram of an embodiment of the present invention.
【図2】図1のA−A’断面図である。FIG. 2 is a sectional view taken along line A-A 'of FIG.
【図3】プラズマエッチング、コーティング加工におけ
る回り込み角の説明図である。FIG. 3 is an explanatory diagram of a wraparound angle in plasma etching and coating processing.
【図4】従来のイオン散乱の説明図である。FIG. 4 is an explanatory diagram of conventional ion scattering.
1 被加工材 2 イオン集束用パルス磁界発生コイル 3 マイクロ波と平行なパルス磁界発生コイル 4 ヨーク 5 マイクロ波に垂直なパルス磁界発生コイル 6 イオン源 7 冷却水排水管 8 マイクロ波の進行方向 9 反応ガス導入管 10 冷却水導入管 11 ヨーク 12 コイルREFERENCE SIGNS LIST 1 workpiece 2 pulse magnetic field generating coil for ion focusing 3 pulse magnetic field generating coil parallel to microwave 4 yoke 5 pulse magnetic field generating coil perpendicular to microwave 6 ion source 7 cooling water drain pipe 8 microwave traveling direction 9 reaction Gas inlet pipe 10 Cooling water inlet pipe 11 Yoke 12 Coil
───────────────────────────────────────────────────── フロントページの続き (72)発明者 嶋 好範 神奈川県川崎市麻生区王禅寺768番地15 (72)発明者 大場 章 埼玉県朝霞市浜崎1丁目9番地の3− 205 (56)参考文献 特開 平3−229859(JP,A) ──────────────────────────────────────────────────続 き Continuation of front page (72) Inventor Yoshinori Shima 768-15 Ozenji Temple, Aso-ku, Kawasaki City, Kanagawa Prefecture (72) Inventor Akira Oba 3-205, 1-9-9 Hamasaki, Asaka-shi, Saitama JP-A-3-229859 (JP, A)
Claims (2)
直に、又は垂直にそして平行に磁界を与えて生じる電子
サイクロトロン共鳴(ECR)現象を利用したECRプ
ラズマ処理方法において、磁力線が回転し、その回転径
が被加工体に近くなるにしたがって小さくなるような漏
斗型の中心をもった磁力線回転コイルにパルス電圧を印
加することによって磁力線を回転させ、プラズマ中のイ
オンを漏斗型に沿って集束し、イオン流を絞って被加工
体面に当てて加工することを特徴とするECRプラズマ
処理方法。1. The method according to claim 1, wherein the direction is parallel to or perpendicular to the traveling direction of the microwave.
In an ECR plasma processing method using an electron cyclotron resonance (ECR) phenomenon generated by applying a magnetic field directly, or vertically and in parallel , a magnetic field line rotates so that a line of rotation becomes smaller as the diameter of rotation becomes closer to a workpiece. Pulse voltage is applied to the rotating magnetic coil with a funnel-shaped center
Thus by rotating the magnetic field lines to pressure, the ions in the plasma converging along the funnel, ECR plasma processing method characterized by machining against the workpiece body surface squeezing ion stream.
生させるコイル、又はマイクロ波の進行方向に垂直な磁
界を発生させるコイルにパルス電圧を印加する請求項1
記載のECRプラズマ処理方法。2. A magnetic field parallel to the traveling direction of the microwave is generated.
Coils or magnets perpendicular to the direction of microwave travel.
2. A pulse voltage is applied to a coil for generating a field.
The ECR plasma processing method described in the above.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4270485A JP2706022B2 (en) | 1992-10-08 | 1992-10-08 | ECR plasma processing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP4270485A JP2706022B2 (en) | 1992-10-08 | 1992-10-08 | ECR plasma processing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06124796A JPH06124796A (en) | 1994-05-06 |
| JP2706022B2 true JP2706022B2 (en) | 1998-01-28 |
Family
ID=17486953
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP4270485A Expired - Lifetime JP2706022B2 (en) | 1992-10-08 | 1992-10-08 | ECR plasma processing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2706022B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2020214226A1 (en) * | 2019-01-27 | 2020-10-22 | Lyten, Inc. | Covetic materials |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH03229859A (en) * | 1990-02-05 | 1991-10-11 | Nippon Steel Corp | Plasma treating device |
-
1992
- 1992-10-08 JP JP4270485A patent/JP2706022B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH06124796A (en) | 1994-05-06 |
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