JPH0227775A - Manufacture of solar cell - Google Patents
Manufacture of solar cellInfo
- Publication number
- JPH0227775A JPH0227775A JP63176939A JP17693988A JPH0227775A JP H0227775 A JPH0227775 A JP H0227775A JP 63176939 A JP63176939 A JP 63176939A JP 17693988 A JP17693988 A JP 17693988A JP H0227775 A JPH0227775 A JP H0227775A
- Authority
- JP
- Japan
- Prior art keywords
- substrate
- reaction chamber
- layer
- electric field
- amorphous semiconductor
- 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
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)
Abstract
Description
【発明の詳細な説明】
く技術分野〉
本発明は、化学的気相分解により非晶質半導体層を形成
する所定数の反応室のプラズマ雰囲気中を通って基板を
搬送し、該基板上に順次所定の導電型の非晶質半導体層
を成膜して、010等所定構造の光起電力層を形成する
ようにした太陽電池の製造装置に関する。DETAILED DESCRIPTION OF THE INVENTION [Technical Field] The present invention involves transporting a substrate through a plasma atmosphere of a predetermined number of reaction chambers in which an amorphous semiconductor layer is formed by chemical vapor phase decomposition; The present invention relates to a solar cell manufacturing apparatus that sequentially forms amorphous semiconductor layers of a predetermined conductivity type to form a photovoltaic layer having a predetermined structure such as 010.
〈従来技術〉
化学的気相分解(CVD)によるプラズマ雰囲気中で基
板上に薄膜半導体層等を成膜して半導体装置等を製造す
るプラズマ気相成長装置は、例えばシラン(Si H4
)ガスを放電分解して非晶質シリコン太陽電池を製造す
る方法として広く実用化された公知の技術である。<Prior art> A plasma vapor deposition apparatus for manufacturing semiconductor devices by forming a thin film semiconductor layer on a substrate in a plasma atmosphere using chemical vapor decomposition (CVD) uses, for example, silane (SiH4).
) This is a well-known technique that has been widely put into practical use as a method for manufacturing amorphous silicon solar cells by discharging gas.
かかる製造方法において、効率よく非晶質シリコン薄膜
半導体層を成膜するものとして、特開昭58−2164
75号公報、特面昭59−34668号公報等で公知の
プラズマcvo装置を用いてロール・ツ・ロール方式に
より搬送する基板上に連続的に非晶質シリコンIIIの
成膜を行うことが知られている。In such a manufacturing method, a method for efficiently forming an amorphous silicon thin film semiconductor layer is disclosed in Japanese Patent Application Laid-Open No. 58-2164.
It has been known from Japanese Patent No. 75, Special Publication No. 59-34668, etc. that amorphous silicon III can be continuously formed on a substrate transported by a roll-to-roll method using a known plasma CVO device. It is being
この方式で非晶質シリコン太陽電池を作成する場合は少
なくともp、i、nの非晶質シリコンあるいは微結晶化
非晶質シリコンをそれぞれ独立の反応室で成膜する為複
数の専用反応室を連結して反応室ごとに反応ガスを変え
て成膜し、順次基板を移送させる方法が行われている。When creating an amorphous silicon solar cell using this method, multiple dedicated reaction chambers are required to form at least p, i, and n amorphous silicon or microcrystalline amorphous silicon in independent reaction chambers. A method is used in which the reaction chambers are connected to form a film using a different reaction gas in each reaction chamber, and the substrates are sequentially transferred.
これは単一の反応室内ではプラズマ雰囲気中のガス組成
は空間的にほぼ均一であり、反応室内に組成の異なった
ガス雰囲気を適当に分布させることができないためであ
る。This is because the gas composition in the plasma atmosphere is spatially substantially uniform within a single reaction chamber, and gas atmospheres having different compositions cannot be appropriately distributed within the reaction chamber.
ところで、かかる複数の反応室間′C艮尺の可撓性基板
を連続搬送するロール・ツ・ロール方式においては、各
反応室は完全に分離・独立している訳ではなく、基板の
通路で連結されている。このため、隣接した反応室間で
該基板通路を経由して各反応室の反応ガスの相互混合を
さけることができない。この相互混合が作成しようとす
る非晶質シリコン太陽電池の特性を劣化させる場合には
反応室間の基板通路に一方向性のガスの流れを形成した
り、特開昭58−216475号公報、特開昭5934
668号公報等に開示の如く、反応室間に専用のmm室
を設けて油気又は差動排気して必要な程度迄ガス分離を
行っていた。しかし、かかる従来方法ではひとたびこれ
らガス分離機構を越えて侵入した隣接反応室の反応ガス
は反応室全域に拡散して反応室内で均一となり、非晶質
シリコン太陽電池の特性向上に有効な隣接層との界面の
膜厚方向の組成分布や不純物分布のプロファイルの制御
性、例えばゆるやかな傾斜接合にするか、シャープな階
段接合にするかと云った制御性にとぼしかった。By the way, in the roll-to-roll method in which flexible substrates of approximately C length are continuously conveyed between a plurality of reaction chambers, each reaction chamber is not completely separated and independent; connected. Therefore, it is impossible to avoid mutual mixing of the reaction gases in the reaction chambers between adjacent reaction chambers via the substrate passage. If this mutual mixing deteriorates the characteristics of the amorphous silicon solar cell to be produced, a unidirectional gas flow may be formed in the substrate passage between the reaction chambers, or Japanese Patent Publication No. 5934
As disclosed in Japanese Patent No. 668, etc., a dedicated mm chamber was provided between the reaction chambers, and oil or gas was differentially pumped out to perform gas separation to the extent necessary. However, in such conventional methods, once the reaction gas from the adjacent reaction chamber has penetrated beyond these gas separation mechanisms, it is diffused throughout the reaction chamber and becomes uniform within the reaction chamber. The controllability of the composition distribution and impurity distribution profile in the film thickness direction at the interface with the film, such as whether to form a gentle sloped junction or a sharp stepped junction, was poor.
