JPH0199213A - Device for formation of film - Google Patents
Device for formation of filmInfo
- Publication number
- JPH0199213A JPH0199213A JP62256403A JP25640387A JPH0199213A JP H0199213 A JPH0199213 A JP H0199213A JP 62256403 A JP62256403 A JP 62256403A JP 25640387 A JP25640387 A JP 25640387A JP H0199213 A JPH0199213 A JP H0199213A
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- electrode
- film
- high frequency
- film forming
- 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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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
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- Photovoltaic Devices (AREA)
Abstract
Description
【発明の詳細な説明】
[技術分野]
本発明は、グロー放電により連続的に薄膜を形成する成
膜装置に関するものであり、とくに、高性能の半導体薄
膜を高成膜速度において均一に形成する成膜装置に関す
る。[Detailed Description of the Invention] [Technical Field] The present invention relates to a film forming apparatus that continuously forms thin films by glow discharge, and in particular, relates to a film forming apparatus that uniformly forms a high performance semiconductor thin film at a high film forming rate. It relates to a film forming apparatus.
[従来技術]
シリコン化合物のグロー放電分解や光分解により得られ
る非晶質シリコン系の半導体薄膜は、光−電気エネルギ
ーの変換能力に優れ、光起電力素子として利用されてい
る。しかも、電卓等民生用機器ばかりでなく、電力用太
陽電池としての利用も検討されているが、このためには
、大面積の太陽電池を安価に製造する必要がある。この
点においても、非晶質シリコン系太陽電池は、基本的に
面積の拡大が比較的容易であり、大面積化の研究が行わ
れている。[Prior Art] Amorphous silicon-based semiconductor thin films obtained by glow discharge decomposition or photodecomposition of silicon compounds have an excellent ability to convert light to electrical energy, and are used as photovoltaic devices. Furthermore, use is being considered not only for consumer devices such as calculators, but also as power solar cells, but for this purpose it is necessary to manufacture large-area solar cells at low cost. In this respect, it is basically relatively easy to expand the area of amorphous silicon-based solar cells, and research on increasing the area is being conducted.
しかしながら、従来の容量結合型の平行平板電極を用い
る成膜装置においては、高性能の半導体薄膜を高成膜速
度で均一に形成するとき、いくつかの問題があった。However, conventional film forming apparatuses using capacitively coupled parallel plate electrodes have had several problems when uniformly forming a high performance semiconductor thin film at a high film forming rate.
すなわち、まず第一にこの成膜方法は高周波が印加され
る電極(高周波印加電極)と接地されている電極(接地
電極)の間に膜が形成される基板が設置されるものであ
るが、この場合、高周波印加電極面内において、グロー
放電の均一性が確保されなければ、薄膜の均一性は得ら
れない0次に、大面積の基板に成膜する場合には、当然
のことながら、高周波印加電極の面積を基板よりも大き
くせねばならないが、大面積の電極においては、高周波
電流独特の表皮効果が生じて有効に高周波電流を導入す
ることができない。また、電気力線にもとすく端効果お
よび先の表皮効果の結果、高周波印加電極周辺部のグロ
ー放電が強くなり、成膜速度が不均一になるばかりでな
く、得られた薄膜の特性も不均一となるうえ、高速成膜
条件においては、高周波印加電極周辺部のグロー放電は
より一層強くなり、かかる問題点がさらに一層強澗され
る。That is, first of all, in this film forming method, a substrate on which a film is formed is installed between an electrode to which a high frequency is applied (high frequency application electrode) and an electrode that is grounded (ground electrode). In this case, the uniformity of the thin film cannot be obtained unless the uniformity of the glow discharge is ensured within the plane of the high-frequency applied electrode.Naturally, when depositing a film on a large-area substrate, The area of the high frequency application electrode must be made larger than the substrate, but with a large area electrode, a skin effect peculiar to high frequency current occurs, making it impossible to effectively introduce high frequency current. In addition, as a result of the edge effect and skin effect on the electric lines of force, glow discharge becomes stronger around the electrode to which high frequency is applied, which not only makes the film formation rate uneven, but also deteriorates the properties of the obtained thin film. In addition to the non-uniformity, under high-speed film formation conditions, the glow discharge around the high-frequency application electrode becomes even stronger, further exacerbating this problem.
