JPH0760797B2 - Amorphous thin film forming equipment - Google Patents
Amorphous thin film forming equipmentInfo
- Publication number
- JPH0760797B2 JPH0760797B2 JP61105109A JP10510986A JPH0760797B2 JP H0760797 B2 JPH0760797 B2 JP H0760797B2 JP 61105109 A JP61105109 A JP 61105109A JP 10510986 A JP10510986 A JP 10510986A JP H0760797 B2 JPH0760797 B2 JP H0760797B2
- Authority
- JP
- Japan
- Prior art keywords
- thin film
- substrate
- electrodes
- amorphous thin
- coil
- 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.)
- Expired - Fee Related
Links
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E10/00—Energy generation through renewable energy sources
- Y02E10/50—Photovoltaic [PV] energy
Landscapes
- Photovoltaic Devices (AREA)
Description
【発明の詳細な説明】 〔産業上の利用分野〕 この発明は,太陽電池,薄膜半導体,電子写真感光体や
光センサなどの,各種電子デバイスに使用される非晶質
薄膜の製造装置に関するものである。Description: TECHNICAL FIELD The present invention relates to an apparatus for producing an amorphous thin film used in various electronic devices such as a solar cell, a thin film semiconductor, an electrophotographic photosensitive member and an optical sensor. Is.
〔従来の技術〕 第2図には,従来より用いられている半導体薄膜の製造
装置を示してある。[Prior Art] FIG. 2 shows a conventional semiconductor thin film manufacturing apparatus.
図において,気密の反応容器01内に放電空間を形成する
ための電極02,03が上下方向に設けてあり,この電極02,
03は高周波電源04に電気的に接続されている。上記反応
容器01の外周には,上記放電空間内の電界方向と平行な
磁界を発生させるためのコイル05が水平に配置されてお
り,交流電源06と電気的に接続されている。排気孔07は
図示しない真空ポンプに連通しており,反応ガス導入管
08は,モノシランと水素ガスのボンベにそれぞれ連通し
ている。なお,09はヒータで,基板010を加熱するもので
ある。In the figure, electrodes 02, 03 for forming a discharge space are provided vertically in an airtight reaction vessel 01.
03 is electrically connected to the high frequency power supply 04. A coil 05 for generating a magnetic field parallel to the electric field direction in the discharge space is horizontally arranged on the outer periphery of the reaction vessel 01, and is electrically connected to an AC power source 06. The exhaust hole 07 communicates with a vacuum pump (not shown), and a reaction gas introduction pipe
08 communicates with the monosilane and hydrogen gas cylinders, respectively. A heater 09 heats the substrate 010.
さて,電極03上に基板010を載せ,反応容器01内を1mmHg
程度に減圧した後,モノシランと水素ガスとの混合ガス
を反応ガス導入管08より供給しつつ,電極02,03間に13.
5MHzの高周波電圧を印加する。Now, place the substrate 010 on the electrode 03, and set the inside of the reaction vessel 01 to 1 mmHg.
After reducing the pressure to a certain degree, while supplying a mixed gas of monosilane and hydrogen gas from the reaction gas introduction pipe 08, the pressure between the electrodes 02 and 03 was 13.
Apply high frequency voltage of 5MHz.
一方,コイル05には,50あるいは60Hzの商業用交流電圧
を印加し,電極02,03間に約100ガウスの磁界を発生させ
る。なお、基板010は,ヒータ09により300℃程度に加熱
しておく。On the other hand, a commercial AC voltage of 50 or 60 Hz is applied to the coil 05 to generate a magnetic field of about 100 gauss between the electrodes 02 and 03. The substrate 010 is heated to about 300 ° C. by the heater 09.
反応ガス導入管08より導入されたモノシラン等のガス
は,電極02,03間の放電空間で分解され,コイル05によ
り発生された磁界により撹拌されつつ基板010の表面に
付着し,非晶質薄膜を形成する。The gas such as monosilane introduced from the reaction gas introduction pipe 08 is decomposed in the discharge space between the electrodes 02 and 03, and is adhered to the surface of the substrate 010 while being stirred by the magnetic field generated by the coil 05. To form.