さらに、非晶質シリコン太陽電池の特性向上において、
少なくとも太陽光入射ip層あるいは0層は100A
IFi後と極めて薄い微結晶化シリコン層を均一にf[
する必要があることが知られてきた。Furthermore, in improving the characteristics of amorphous silicon solar cells,
At least the sunlight incident IP layer or 0 layer is 100A
After IFi, the extremely thin microcrystalline silicon layer is uniformly f[
It has become known that it is necessary to
ところで、これらの微結晶化シリコン簿膜を前述のロー
ル・ツ・ロール方式で堆積する場合、その+1#!の膜
質及びII厚調整を行う為に、一般にはマスクを設け、
基板面に達するブラズ7mをその開口部幅によって調整
し、堆積膜質及びII厚を制御しCいる。又、所定のパ
ターンに形成するためにもマスクが用いられている。By the way, when depositing these microcrystalline silicon films by the roll-to-roll method described above, the +1#! In order to adjust the film quality and II thickness, a mask is generally provided.
The plasma 7m reaching the substrate surface is adjusted by its opening width to control the deposited film quality and II thickness. A mask is also used to form a predetermined pattern.
しかしながら、このように基板と放電電極との間にマス
クが設置されたプラズマCVD装置を用い、微結晶化非
晶質シリコン膜を成膜したところ、マスクの開口エッヂ
部に近い部分では微結晶化しているが、中央部に近づく
に従って徐々に導電率が低下し、ついにはアモルファス
膜のままで微結晶化がおこらないことが確認された。However, when a microcrystalline amorphous silicon film was formed using a plasma CVD apparatus in which a mask was installed between the substrate and the discharge electrode, microcrystalization occurred in the areas near the opening edges of the mask. However, the conductivity gradually decreased as it approached the center, and it was confirmed that the film remained amorphous and no microcrystallization occurred.
すなわち、マスク設置によりマスク開口部の中央部具体
的には基板中央部とマスク開口部のエツジに近い部分す
なわち基板両端部では得られる膜質が大きく変化する問
題が生じることを見出した。That is, it has been found that, due to mask installation, the quality of the film obtained changes significantly at the center of the mask opening, specifically, at the center of the substrate, and at the edges of the mask opening, that is, at both ends of the substrate.
以上に述べた様にロール・ツ・ロール法を用いて^性能
な非晶質シリコン太陽電池を能率よく作成する為には上
述の問題点を解決しなければならない。As described above, in order to efficiently produce a high-performance amorphous silicon solar cell using the roll-to-roll method, the above-mentioned problems must be solved.
〈発明の目的〉
本発明はかかる現状に鑑みなされたもので、1層形成に
おいて隣接半導体層との界面急峻性を制御し、nつ層内
でも組成や不純物分布に所望のデプスプロファイルをも
たせることを可能とすると共に、微結晶化半導体層の形
成において、膜質膜厚の分布なく均一な膜形成を可能と
する通産に適した太陽電池の製造装置を提供することを
目的とする。<Objective of the Invention> The present invention was made in view of the current situation, and it is an object of the present invention to control the steepness of the interface with an adjacent semiconductor layer in the formation of one layer, and to provide a desired depth profile in composition and impurity distribution even within n layers. It is an object of the present invention to provide a solar cell manufacturing apparatus suitable for industrial use, which enables uniform film formation without distribution of film quality and thickness in the formation of a microcrystalline semiconductor layer.
〈発明の構成〉 上述の目的は以下の本発明によって達成される。<Structure of the invention> The above objects are achieved by the invention as follows.
すなわち、本発明は、基板がその放電電極間を通って搬
送できるように連結された化学的気相分解法により所定
の非晶質半導体膜を形成する所定数の反応室を備え、該
基板を各反応室を通して搬送し、該基板上に少なくとも
一層の微結晶化非晶質半導体層とi型非晶質半導体層と
を有する光起電力層を形成するようになした太陽電池の
製造装置において、反応ガスを遮断する仕切板を基板搬
送方向に所定間隔で放電電極面に垂直方向に配設して、
少なくともプラズマ雰囲気を基板通路等の限られた隙間
を除いて基板搬送方向にガス拡散のない複数の区域に区
画した、前記i型非晶質半導体層を形成するi層反応室
と、基板と放電N極との間にマスクを配置すると共にそ
の開口部に開口部の電界分布を調節するための電界調整
部材を設けた前記微結晶化非晶質半導体層を形成する微
結晶化反応室とを具備したことを特徴とする太陽電池の
製造装置である。That is, the present invention comprises a predetermined number of reaction chambers for forming a predetermined amorphous semiconductor film by chemical vapor phase decomposition, which are connected so that the substrate can be transported between the discharge electrodes, In a solar cell manufacturing apparatus, the photovoltaic layer is transported through each reaction chamber to form a photovoltaic layer having at least one microcrystallized amorphous semiconductor layer and an i-type amorphous semiconductor layer on the substrate. , partition plates for blocking reaction gas are arranged perpendicularly to the discharge electrode surface at predetermined intervals in the substrate transport direction,
an i-layer reaction chamber in which the i-type amorphous semiconductor layer is formed, and an i-layer reaction chamber in which the plasma atmosphere is divided into a plurality of zones in which gas is not diffused in the substrate transport direction except for limited gaps such as substrate passages; a microcrystallization reaction chamber for forming the microcrystallized amorphous semiconductor layer, in which a mask is disposed between the N pole and an electric field adjustment member is provided in the opening for adjusting the electric field distribution in the opening; This is a solar cell manufacturing apparatus characterized by comprising:
上述の本発明において、基板を合成樹脂フィルム等の長
尺の可撓性帯状基板とし、前記連結された反応室の前後
に巻出室と巻取室とを連結し、該基板をロール・ツ・ロ
ールで搬送しつつ各非晶質半導体薄膜を基板上に形成す
るようにした構成により、特に量産に適した生産性の良
い太陽電池の製造装置が得られる。In the above-described present invention, the substrate is a long flexible strip substrate such as a synthetic resin film, an unwinding chamber and a winding chamber are connected before and after the connected reaction chamber, and the substrate is rolled. - With the configuration in which each amorphous semiconductor thin film is formed on a substrate while being transported by rolls, a solar cell manufacturing apparatus with high productivity particularly suitable for mass production can be obtained.