[発明の目的]
本発明の目的は、高周波印加tF11と接地電極間にお
いて、高濃度プラズマを生じさせ、均一な半導体薄膜を
高成膜速度で基板上に形成することのできる半導体薄膜
の所謂インライン成膜装置を提供することである。[Object of the Invention] The object of the present invention is to generate a high concentration plasma between the high frequency application tF11 and the ground electrode, and to form a uniform semiconductor thin film on a substrate at a high deposition rate. An object of the present invention is to provide a film forming apparatus.
[基本的着想コ
本発明者らは、かかる観点から鋭意検討した結果、連続
形成に用いられる種々のプラズマCVD装置およびグロ
ー放電の詳細な検討の結果、高周波印加電極表面を凹凸
に形成することにより、電極全体に高濃度プラズマが均
一に拡がることを見いだして、本発明を完成するに至っ
た。すなわち大面積の平行平板電極においては上記のご
とく電極面上でプラズマが局在すると云う問題点がある
ところ、本発明者らは、特定の表面形状の電極を用いる
と、高密度のプラズマが雪掻全面に一様に生成すること
をみいだし、これをインライン方式の成膜装置による高
速成膜に利用したものである。[Basic idea] As a result of intensive studies from this point of view, and detailed studies of various plasma CVD devices and glow discharges used for continuous formation, the inventors found that by forming the surface of the high-frequency application electrode in an uneven manner, They discovered that high-concentration plasma spreads uniformly over the entire electrode, leading to the completion of the present invention. In other words, parallel plate electrodes with large areas have the problem that plasma is localized on the electrode surface as described above, but the present inventors found that when electrodes with a specific surface shape are used, high-density plasma is It was found that the film was formed uniformly over the scratched surface, and this was utilized for high-speed film formation using an in-line film forming apparatus.
[発明の開示〕
本発明は、高周波印加電極と接地電極の間に発生するグ
ロー放電中に、基板を設置・もしくは進行せしめて該基
板上に薄膜を形成するインライン成膜装置において、該
高周波印加電極表面が凹凸状に形成されていることを特
徴とする成膜装置、にかかるものである。[Disclosure of the Invention] The present invention provides an in-line film forming apparatus for forming a thin film on a substrate by setting or advancing a substrate during a glow discharge generated between a high frequency applying electrode and a grounded electrode. The present invention relates to a film forming apparatus characterized in that an electrode surface is formed in an uneven shape.
本発明の対象としているインライン成膜装置とは、真空
を破ることなく基板(実際には、基板保持具に保持固定
された基板)を成膜室に搬送し、基板は成膜室内に設置
され、もしくは室内を移動・進行しながら半導体薄膜が
形成される装置である。The in-line film forming apparatus that is the object of the present invention transports a substrate (actually, a substrate held and fixed to a substrate holder) to a film forming chamber without breaking the vacuum, and the substrate is installed in the film forming chamber. Alternatively, it is an apparatus in which a semiconductor thin film is formed while moving and progressing within a room.
第1図に本発明の一実施例たる具体的な態様を模式的な
断面図で示した。FIG. 1 shows a specific embodiment of the present invention in a schematic cross-sectional view.
すなわち、高周波印加電極1と接地電極2の間に発生す
るグロー放電中に、基板4を設置せしめて該基板上に薄
膜を形成するインライン成膜装置において、液高周波印
加電極表面が凹凸状に形成されている成膜装置である。That is, in an in-line film forming apparatus in which a substrate 4 is placed during a glow discharge generated between a high frequency applying electrode 1 and a ground electrode 2 and a thin film is formed on the substrate, the surface of the liquid high frequency applying electrode is formed in an uneven shape. This is a film-forming device that has been used for many years.