上記した従来の装置では,2枚の電極02,03間に発生する
電界の方向と平行にコイル05で磁界を印加するので,電
極02,03間の放電空間に存在するシリコン等のイオンが
撹拌され,基板010上に比較的均一な非晶質薄膜が形成
される。In the conventional device described above, since the magnetic field is applied by the coil 05 in parallel with the direction of the electric field generated between the two electrodes 02 and 03, ions such as silicon existing in the discharge space between the electrodes 02 and 03 are agitated. As a result, a relatively uniform amorphous thin film is formed on the substrate 010.
しかし, 基板010が置かれる場所は,電極03の上であり,電
極02,03間の放電空間内に位置することになる。このた
め,基本的に高エネルギーをもつイオンの直撃を受ける
ことになる。However, the place where the substrate 010 is placed is on the electrode 03, and is located in the discharge space between the electrodes 02 and 03. Therefore, basically, it is directly hit by ions having high energy.
すなわち,電極間の電界により電荷qのイオンにはク
ーロン力1=qが働き,イオン粒子が基板を直撃し
て形成されつつある非晶質薄膜に損傷を与えることにな
る。That is, due to the electric field between the electrodes, Coulomb force 1 = q acts on the ions of charge q, and the ion particles directly hit the substrate to damage the amorphous thin film that is being formed.
基板が一方の電極の上に載せられるので,一度に処
理させる基板の大きさも限定されることになり,電極よ
り面積の大きな基板に非晶質薄膜を形成することができ
ない。Since the substrate is placed on one of the electrodes, the size of the substrate to be processed at one time is limited, and the amorphous thin film cannot be formed on the substrate having a larger area than the electrode.
この発明の装置は,グロー筒状の反応容器と,同反応容
器内へ軸芯と平行に相対して収納された長尺な放電用電
極と,同放電用電極にグロー放電用電圧を供給する交流
電源と,上記反応容器を囲繞し軸芯方向に磁界を発生さ
せるコイルと,同コイルに磁界発生用の電流を供給する
電源とを有し,上記放電用電極間空間外に同放電用電極
と直角に置かれた基板へ非晶質薄膜を形成するものであ
る。The apparatus of the present invention supplies a glow-tube-shaped reaction container, a long discharge electrode housed in the reaction container in parallel with and parallel to the axis, and a glow discharge voltage to the discharge electrode. An AC power supply, a coil that surrounds the reaction vessel and generates a magnetic field in the axial direction, and a power supply that supplies a current for generating a magnetic field to the coil, and the discharge electrode is provided outside the space between the discharge electrodes. An amorphous thin film is formed on a substrate placed at a right angle.
この発明では,グロー放電プラズマを発生させる電極間
の放電用電界と直交する方向に磁界を発生させた。In the present invention, the magnetic field is generated in the direction orthogonal to the electric field for discharge between the electrodes for generating glow discharge plasma.
荷電粒子は放電電界より与えられたクーロン力と,磁界
により与えられたローレンツ力に初速を与えられた形で
電界と直交する方向にドリフトするが,電界空間を出た
ところでクーロン力が弱まりローレンツ力によるサイク
ロトロン運動によりLarmor軌道を描いて飛んでいく。The charged particles drift in the direction orthogonal to the electric field in a form in which the initial velocity is given to the Coulomb force given by the discharge electric field and the Lorentz force given by the magnetic field, but the Coulomb force weakens when leaving the electric field space and the Lorentz force is exerted. Draw a Larmor orbit by the cyclotron motion by and fly.
一方,電気的に中性であるラジカル粒子は荷電粒子群の
軌道からそれて直進しようとする。On the other hand, electrically neutral radical particles deviate from the orbits of the charged particle group and try to go straight.
従って,放電電界空間外へ該電界と平行に基板を支持す
れば,基板の表面に荷電粒子のダメージの無い非晶質薄
膜が形成されることになる。Therefore, if the substrate is supported outside the discharge electric field space in parallel with the electric field, an amorphous thin film without damage of charged particles is formed on the surface of the substrate.