以下本発明の詳細な説明する。The present invention will be explained in detail below.
まず、本発明のi層反応室について説明する。First, the i-layer reaction chamber of the present invention will be explained.
i層反応室の構成は以下のようにして得られたものであ
る。The configuration of the i-layer reaction chamber was obtained as follows.
すなわち、放電電極間に垂直にガスを遮断する仕切板を
設けてプラズマ雰囲気を区画してもプラズマ放電は影響
されず安定製膜ができることを見出すと共に、ガスを遮
断できる仕切板により区画されたプラズマ雰囲気の各区
域間の反応ガスの流路を基板表面近傍等に限定すること
により、ガス導入口と排気口の基板搬送方向の位置によ
り基板搬送方向のガス組成分布を制御できることを見出
しなされたものである。In other words, we found that even if a partition plate that blocks gas is provided vertically between the discharge electrodes to partition the plasma atmosphere, the plasma discharge is not affected and stable film formation can be achieved. It was discovered that the gas composition distribution in the substrate transport direction can be controlled by the position of the gas inlet and exhaust port in the substrate transport direction by limiting the flow path of the reaction gas between each area of the atmosphere to the vicinity of the substrate surface. It is.
なお、この理由は前記仕切板により区画されたプラズマ
雰囲気の各区域間の基板搬送方向のガスの相互拡散が限
定され、各区域のガス組成は略独立したものとなるため
と思われる。The reason for this is believed to be that mutual diffusion of gas in the substrate transport direction between the zones of the plasma atmosphere divided by the partition plates is limited, and the gas compositions of each zone become substantially independent.
従って、本発明の仕切板はガスを遮断できるものであれ
ば良く、その材質は特に限定されないが、中でもプラズ
マ損傷のないものが好ましく、ステンレス等が使用され
る。なお、仕切板は反応室と共に接地するのが一般であ
るが、浮遊もしくは適当なバイアス電圧を印加させても
良い。そしてその形状は、基板搬送方向のガスの拡散が
無視できるものであれば良く1通常は基板搬送路及び6
1B4fffi面との間に微小な間隙を有するのみで、
その他の部分は完全に遮断し、前記間隔以外ではガス移
動のない形状が選定される。このようにすると間隙部で
ガス流速が大となり、ガス拡散の防止がより完全となる
点で好ましい。しかし、反応室内の部材の配置によりガ
ス流路が限定される場合には該ガス流路を遮断するよう
に仕切板は設置すれば良いことは云うまでもない。なお
、仕切板は少なくとも基板前面との間にガス流路となる
スリットを有する必要がある。Therefore, the partition plate of the present invention may be any material as long as it can block gas, and its material is not particularly limited, but it is preferably one that is free from plasma damage, such as stainless steel. Although the partition plate is generally grounded together with the reaction chamber, it may be floating or a suitable bias voltage may be applied thereto. The shape may be such that the diffusion of gas in the substrate transport direction can be ignored (1) Usually, the substrate transport path and 6
There is only a small gap between the 1B4fffi surface,
The other parts are completely blocked off, and a shape is selected in which there is no gas movement outside the above-mentioned interval. This is preferable because the gas flow rate increases in the gap and gas diffusion is more completely prevented. However, if the gas flow path is limited due to the arrangement of members within the reaction chamber, it goes without saying that a partition plate may be installed to block the gas flow path. Note that the partition plate needs to have at least a slit between it and the front surface of the substrate to serve as a gas flow path.
又仕切板の数及びその間隙は、形成する膜の膜厚方向の
プロファイルに応じて選定される。この選定は実験によ
る。Further, the number of partition plates and the gap between them are selected depending on the profile of the film to be formed in the film thickness direction. This selection is based on experimentation.
一方反応ガスの導入口、排気口の配置も、同様に形成す
る膜厚方向のプロファイルに応じて実験により選定され
る。例えば膜内の組成を変化させたい場合は夫々の反応
ガスの導入口を反応室の基板搬送方向の両端部に配置し
、その一端に共通の排気口を設けること等により適当な
勾配の組成分布を得ることができる。On the other hand, the arrangement of the reactant gas inlet and exhaust port is similarly selected through experiments according to the profile in the thickness direction of the film to be formed. For example, if you want to change the composition within the film, you can create a composition distribution with an appropriate gradient by arranging the inlets for each reaction gas at both ends of the reaction chamber in the substrate transport direction, and providing a common exhaust port at one end. can be obtained.
次に本発明のもう一つの要件である微結晶化反応室につ
いて説明する。Next, the microcrystallization reaction chamber, which is another requirement of the present invention, will be explained.
微結晶化反応室の構成は以下のようにしてなされたもの
である。すなわち、前述のマスクによる膜質変化の原因
を検討したところ、マスクの開口エッヂ部に電界の集中
が生じ、基板とマスク間口エッヂ部との間に局部放電が
発生して強いプラズマが生じ、一方これによって基板中
央部の電界強度が弱められることが原因と判明した。The microcrystallization reaction chamber was constructed as follows. In other words, when we investigated the cause of film quality change due to the mask mentioned above, we found that the electric field concentrates at the edge of the opening of the mask, and a local discharge occurs between the substrate and the edge of the mask, generating strong plasma. The cause was found to be that the electric field strength at the center of the substrate was weakened by
そこで、該マスク開口エッヂ部での電界集中を緩和する
ため、エッチ周辺部を等電位面に沿ったものに近い形に
丸める、マスクを極力基板に近づける、印加パワーをな
るべく抑える等種々の方法を検討したが大きな効果を得
られなかった。そして、電極と基板の間に設置されたマ
スクの開口中央部に、電界が集中するような電界調整部
材を設け、マスクの開口部の電界分布を均一化すること
により解決することを見出し前記構成に想到したもので
ある。Therefore, in order to alleviate the electric field concentration at the edge of the mask opening, various methods have been used, such as rounding the etch periphery to a shape similar to that along an equipotential surface, moving the mask as close to the substrate as possible, and suppressing the applied power as much as possible. I tried it, but it didn't have a big effect. Then, they found that the above structure can be solved by providing an electric field adjustment member that concentrates the electric field in the center of the opening of the mask installed between the electrode and the substrate, and uniformizing the electric field distribution in the opening of the mask. This is what I came up with.