なお、第2図はその斜視図である。もちろん、基板4は
グロー放電中を移動・進行せしめられ、該基板上に薄膜
が連続的に形成されることも出来る。Note that FIG. 2 is a perspective view thereof. Of course, the substrate 4 can be moved and advanced through the glow discharge, and the thin film can be continuously formed on the substrate.
本発明において、凹凸の形状は特に限定されないが、製
作上からは、断面を矩形に作ることがプラズマの均一性
もそこなわれないので実用的であり好ましい。第1図に
示したものの外に、断面が矩形である高周波印加電極の
凹凸形状における具体的な示例のいくつかを第3図に示
す。In the present invention, the shape of the unevenness is not particularly limited, but from the viewpoint of manufacturing, it is practical and preferable to make the cross section rectangular because the uniformity of the plasma is not impaired. In addition to what is shown in FIG. 1, FIG. 3 shows some specific examples of uneven shapes of high-frequency applying electrodes having rectangular cross sections.
第1図に示すような高周波印加電極の凹凸における山の
高さh5すなち凹部の深さは、電極間隔dの172以上
、好ましくはdと同じかそれ以上である。けだし、高速
成膜条件においては成膜時の圧力を高めることが要求さ
れるので、山の高さhが電極間隔dに比べて1/2未満
のように小さい場合には、電極表面を凹凸に形成した効
果が小さくなり、好ましいものではない。また、薄膜の
均一性は高周波印加電極と接地電極との間隔dや高周波
印加電極と基板との間隔等の装置形状によっても影響さ
れるが、高周波印加電極の凹凸における山の高さhを電
極間隔dの1/2以上、好ましくはdと同じかそれ以上
とすることにより、これらの装置形状による影響をほと
んど無くすことが可能である。The height h5 of the ridges in the unevenness of the high-frequency applying electrode as shown in FIG. 1, that is, the depth of the recesses, is 172 or more of the electrode spacing d, preferably the same as or more than d. However, under high-speed film-forming conditions, it is required to increase the pressure during film-forming, so if the peak height h is less than 1/2 of the electrode spacing d, the electrode surface may be uneven. This is not preferable because the effect created by the process becomes smaller. The uniformity of the thin film is also affected by the shape of the device, such as the distance d between the high-frequency applying electrode and the ground electrode and the distance between the high-frequency applying electrode and the substrate. By setting the distance to 1/2 or more of the distance d, preferably the same as or more than d, it is possible to almost eliminate the influence of these device shapes.
一方、第1図、第2図に示すような高周波印加電極の凹
凸における山の巾Wすなわち凸部の幅は、電極間隔dの
172以上、好ましくはdと同じかそれ以上である。し
かしながら、あまり巾が広い場合には、電極の凹凸によ
る均一成膜の効果が小さ(なり好ましいものではない。On the other hand, the width W of the ridges in the unevenness of the high-frequency applying electrode as shown in FIGS. 1 and 2, that is, the width of the convex portion, is 172 or more of the electrode spacing d, preferably the same as or more than d. However, if the width is too wide, the effect of uniform film formation due to the unevenness of the electrode is small (which is not preferable).
薄膜の均一性は高周波印加電極と接地電極との間隔や高
周波印加電極と基板との間隔等の装置形状によっても影
響されるが、高周波印加電極の山の巾Wを5cm以下と
することにより、これらの装置形状による影響はほとん
ど無くすことが可能である。さらに、この場合も高周波
印加電極と接地電極および基板等との間隔はと(に限定
されるものではない。The uniformity of the thin film is also affected by the shape of the device, such as the distance between the high frequency application electrode and the ground electrode and the distance between the high frequency application electrode and the substrate, but by setting the width W of the peak of the high frequency application electrode to 5 cm or less, It is possible to almost eliminate the influence of these device shapes. Furthermore, in this case as well, the distance between the high frequency application electrode, the ground electrode, the substrate, etc. is not limited to ().