また,電極は長尺であって,筒状の反応容器内に軸芯と
平行に配置されているので,長尺な基板にも非晶質薄膜
を形成することができる。Moreover, since the electrodes are long and arranged in parallel with the axis in the tubular reaction vessel, an amorphous thin film can be formed on a long substrate.
以下,この発明を第1図に示す一実施例の装置に基づき
説明する。The present invention will be described below based on the apparatus of one embodiment shown in FIG.
1は筒状の反応容器で,その中にグロー放電プラズマを
発生させるための長尺な電極2・3が軸芯と平行に対向
して配置されている。4は交流電源で,上記電極2・3
に接続されている。コイル5は,上記反応容器1を囲繞
するもので,電源6に接続されている。7は反応ガス導
入管で,図示しないボンベに連通し,モノシランとアル
ゴンの混合ガスを上記反応容器1に供給するものであ
る。排気孔8は,真空ポンプ9に連通しており,反応容
器1内のガスを排気するものである。Reference numeral 1 denotes a cylindrical reaction vessel in which long electrodes 2 and 3 for generating glow discharge plasma are arranged so as to face each other in parallel with the axis. 4 is an AC power supply, the electrodes 2 and 3 above
It is connected to the. The coil 5 surrounds the reaction vessel 1 and is connected to the power source 6. Reference numeral 7 denotes a reaction gas introduction pipe, which is connected to a cylinder (not shown) and supplies a mixed gas of monosilane and argon to the reaction container 1. The exhaust hole 8 communicates with the vacuum pump 9 and exhausts the gas in the reaction vessel 1.
さて,基板10を図示のように電極2・3の面と直交する
方向で,かつ,電極2・3が形成する放電空間の外側に
適宜手段で支持する。真空ポンプ9を駆動して反応容器
1内を排気した後,反応ガス導入管7からモノシランと
アルゴンの混合ガスを供給する。上記混合ガスを反応容
器1内に充満させて圧力を0.05ないし0.5Torrに保ち,
低周波電源4から電極2・3に電圧を印加するとグロー
放電プラズマが電極2・3間に発生する。Now, the substrate 10 is supported by an appropriate means in a direction orthogonal to the surface of the electrodes 2 and 3 and outside the discharge space formed by the electrodes 2 and 3 as shown in the figure. After the vacuum pump 9 is driven to exhaust the inside of the reaction vessel 1, a mixed gas of monosilane and argon is supplied from the reaction gas introduction pipe 7. The reaction vessel 1 is filled with the above mixed gas to keep the pressure at 0.05 to 0.5 Torr,
When a voltage is applied from the low frequency power source 4 to the electrodes 2 and 3, glow discharge plasma is generated between the electrodes 2 and 3.
一方,コイル5は,電極2・3間に発生する電界と直
交する方向の磁界を発生させる。なお,その磁束密度
は10ガウス程度で良い。On the other hand, the coil 5 generates a magnetic field in a direction orthogonal to the electric field generated between the electrodes 2 and 3. The magnetic flux density may be about 10 gauss.
反応ガス導入管7から供給されたガスのうちモノシラン
ガスは,電極2・3の間に生じるグロー放電プラズマで
ラジカルSiに分解され,基板10の表面に付着し薄膜を形
成する。Of the gas supplied from the reaction gas introduction pipe 7, monosilane gas is decomposed into radical Si by glow discharge plasma generated between the electrodes 2 and 3, and adheres to the surface of the substrate 10 to form a thin film.
このとき,アルゴンイオン等の荷電粒子は,電極2・3
間で電界Eによるクーロン力1=qとローレンツ力
2=q(×)によっていわゆる×ドリフトの
運動を起こす。At this time, charged particles such as argon ions will be absorbed by the electrodes 2 and 3.
Coulomb force 1 = q and Lorentz force due to electric field E between
2 = q (x) causes a so-called x drift motion.