従って、本発明のマスクの開口部に設ける電界調整部材
は開口部の機能を損わない範囲で、開口部の電界分布を
均一化できるものであれば特に限定されないが、膜厚分
布等への影響がなく効果的に電界分布を調整できる点か
ら線状材が好ましい。Therefore, the electric field adjusting member provided in the opening of the mask of the present invention is not particularly limited as long as it can uniformize the electric field distribution in the opening without impairing the function of the opening. A wire material is preferable since the electric field distribution can be effectively adjusted without any influence.
そして線材の配置は、単なる間口部の中央配置、あるい
は適当な間隔の平行配置、格子状配置、更には同心円状
配置等開口部の大きさ、形状に応じて実験的に選定する
のが好ましい。又その材質は、RFM電中で゛電界を集
中させることができ、開口部の電界分布を調整できるも
のなら如何なる物質でもよいが、好ましくは加工性のよ
い導電性物質がよく、更に好ましくは放電中膜ガスが少
ない金属が好ましく、ステンレス、タングステン、チタ
ン、モリブデン等の対プラズマ耐性のある金属材料の中
から選択される。The arrangement of the wire rods is preferably selected experimentally depending on the size and shape of the opening, such as simple arrangement in the center of the opening, parallel arrangement at appropriate intervals, lattice arrangement, or even concentric arrangement. The material may be any material as long as it can concentrate the electric field in RFM and adjust the electric field distribution in the opening, but it is preferably a conductive material with good workability, and more preferably a conductive material with good workability. A metal with a small amount of film gas is preferable, and is selected from metal materials resistant to plasma such as stainless steel, tungsten, titanium, and molybdenum.
なお、良好な微結晶化非晶質半導体膜を得る為には、基
板表面に印加されるパワーがいかなる箇所においても少
なくとも5 mW/d以上必要であるのでこの条件を満
すために好ましくは直径0.5〜21111.、更に好
ましくは直径1〜1,5#lI程度の線状材(単線でも
撚線でも良い)で電界調整部材を構成することが望まし
い。Note that in order to obtain a good microcrystalline amorphous semiconductor film, the power applied to the substrate surface must be at least 5 mW/d or more at any point, so in order to satisfy this condition, it is preferable to 0.5-21111. More preferably, it is desirable to construct the electric field adjusting member with a wire material (either a single wire or a stranded wire) having a diameter of about 1 to 1.5 #lI.
又、その電界強度の調整は、電界調整部材と基板との距
離で自由に調整できる。Further, the electric field strength can be freely adjusted by changing the distance between the electric field adjusting member and the substrate.
本発明の適用できる放電電極の形状は、平行平板型、キ
ャンを用いた平行曲面型はもちろんのこと、非平行な電
極においても電界調整部材の形状。The shape of the discharge electrode to which the present invention can be applied is not only a parallel plate type and a parallel curved type using a can, but also the shape of the electric field adjustment member in non-parallel electrodes.
位置、材質等を変えることによって不平等電界の緩和が
でき、適用できる。By changing the position, material, etc., the unequal electric field can be alleviated and applied.
以上本発明の特徴要件であるi層反応室及び微結晶化反
応室について説明した。The i-layer reaction chamber and the microcrystallization reaction chamber, which are the characteristics of the present invention, have been described above.
本発明はこれらi層反応室及び微結晶化反応室を具備す
るものであるが、全体としては製造する太陽電池の光起
電力層の構成に応じて従来より公知の反応室をこれら反
応室に組み合わせるものであることは云うまでもない。The present invention is equipped with these i-layer reaction chambers and microcrystallization reaction chambers, but in general, conventionally known reaction chambers may be used in these reaction chambers depending on the configuration of the photovoltaic layer of the solar cell to be manufactured. Needless to say, they must be combined.
又必要な各反応室の数、その配列等は特に限定されず、
製造する太陽電池の光起電力層及びその形成法により決
定すべきであることは本発明の趣旨より明らかである。In addition, the number of required reaction chambers, their arrangement, etc. are not particularly limited.
It is clear from the gist of the present invention that it should be determined by the photovoltaic layer of the solar cell to be manufactured and its formation method.
更に本発明が適用できる太陽電池の構成は、少なくとも
i形の非晶質半導体層及び微結晶化半導体厨を有するも
のであればよい。代表例としては非晶質シリコン半導体
からなるpiO構成のp層あるいは0層のいずれかの層
又はこの両層を微結晶化層としたもの、あるいはこれの
タンデム構成等挙げることができるが、いずれの構成に
おいても少なくとも光入射側のp層あるいは0層を微結
晶化層とすることが太陽光の利用効率の面からは好まし
い。Further, the solar cell to which the present invention can be applied may have at least an i-type amorphous semiconductor layer and a microcrystalline semiconductor layer. Typical examples include a p-layer or a 0-layer of a piO structure made of an amorphous silicon semiconductor, or a structure in which both layers are microcrystalline layers, or a tandem structure of these. Also in the structure described above, it is preferable from the viewpoint of sunlight utilization efficiency that at least the p layer or the 0 layer on the light incidence side is a microcrystalline layer.
以上の点より本発明の好ましい基本的な態様としては、
導電形がp形又はn形の非晶質半導体層を形成する第−
層反応室と、i形の非晶質半導体層を形成するi層反応
室と、第−層反応室と逆の導電形の非晶質半導体層を形
成する微結晶化反応室を基板搬送方向にこの順序で配置
したものであり、中でも第−層反応室の前に巻出苗を、
微結晶化反応室の後に巻取室を連結してロール・ツ・ロ
ール方式により長尺の帯状基板を連続的に移送しつつ膜
形成するようにしたものが、生産性面、安定した連続膜
形成面で好ましい。From the above points, preferred basic aspects of the present invention include:
A third layer forming an amorphous semiconductor layer of p-type or n-type conductivity.