さらに、第1図、第2図に示すような、高周波印加電極
の凹凸における谷の巾りは、5IIII11以上で、好
ましくはdと同じかそれ以上である。この場合もしかあ
まり広いと電極表面を凹凸状に形成したことによる均一
成膜の効果は小さ(なり、5cm以下であることが好ま
しい。Furthermore, the width of the valley in the unevenness of the high frequency application electrode as shown in FIGS. 1 and 2 is 5III11 or more, preferably the same as d or more. In this case, if the electrode surface is too wide, the effect of uniform film formation by forming the electrode surface in an uneven shape will be small (the width is preferably 5 cm or less).
本発明において、凹凸形状の高周波印加電極にアースシ
ールド5.5′を設備することは必須の条件ではないが
、高周波印加電極にアースシール−ドを設備することに
より、放電を有効に対向する接地電極側に方向づけるこ
とができる。このために、アースシールドを形成できる
間隔をとることが好ましい。具体的な示例としては、5
+a+m以上の間隔が存在すれば十分である。第1図に
異体的な示例を示した。In the present invention, although it is not an essential condition to provide the earth shield 5.5' to the irregularly shaped high frequency application electrode, by providing the earth shield to the high frequency application electrode, it is possible to effectively prevent the discharge from being grounded. It can be oriented towards the electrode side. For this reason, it is preferable to provide a spacing that allows formation of an earth shield. As a specific example, 5
It is sufficient if there is an interval of +a+m or more. Fig. 1 shows a different example.
これら高周波印加電極や接地電極等の材質については、
とくに制限されるものではないが、形成される半導体薄
膜に与える不純物量、電気伝導性、熱的安定性等を考慮
するとステンレス鋼である5US316や5US304
やアルミニウムが好ましい材料として用いられる。Regarding the materials of these high frequency application electrodes and grounding electrodes,
Although not particularly limited, considering the amount of impurities imparted to the formed semiconductor thin film, electrical conductivity, thermal stability, etc., stainless steels such as 5US316 and 5US304 may be used.
and aluminum are used as preferred materials.
本発明のインライン成膜装置とは、上記したごとく、真
空を破ることな(基板を成膜室に搬送することのできる
、基板導入室および基板取り出し室、または基板取り出
し室を兼ねる基板導入室、またはこれらの機能を果たす
基板導入手段や基板取り出し手段を少なくとも有する成
膜装置であり、基板は成膜室内に設置され、もしくは室
内を移動しながら半導体薄膜が形成される装置である。As described above, the in-line film forming apparatus of the present invention includes a substrate introducing chamber and a substrate unloading chamber, or a substrate introducing chamber that also serves as a substrate unloading chamber, in which the substrate can be transferred to the film forming chamber without breaking the vacuum. Alternatively, it is a film forming apparatus that has at least a substrate introduction means and a substrate ejection means that perform these functions, and a semiconductor thin film is formed on the substrate while the substrate is installed in a film forming chamber or moved within the chamber.
成膜室は反応ガス導入手段および排気手段を備えた金属
製の反応容器であり、少なくとも基板を加熱するための
加熱手段、高密度のプラズマを発生するための中挟の高
周波印加電極および接地電極、基板保持具(基板キャリ
ヤー)を移動させるための搬送手段が設備されているも
のである。なお、基板保持具とは、半導体薄膜が形成さ
れる基板を、はめ込み、設置等により固定して搬送する
ための搬送具である。従って、基板の主面が露出してお
り、この面上に薄膜が形成されうるちのである限り、基
板の基板キャリアへの設置方法については、何ら限定さ
れるものはない。通常、基板保持具は、基板と路間−の
大きさか、これよりやや大きいのが普通である。基板保
持具上に保持された基板は、高周波印加電極と接地電極
の間に発生する高周波プラズマ中を、高周波印加電極お
よび対向する接地電極とに対して垂直方向に設置され、
もしくは該方向に進行し、半導体薄膜等が移動中の基板
上に形成されるのである。The film forming chamber is a metal reaction vessel equipped with a reaction gas introduction means and an exhaust means, and at least a heating means for heating the substrate, an intermediate high frequency application electrode for generating high-density plasma, and a ground electrode. , a transport means for moving the substrate holder (substrate carrier) is provided. Note that the substrate holder is a transport tool for transporting a substrate on which a semiconductor thin film is formed while fixing it by fitting, installing, or the like. Therefore, as long as the main surface of the substrate is exposed and a thin film can be formed on this surface, there are no limitations on the method of installing the substrate on the substrate carrier. Normally, the substrate holder is the same size as the substrate and the path, or slightly larger than this. The substrate held on the substrate holder is placed in a direction perpendicular to the high frequency application electrode and the opposing ground electrode in a high frequency plasma generated between the high frequency application electrode and the ground electrode,
Alternatively, it moves in that direction, and a semiconductor thin film or the like is formed on the moving substrate.