なお,は荷電粒子の速度である。Note that is the velocity of the charged particles.
すなわち,×ドリフトにより初速を与えられた形
で,電極2・3と直交する方向に飛び出し,基板10に向
けて飛んでいく。しかし,電極2・3間に生じる電界の
影響が小さい放電空間の外側では,コイル5により生じ
た磁界によるサイクロトロン運動によりLarmor軌道を
描いて飛んでいく。That is, in the form in which the initial velocity is given by the x drift, it jumps out in the direction orthogonal to the electrodes 2 and 3 and flies toward the substrate 10. However, outside the discharge space where the influence of the electric field generated between the electrodes 2 and 3 is small, the magnetic field generated by the coil 5 causes a cyclotron motion to fly along a Larmor trajectory.
従って,アルゴンイオン等の荷電粒子が基板10を直撃す
ることはなくなる。Therefore, charged particles such as argon ions do not hit the substrate 10 directly.
一方,電気的に中性であるラジカルSiは磁界の影響を
受けず,上記荷電粒子群の軌道よりそれで基板10に至
り,その表面に非晶質薄膜を形成する。On the other hand, the electrically neutral radicals Si are not affected by the magnetic field and reach the substrate 10 from the orbits of the charged particle groups, forming an amorphous thin film on the surface thereof.
この発明によれば,太陽電池・電子写真感光体などの各
種ディバイスの製造において,大面積の非晶質薄膜が形
成されることになるので,産業上きわめて価値がある。According to the present invention, a large-area amorphous thin film is formed in the production of various devices such as solar cells and electrophotographic photoconductors, which is extremely valuable in industry.
第1図は本発明の一実施例を示す装置の横断面図, 第2図は従来装置の側断面図である。 1……反応容器,2,3……電極, 4……交流電源,5……コイル,6……電源, 7……反応ガス導入管,8……排気孔, 9……真空ポンプ,10……基板。 FIG. 1 is a lateral sectional view of an apparatus showing an embodiment of the present invention, and FIG. 2 is a side sectional view of a conventional apparatus. 1 ... Reaction vessel, 2, 3 ... Electrode, 4 ... AC power supply, 5 ... Coil, 6 ... Power supply, 7 ... Reaction gas introduction pipe, 8 ... Exhaust hole, 9 ... Vacuum pump, 10 ……substrate.
Claims (1)
平行に相対して収納された長尺な放電用電極と,同放電
用電極にグロー放電用電圧を供給する交流電源と,上記
反応容器を囲繞し軸芯方向に磁界を発生させるコイル
と,同コイルに磁界発生用の電流を供給する電源とを有
し,上記放電用電極間空間外に同放電用電極と直角に置
かれた基板へ非晶質薄膜を形成することを特徴とする非
晶質薄膜形成装置。1. A cylindrical reaction vessel, a long discharge electrode housed in the reaction vessel in parallel with and parallel to an axis, and an AC power supply for supplying a glow discharge voltage to the discharge electrode. And a coil that surrounds the reaction container and generates a magnetic field in the axial direction, and a power supply that supplies a current for generating a magnetic field to the coil, and is perpendicular to the discharge electrode outside the discharge electrode space. An amorphous thin film forming apparatus characterized by forming an amorphous thin film on a substrate placed on a substrate.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61105109A JPH0760797B2 (en) | 1986-05-08 | 1986-05-08 | Amorphous thin film forming equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP61105109A JPH0760797B2 (en) | 1986-05-08 | 1986-05-08 | Amorphous thin film forming equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62261121A JPS62261121A (en) | 1987-11-13 |
| JPH0760797B2 true JPH0760797B2 (en) | 1995-06-28 |
Family
ID=14398677
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP61105109A Expired - Fee Related JPH0760797B2 (en) | 1986-05-08 | 1986-05-08 | Amorphous thin film forming equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0760797B2 (en) |
-
1986
- 1986-05-08 JP JP61105109A patent/JPH0760797B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62261121A (en) | 1987-11-13 |
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Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| LAPS | Cancellation because of no payment of annual fees |