A layer reaction chamber, an i-layer reaction chamber for forming an i-type amorphous semiconductor layer, and a microcrystallization reaction chamber for forming an amorphous semiconductor layer of a conductivity type opposite to that of the -th layer reaction chamber are arranged in the substrate transport direction. The seedlings were placed in this order, and the unrolled seedlings were placed in front of the reaction chamber in the first layer.
A device that connects a winding chamber after the microcrystallization reaction chamber and forms a film while continuously transporting a long strip substrate using a roll-to-roll method is the most efficient method in terms of productivity and stable continuous film formation. Preferable in terms of formation.
以下、本発明の詳細を窓側に微結晶化n層を配したpi
0構成の非晶質シリコン太陽電池の製造に適用した実施
例に基いて説明する。The details of the present invention will be described below.
The explanation will be based on an example applied to the production of an amorphous silicon solar cell with zero configuration.
〈実施例〉 第1図は上記実施例の構成図である。<Example> FIG. 1 is a configuration diagram of the above embodiment.
その基本構成は前述の特開昭58−216475号公報
。Its basic structure is disclosed in the above-mentioned Japanese Patent Application Laid-Open No. 58-216475.
特開昭59−34668号公報開示のものと同じで、p
型。Same as that disclosed in Japanese Patent Application Laid-open No. 59-34668, p.
Type.
型及び微結晶化n (0(μC))型の各非晶質シリコ
ン層を形成するCVDプラズマ放電の第層反応室1.i
層反応室2.微結晶化反応室3及び巻出室18並びに巻
取室19を排気系(図示省略)により所定のガス圧まで
排気されるガス隔離のための緩衝室13で連結し、巻出
しロール20から巻取りロール2込1板17をロール・
ツ・ロール方式で移送しつつ、p、i、n(μC)の3
層を連続形成する構成となっている。なお、図の4〜9
は放電電極で、図の10は各放電電極に高周波電力を供
給する高周波電源具体的にはRF主電源あり、各反応室
1.2.3は夫々ガス導入口15と排気ボート16を有
し、所定のガスを導入してCVD法により所定の非晶質
半導体膜が形成できるようになっている。1. CVD plasma discharge forming amorphous silicon layer of type and microcrystallization n(0(μC)) type. i
Layer reaction chamber 2. The microcrystallization reaction chamber 3, the unwinding chamber 18, and the winding chamber 19 are connected by a buffer chamber 13 for gas isolation, which is exhausted to a predetermined gas pressure by an exhaust system (not shown), and the unwinding is carried out from the unwinding roll 20. Roll 1 plate 17 including 2 rolls.
p, i, n (μC) while transferring by two-roll method.
It has a structure in which layers are formed continuously. In addition, 4 to 9 in the figure
10 is a discharge electrode, and 10 in the figure is a high frequency power source that supplies high frequency power to each discharge electrode, specifically an RF main power source, and each reaction chamber 1.2.3 has a gas inlet 15 and an exhaust boat 16, respectively. A predetermined amorphous semiconductor film can be formed by a CVD method by introducing a predetermined gas.
ところで、i形非晶質シリコンを形成する1層反応室2
は本発明に従い以下の構成となっている。By the way, the single-layer reaction chamber 2 for forming i-type amorphous silicon
has the following configuration according to the present invention.
対向する放電電極6.7の中間のプラズマ雰囲気を基板
搬送方向に必要な通路を除いて区画する仕切板11を電
極面に垂直かつ第2図の通り隙間14を除いて反応室の
全断面を遮断するように基板の搬送方向に所定間隔にな
るように5枚設置した。従って該仕切板11によりプラ
ズマ空間は、電極間で複数の区域に区分され、反応室2
の基板搬送方向下流端に設けたガス導入口15から供給
された反応ガスはその上流端部の排気ボート16に達す
るためには必ず該仕切板11で設定された隙間14を通
って流れる。A partition plate 11 that partitions the plasma atmosphere between the facing discharge electrodes 6 and 7 in the substrate transport direction, excluding a necessary passage, is installed perpendicular to the electrode surface and covering the entire cross section of the reaction chamber, excluding the gap 14, as shown in FIG. Five boards were installed at predetermined intervals in the transport direction of the board so as to block the board. Therefore, the plasma space is divided into a plurality of areas between the electrodes by the partition plate 11, and the reaction chamber 2
The reaction gas supplied from the gas inlet 15 provided at the downstream end in the substrate transport direction always flows through the gap 14 set by the partition plate 11 in order to reach the exhaust boat 16 at the upstream end.
なお、前述の通り仕切板11は隙間14を形成するよう
に対向する放電電橋の双方に対して若干の距離を離して
設置されている。この隙間14は1つには反応ガスの通
路として、また、図で下方のパワー電147に対して電
極絶縁のため、そして図で上方のアース電極6に対して
は基板17の通路を目的としており、本実施例では3履
とした。ガス仕切板11の材料は電気的に導体、不導体
のいずれであっても本発明の目的を達するが、プラズマ
雰囲気中に不純物を放出しないことが必要である。本例
ではステンレス合金で作成し、電気的にはアースに接続
した。Note that, as described above, the partition plate 11 is installed at a certain distance from both of the opposing discharge bridges so as to form a gap 14. This gap 14 is used as a path for the reaction gas, for electrode insulation with respect to the power electrode 147 shown below in the figure, and as a passage for the substrate 17 with respect to the ground electrode 6 shown above in the figure. In this example, three shoes were used. Although the object of the present invention is achieved regardless of whether the material of the gas partition plate 11 is electrically conductive or nonconductive, it is necessary that impurities are not released into the plasma atmosphere. In this example, it was made of stainless steel and electrically connected to ground.