反応容器の材質は限定されるものではないが、好ましい
材質としてはステンレススチール、ニッケルおよびその
合金、アルミニウムおよびその合金などである。加工性
や耐蝕性を考慮した取扱い上からはス−r 71/ ス
、!、 チール(SUS316.5US304 )ある
いはアルミニウムおよびその合金が好ましいものである
。The material of the reaction vessel is not limited, but preferred materials include stainless steel, nickel and its alloys, aluminum and its alloys. From the viewpoint of handling considering workability and corrosion resistance, it is very easy! , steel (SUS316.5US304) or aluminum and its alloys are preferred.
本発明において、基板の材質は限定されるものではない
、ガラス基板、酸化スズや酸化スズ・インジウムの様な
透明導電膜付きガラス基板、セラミックス基板、アルミ
ニウム、クロム、ステンレス(sus316,5US3
04 )などの金属薄板やアルミニウム、クロム、ステ
ンレス(SIIS316.5tlS304 )などの金
属を蒸着したセラミックス基板やポリエチレンテレフタ
レートなどの高分子基板、ステンレス基板、多結晶およ
び単結晶シリコンウェハーなどが基板として有効に用い
られる。In the present invention, the material of the substrate is not limited to a glass substrate, a glass substrate with a transparent conductive film such as tin oxide or tin oxide/indium, a ceramic substrate, aluminum, chromium, stainless steel (sus316, 5US3
Metal thin plates such as 04), ceramic substrates with metals such as aluminum, chromium, and stainless steel (SIIS316.5tlS304) vapor-deposited, polymer substrates such as polyethylene terephthalate, stainless steel substrates, and polycrystalline and single-crystalline silicon wafers are effective substrates. used.
本発明で用いる反応性ガスは、主にシリコン化合物ガス
であり、一般式51hHzn*z (ここでnは自然
数)で示されるシラン、例えばモノシラン、ジシランで
ある。さらに、一般式SiH+cF<−x (χは、0
〜4の整数)で示されるフルオロシラン、一般弐〇〇、
FIzn*t (nは、自然数)で示される水素化ゲ
ルマンなどである。また、目的に応じて、フォスフイン
PHx 、ジボランBJh、ヘリウムHe1炭化水素ガ
ス CyHzy*z 、CyHzy −CyHzy〜2
(yは、自然数)、モノメチルシランなどの有機けい素
ガスなどを単独ないし混合して用いることができる。The reactive gas used in the present invention is mainly a silicon compound gas, and is a silane represented by the general formula 51hHzn*z (where n is a natural number), such as monosilane and disilane. Furthermore, the general formula SiH+cF<-x (χ is 0
Fluorosilane represented by an integer of ~4), general 2〇〇,
Examples include hydrogenated germane represented by FIzn*t (n is a natural number). Depending on the purpose, phosphine PHx, diborane BJh, helium He1 hydrocarbon gas CyHzy*z, CyHzy -CyHzy~2
(y is a natural number), organic silicon gas such as monomethylsilane, etc. can be used alone or in combination.
[実施例]
まず、基板挿入室に基板保持具を設置し、真空系で0.
01torr以下に排気しつつ、加熱手段で基板を所定
の温度になるまで加熱する。所定の圧力並びに基板温度
に達した後、第1図に示される形状の凹凸状の高周波印
加電i(h =20mm 、 w=20mm。[Example] First, a substrate holder is installed in the substrate insertion chamber, and the temperature is set to 0.