さらに太陽電池の窓層としてn (μC)層の微結晶化
非晶質シリコンを形成する微結晶化反応室3は本発明に
従い以下の構成となっている。すなわち、第3図にその
反応室内の側断面を示した如く、8は基板側電極でアー
スされている。17は高分子フィルム基板で矢印の方向
に移動走行する。Furthermore, the microcrystallization reaction chamber 3 for forming an n (μC) layer of microcrystalline amorphous silicon as a window layer of a solar cell has the following configuration according to the present invention. That is, as shown in FIG. 3, which shows a side cross section of the inside of the reaction chamber, 8 is grounded at the substrate side electrode. 17 is a polymer film substrate that moves in the direction of the arrow.
30は開口部(30a)を有する堆積膜厚調整用のマス
クで、本例では接地したが浮遊していても良い。Reference numeral 30 denotes a mask for adjusting the deposited film thickness having an opening (30a), which is grounded in this example, but may be floating.
なお、開口部の大きさは本例では50#lI L X
250#IIIWである。31の点線はプラズマである
。9.10は航述の通り、放電電極とそのRF主電源あ
り、よって放電周波数は公知の通り13.56 M H
zである。In addition, the size of the opening is 50 #lI L X in this example.
250#IIIW. The dotted line 31 is plasma. As mentioned above, 9.10 has a discharge electrode and its RF main power source, so the discharge frequency is 13.56 MH as well known.
It is z.
この装置を用いてまず、比較のため第4図に示された中
に前述の面積の開口部(30a)を設けた従来のマスク
で、n型微結晶化非晶質シリコン膜を作成した。(水素
+シラン+ホスフィン)混合ガスを用い、放電圧力がI
Torr 、基板温度が160℃、印加パワーが0.
05 W/CIiの条件下で、基板の走行を停止して3
0分間静止状態で形成した。その結果、マスク開口部(
30a)のエッチ部付近では、導電率が約58−CIl
−1と微結晶化していることが認められたが、中央部で
は9 x 104S−1−電とかなり高い値を示し、ア
モルファス膜のままであることが確認された。Using this apparatus, first, for comparison, an n-type microcrystalline amorphous silicon film was formed using a conventional mask shown in FIG. 4 in which an opening (30a) having the above-mentioned area was provided. (Hydrogen + silane + phosphine) mixed gas is used, and the discharge pressure is I
Torr, the substrate temperature is 160°C, and the applied power is 0.
05 Under the conditions of W/CIi, stop running the board and
It was formed in a stationary state for 0 minutes. As a result, the mask opening (
In the vicinity of the etched portion of 30a), the conductivity is approximately 58-CIl.
-1, which was observed to be microcrystalline, but the central part showed a fairly high value of 9 x 104S-1, confirming that it remained an amorphous film.
次に第5図に示す本発明の電界調整部材32として開口
部(30a)の塞板17の移送方向の中央部に基板17
の巾方向に一本の線材を設けたマスクを用いて印加パワ
ーを除いては、同じ条件で成膜を行った。ここで電界調
整部材32には1sIφのステンレス線を用いた。印加
パワーは、0.01〜0.04W/C!iと変化させて
行った。Next, as the electric field adjusting member 32 of the present invention shown in FIG.
Film formation was performed under the same conditions except for the applied power using a mask with a single wire in the width direction. Here, a stainless steel wire of 1 sIφ was used for the electric field adjustment member 32. The applied power is 0.01 to 0.04 W/C! I changed it to i.
第6図は上記条件で製膜した基板中央部の導電率を示し
たものである。この図で白丸印は光照射時、黒丸印は暗
中の測定値であり、この結果よりn型非晶質シリコンは
、中央部においても完全微結晶化がおこっていることが
確認され、且つ、開口部(30a)全面で均一な特性の
微結品化非晶質シリコン膜が得られることが確認され、
所期の特性の改善がはかられることがわかった。FIG. 6 shows the conductivity at the center of the substrate formed under the above conditions. In this figure, the white circles are the measured values during light irradiation, and the black circles are the measured values in the dark. From these results, it is confirmed that complete microcrystalization occurs even in the center of the n-type amorphous silicon, and, It was confirmed that a microcrystalline amorphous silicon film with uniform characteristics was obtained over the entire opening (30a),
It was found that the desired characteristics could be improved.
更に、印加パワーも従来のマスクを用いた場合に比し1
/2以下の低パワーの0.02W/−捏度で十分微結晶
化することも合せてliv認され、生産プロセス上有利
であることも判明した。なお、膜厚分布等は従来のマス
クと同様であり、全く問題ないことを確認した。Furthermore, the applied power is 1
It has also been confirmed that microcrystalization can be achieved sufficiently with a low power of 0.02 W/-2 or less, and it has also been found to be advantageous in terms of the production process. It was confirmed that the film thickness distribution, etc., were the same as those of conventional masks, and there were no problems at all.
一方本例のロール・ツ・ロール方式では、通常、隣接す
るp、n (μC)形非晶質シリコンを形成する第1
層反応室1と微結晶化反応室3から1層を形成する1層
反応室2へ828s及びPH3ガスが緩!i室13を経
由して微量混入する。On the other hand, in the roll-to-roll method of this example, normally the first layer forming adjacent p, n (μC) type amorphous silicon
828s and PH3 gas are slowly flowing from the layer reaction chamber 1 and microcrystallization reaction chamber 3 to the single layer reaction chamber 2 that forms one layer! A trace amount is mixed in via the i-chamber 13.
これに対して1層反応室2は前述の構成としであるので
、i形非晶質シリコンを形成する1層反応室2において
反応ガスはn (μC)層用の微結晶化反応室3寄りの
ガス導入口15から導入され0層用の第1層反応室1寄
りの排気口16の方向に流れる。従って前述の作用が得
られる。On the other hand, since the single-layer reaction chamber 2 has the above-mentioned configuration, the reaction gas in the single-layer reaction chamber 2 for forming i-type amorphous silicon is closer to the microcrystallization reaction chamber 3 for the n (μC) layer. The gas is introduced from the gas inlet 15 and flows toward the exhaust port 16 near the first layer reaction chamber 1 for the zero layer. Therefore, the above-mentioned effect can be obtained.
この点をFIl認するため、本実施例において、100
μm厚のポリエチレンテレフタレートフィルム上に下部
電極層としてアルミニウム層とステンレス層を順次積層
した基板を用い、公知の常法と同様第1反応室1に水素
ガス希釈のBzHsとSiト14の混合ガスを、1層反
応室2に5IH4ガスを、微結晶化反応室3に水素ガス
希釈のP H3とS!H4の混合ガスを供給し、p。In order to confirm this point, in this example, 100
Using a substrate in which an aluminum layer and a stainless steel layer are sequentially laminated as a lower electrode layer on a μm-thick polyethylene terephthalate film, a mixed gas of BzHs and Si 14 diluted with hydrogen gas is introduced into the first reaction chamber 1 as in the conventional method. , 5IH4 gas in the single-layer reaction chamber 2, and hydrogen gas diluted PH3 and S! in the microcrystallization reaction chamber 3. Supply a mixed gas of H4, p.
n (μC)積層構造の非晶質シリコンからなる光起電
力層を形成し、以下のように評価した。すなわち、光起
電力層について、ボロン(B)原子のデプスプロファイ
ルを二次イオン質量分析法(Si MS)で測定した。A photovoltaic layer made of amorphous silicon having a laminated structure of n (μC) was formed and evaluated as follows. That is, the depth profile of boron (B) atoms in the photovoltaic layer was measured by secondary ion mass spectrometry (Si MS).
その結果を第7図に実I!Aで示す。比較のために、他
の条件は同じで、仕切#f111及び電界調整部材32
を設置しない従来装置の場合により形成した同じp、i
、n積層型の光起電力層の分析結果を破線Bで同図に示
した。The results are shown in Figure 7! Indicated by A. For comparison, other conditions are the same, partition #f111 and electric field adjustment member 32
The same p, i formed in the case of conventional equipment without installing
, n stack type photovoltaic layer is shown in the figure by a broken line B.
仕切板11を設けない従来装置の場合には第1層反応室
1から混入した8zH6ガスが1層反応室2全体に均一
に拡散する結果、1層中のB原子の膜厚方向の濃度プロ
ファイルはフラットになっている。一方、仕切板11を
設置した実施例の場合はp層とi層との界面におけるB
原子の組成プロファイルは切れが急峻になっており、ま
た、1層中のプロファイルは一定の勾配の傾斜をもって
いることがわかる。この結果は、仕切板11によって1
層反応室2のプラズマ空間を区分することにより、同−
反応至内であっても微結晶化反応室3寄りの部分から第
1層反応室1寄りの部分に亘ってプラズマ雰囲気中の反
応ガスの組成が一定の空間分布を有することを示してい
る。即ち本発明より1つ反応学内の反応ガスに必要な空
回分布が実現できることを意味しており、本発明が従来
不可能であって膜組成制御を可催とする優れた効果のあ
ることを示している。In the case of the conventional device without the partition plate 11, the 8zH6 gas mixed in from the first layer reaction chamber 1 diffuses uniformly throughout the single layer reaction chamber 2, resulting in a concentration profile of B atoms in the layer 1 in the film thickness direction. is flat. On the other hand, in the case of the embodiment in which the partition plate 11 is installed, B at the interface between the p layer and the i layer
It can be seen that the atomic composition profile has a sharp cut, and the profile in one layer has a constant slope. This result is 1 by the partition plate 11.
By dividing the plasma space in the layer reaction chamber 2, the same
This shows that the composition of the reactant gas in the plasma atmosphere has a constant spatial distribution from the part near the microcrystallization reaction chamber 3 to the part near the first layer reaction chamber 1 even during the reaction period. In other words, this means that the present invention can realize the idle circulation distribution required for the reaction gas in reaction science, and that the present invention has an excellent effect of making it possible to control the film composition, which was previously impossible. It shows.
次に一1ニ記で得られた光起電力層上にITO(l n
diul T in 0xide)からなる透明電場
。Next, ITO (l n
A transparent electric field consisting of diul Tin Oxide).
AQからなる収集電極を積層し、その太陽°虐池性能を
調べた。Collection electrodes made of AQ were stacked and their solar pond performance was investigated.
その結果表1に見られるごとく、1層反応室2内へ仕切
板11を設置せず、また微結晶化反応室へ電界調整部材
32を設置しなかった場合を比較例としたとき、本発明
を適用して作成した太陽電池では短絡電流、及び、曲線
因子に向上が得られた。As a result, as shown in Table 1, when the case where the partition plate 11 was not installed in the single-layer reaction chamber 2 and the electric field adjustment member 32 was not installed in the microcrystallization reaction chamber was used as a comparative example, the present invention The solar cells created by applying this method showed improvements in short-circuit current and fill factor.
この結果変換効率も大幅な向上を示し、本発明の有効性
が確認された。短絡電流の向上は、微結晶化n層が完全
に微結晶化したことによる吸収の減少によるものであり
、一方、曲線因子の向上は1層中でのホウ素原子の分布
が改善されたためと考えられる。As a result, the conversion efficiency also showed a significant improvement, confirming the effectiveness of the present invention. The improvement in short-circuit current is thought to be due to a decrease in absorption due to complete microcrystallization of the microcrystalline n-layer, while the improvement in fill factor is thought to be due to an improvement in the distribution of boron atoms in one layer. It will be done.