The substrate is heated by a heating means until it reaches a predetermined temperature while exhausting to a temperature of 0.01 torr or less. After reaching the predetermined pressure and substrate temperature, a high-frequency electric current i (h = 20 mm, w = 20 mm) is applied to the uneven shape shown in FIG.
し・201)を用い、ジシランの放電を発生させている
反応室内に基板保持具に保持せしめて搬送し、接地電極
に固定した後アモルファスシリコン薄膜を成膜した。201), the substrate was transported while being held in a substrate holder into a reaction chamber in which disilane discharge was being generated, and after being fixed to a ground electrode, an amorphous silicon thin film was formed.
底腹条止;
ジシラン 10 cc/min
高周波電力 5〇一
基板温度 250 ’C
反応圧力 Q、l torr
電極寸法 100■ φ
基板寸法 20傘80111I11
底1級果;
平均成膜速度 25 A/see基板上の成膜速
度分布(第4図) ±5χ代表的な光転導度 3.5
傘10−’ S/cm代表的な暗転導度 4.6傘1
0−” S/cm〔比較例〕
成膜条件を実施例と同条件にして電極のみを通常の平衡
平板型高周波印加電極を用いて成膜した結果、
成膜速度はIIA/sec 〜27A/seeの間で変
化し、均一成膜が極めて困難であるを確認した。Disilane 10 cc/min High frequency power 5〇1 Substrate temperature 250'C Reaction pressure Q, l torr Electrode dimensions 100 ■ φ Substrate dimensions 20 umbrellas 80111I11 Bottom 1st grade; Average film formation rate 25 A/see substrate Film formation rate distribution above (Figure 4) ±5χ Typical optical conductivity 3.5
Umbrella 10-' S/cm Typical dark conductivity 4.6 Umbrella 1
0-” S/cm [Comparative Example] As a result of forming a film under the same film forming conditions as in the example and using only the electrode as a normal balanced plate type high frequency application electrode, the film forming rate was IIA/sec to 27 A/sec. It was confirmed that uniform film formation was extremely difficult.
[発明の効果]
以上のごとく、本発明においては、本発明で規定する特
定の表面に凹凸を形成した高周波印加電極を用いること
により、高成膜速度で大面積の基板上に均質に成膜する
ことができる。得られた薄膜の特性は優れたものであり
、本発明の産業上の利用可能性は、極めて大きいもので
ある。[Effects of the Invention] As described above, in the present invention, a film can be formed uniformly on a large-area substrate at a high film-forming rate by using a high-frequency application electrode with irregularities formed on the specific surface defined by the present invention. can do. The properties of the obtained thin film are excellent, and the industrial applicability of the present invention is extremely large.
第1図は、表面を凹凸状に形勢した高周波印加電極を有
する反応室の模式的な断面図であり、第2図はおなしく
その斜視図である。
第3図は、断面が矩形である高周波印可電極の凹凸形状
および配置の実施の態様の例を示す説明図である。第4
図は実施例において成膜速度分布を計測した基板上の位
置を示す説明図である。長方形の中心を通り長辺と平行
に5111In間隔で測定点を設けた。
図において、1−・−一一−−−−−−−高周波印加電
極、2−−−−−−−・・−・−接地電極、3.3″・
・−・−・−・−ヒーター、4−・・−・−・−・一基
板、5.5′・・−・−・・−・・アースシールド、h
−・−−−−−一・・・−・−凹凸における山の高さ、
w −−−−−−−−−・−・−凹凸における山の巾、
L −−−−−−−・−−−m−−−・凹凸における谷
の巾FIG. 1 is a schematic cross-sectional view of a reaction chamber having a high-frequency application electrode with an uneven surface, and FIG. 2 is a perspective view thereof. FIG. 3 is an explanatory diagram showing an example of an embodiment of the uneven shape and arrangement of a high frequency application electrode having a rectangular cross section. Fourth
The figure is an explanatory diagram showing the positions on the substrate where the film deposition rate distribution was measured in the example. Measurement points were provided at intervals of 5111 inches passing through the center of the rectangle and parallel to the long sides. In the figure, 1-.