表1 太陽電池性能の比較Table 1 Comparison of solar cell performance
第1図は実施例の非晶質シリコン太陽電池の製造装置の
構成説明図、第2図は第1図A−A’線での断面図、第
3図は微結晶化反応室の側断面図。
第4図は従来例のマスクの平面図、第5図は実施例のマ
スクの平面図、第6図は実施例で得られた微結晶化非晶
質シリコン半導体層のマスク中心部の導電率の測定結果
を示すグラフ、第7図は実施例で得られた太陽電池の起
電力層中でのB(ボロン)原子の膜厚方向分布の測定結
果を示すグラフである。
1:第1層反応室、 2:1層反応室。
3:微結晶化反応室、11:仕切板。
13:緩衝室、17:基板、30:マスク。
32:電界調整部材
特許出願人 帝 人 株 式 会 社
冨Z 11
33図
ニドO
チー
第4図
βP刀ロ
パワー(W/cmJ
才気、m 力゛5の沼でr(pm)Fig. 1 is an explanatory diagram of the configuration of an apparatus for manufacturing an amorphous silicon solar cell according to an example, Fig. 2 is a cross-sectional view taken along line A-A' in Fig. 1, and Fig. 3 is a side cross-section of a microcrystallization reaction chamber. figure. FIG. 4 is a plan view of a conventional mask, FIG. 5 is a plan view of an example mask, and FIG. 6 is the conductivity of the center of the mask of the microcrystalline amorphous silicon semiconductor layer obtained in the example. FIG. 7 is a graph showing the measurement results of the distribution of B (boron) atoms in the film thickness direction in the electromotive force layer of the solar cell obtained in the example. 1: 1st layer reaction chamber, 2: 1st layer reaction chamber. 3: Microcrystallization reaction chamber, 11: Partition plate. 13: buffer chamber, 17: substrate, 30: mask. 32: Electric field adjustment member patent applicant Teijin Co., Ltd. Tomi Z 11 33 Figure Nido O Chi Figure 4 βP sword low power (W/cmJ brilliance, m force゛5 no swamp r (pm)
Claims (1)
結された化学的気相分解法により所定の非晶質半導体膜
を形成する所定数の反応室を備え、該基板を各反応室を
通して搬送し、該基板上に少なくとも一層の微結晶化非
晶質半導体層とi型非晶質半導体層とを有する光起電力
層を形成するようになした太陽電池の製造装置において
、反応ガスを遮断する仕切板を基板搬送方向に所定間隔
で放電電極面に垂直方向に配設して、少なくともプラズ
マ雰囲気を基板通路等の限られた隙間を除いて基板搬送
方向にガス拡散のない複数の区域に区画した、前記i型
非晶質半導体層を形成するi層反応室と、基板と放電電
極との間にマスクを配置すると共にその開口部に開口部
の電界分布を調節するための電界調整部材を設けた前記
微結晶化非晶質半導体層を形成する微結晶化反応室とを
具備したことを特徴とする太陽電池の製造装置。 2、前記連結された反応室の前後に巻出室と巻取室とを
連結して設け、長尺の可撓性の帯状基板をロール・ツ・
ロール方式で搬送するようになした請求項第1項記載の
太陽電池の製造装置。 3、p形又はn形の非晶質半導体層を形成する第1層反
応室、前記i型反応室、第1層反応室と逆の導電形の非
晶質半導体層を形成する前記微結晶化反応室が巻出室か
ら巻取室の間にこの順序で配置された請求項第1項又は
第2項記載の太陽電池の製造装置。[Scope of Claims] 1. A predetermined number of reaction chambers for forming a predetermined amorphous semiconductor film by a chemical vapor phase decomposition method connected so that a substrate can be transported between the discharge electrodes; Manufacture of a solar cell in which a substrate is transported through each reaction chamber and a photovoltaic layer having at least one microcrystallized amorphous semiconductor layer and an i-type amorphous semiconductor layer is formed on the substrate. In the apparatus, partition plates for blocking reaction gas are arranged perpendicularly to the discharge electrode surface at predetermined intervals in the substrate transport direction, so that at least the plasma atmosphere can be kept free of gas in the substrate transport direction except for limited gaps such as substrate passages. A mask is disposed between the i-layer reaction chamber in which the i-type amorphous semiconductor layer is formed, which is divided into a plurality of diffusion-free regions, the substrate and the discharge electrode, and the electric field distribution in the opening is controlled at the opening. 1. A solar cell manufacturing apparatus comprising: a microcrystallization reaction chamber for forming the microcrystallized amorphous semiconductor layer provided with an electric field adjustment member for adjustment. 2. An unwinding chamber and a winding chamber are connected before and after the connected reaction chambers, and a long flexible strip substrate is rolled up.
2. The solar cell manufacturing apparatus according to claim 1, wherein the solar cell manufacturing apparatus is conveyed by a roll method. 3. A first layer reaction chamber forming a p-type or n-type amorphous semiconductor layer, the i-type reaction chamber, and the microcrystal forming an amorphous semiconductor layer having a conductivity type opposite to that of the first layer reaction chamber. 3. The solar cell manufacturing apparatus according to claim 1, wherein the reaction chambers are arranged in this order between the unwinding chamber and the winding chamber.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63176939A JPH0719911B2 (en) | 1988-07-18 | 1988-07-18 | Solar cell manufacturing equipment |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP63176939A JPH0719911B2 (en) | 1988-07-18 | 1988-07-18 | Solar cell manufacturing equipment |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0227775A true JPH0227775A (en) | 1990-01-30 |
| JPH0719911B2 JPH0719911B2 (en) | 1995-03-06 |
Family
ID=16022382
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP63176939A Expired - Fee Related JPH0719911B2 (en) | 1988-07-18 | 1988-07-18 | Solar cell manufacturing equipment |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0719911B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20100159633A1 (en) * | 2008-12-18 | 2010-06-24 | Byoung-Kyu Lee | Method of manufacturing photovoltaic device |
-
1988
- 1988-07-18 JP JP63176939A patent/JPH0719911B2/en not_active Expired - Fee Related
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20100159633A1 (en) * | 2008-12-18 | 2010-06-24 | Byoung-Kyu Lee | Method of manufacturing photovoltaic device |
| US8329500B2 (en) * | 2008-12-18 | 2012-12-11 | Samsung Display Co., Ltd. | Method of manufacturing photovoltaic device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0719911B2 (en) | 1995-03-06 |
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