・−・−・−・−Heater, 4−・・−・−・−・One board, 5.5′・・−・−・・−・・Earth shield, h
−・−−−−−1・−・−Height of the mountain in unevenness,
w −−−−−−−−−・−・−Width of the mountain in unevenness,
L ----------・---m---・Width of valley in unevenness
Claims (1)
放電中に、基板を設置・もしくは進行せしめて該基板上
に薄膜を形成するインライン成膜装置において、該高周
波印加電極表面が凹凸状に形成されていることを特徴と
する成膜装置。(1) In an in-line film forming apparatus that places or advances a substrate to form a thin film on the substrate during glow discharge that occurs between a high-frequency applying electrode and a grounded electrode, the surface of the high-frequency applying electrode is uneven. A film forming apparatus characterized in that:
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62256403A JP2601488B2 (en) | 1987-10-13 | 1987-10-13 | Film forming equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62256403A JP2601488B2 (en) | 1987-10-13 | 1987-10-13 | Film forming equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0199213A true JPH0199213A (en) | 1989-04-18 |
| JP2601488B2 JP2601488B2 (en) | 1997-04-16 |
Family
ID=17292192
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62256403A Expired - Fee Related JP2601488B2 (en) | 1987-10-13 | 1987-10-13 | Film forming equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2601488B2 (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0395630U (en) * | 1990-01-11 | 1991-09-30 | ||
| JP2001181848A (en) * | 1999-12-20 | 2001-07-03 | Anelva Corp | Plasma processing equipment |
Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5374372A (en) * | 1976-12-15 | 1978-07-01 | Hitachi Ltd | Plasma cvd device |
| JPS59125615A (en) * | 1982-12-28 | 1984-07-20 | Fujitsu Ltd | Manufacture of semiconductor device |
| JPS6075460U (en) * | 1983-10-28 | 1985-05-27 | 富士通株式会社 | Plasma vapor phase growth equipment |
| JPS60128613A (en) * | 1983-12-15 | 1985-07-09 | Ricoh Co Ltd | Plasma cvd apparatus |
| JPS61267315A (en) * | 1985-05-22 | 1986-11-26 | Anelva Corp | Plasma cvd device |
| JPS62282434A (en) * | 1986-03-04 | 1987-12-08 | ライボルト−ヘレ−ウス・ゲゼルシヤフト・ミツト・ベシユレンクテル・ハフツング | Apparatus for subjecting substrate to plasma treatment in plasma discharge excited by radio frequency excitation |
-
1987
- 1987-10-13 JP JP62256403A patent/JP2601488B2/en not_active Expired - Fee Related
Patent Citations (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS5374372A (en) * | 1976-12-15 | 1978-07-01 | Hitachi Ltd | Plasma cvd device |
| JPS59125615A (en) * | 1982-12-28 | 1984-07-20 | Fujitsu Ltd | Manufacture of semiconductor device |
| JPS6075460U (en) * | 1983-10-28 | 1985-05-27 | 富士通株式会社 | Plasma vapor phase growth equipment |
| JPS60128613A (en) * | 1983-12-15 | 1985-07-09 | Ricoh Co Ltd | Plasma cvd apparatus |
| JPS61267315A (en) * | 1985-05-22 | 1986-11-26 | Anelva Corp | Plasma cvd device |
| JPS62282434A (en) * | 1986-03-04 | 1987-12-08 | ライボルト−ヘレ−ウス・ゲゼルシヤフト・ミツト・ベシユレンクテル・ハフツング | Apparatus for subjecting substrate to plasma treatment in plasma discharge excited by radio frequency excitation |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPH0395630U (en) * | 1990-01-11 | 1991-09-30 | ||
| JP2001181848A (en) * | 1999-12-20 | 2001-07-03 | Anelva Corp | Plasma processing equipment |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2601488B2 (en) | 1997-04-16 |
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| LAPS | Cancellation because of no payment of annual fees |