JPH03166771A - Thin film solar cell - Google Patents

Thin film solar cell

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Publication number
JPH03166771A
JPH03166771A JP1306013A JP30601389A JPH03166771A JP H03166771 A JPH03166771 A JP H03166771A JP 1306013 A JP1306013 A JP 1306013A JP 30601389 A JP30601389 A JP 30601389A JP H03166771 A JPH03166771 A JP H03166771A
Authority
JP
Japan
Prior art keywords
layer
solar cell
type
substrate
thin film
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.)
Pending
Application number
JP1306013A
Other languages
Japanese (ja)
Inventor
Shinji Fujikake
伸二 藤掛
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP1306013A priority Critical patent/JPH03166771A/en
Publication of JPH03166771A publication Critical patent/JPH03166771A/en
Pending legal-status Critical Current

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Classifications

    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/546Polycrystalline silicon PV cells
    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/50Photovoltaic [PV] energy
    • Y02E10/548Amorphous silicon PV cells

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  • Photovoltaic Devices (AREA)

Description

【発明の詳細な説明】 (産業上の利用分野〕 本発明は非晶質シリコン (以下a −Stと記す)を
主材料とし、p−i−n接合構造により光電変換をする
薄膜太陽電池に関する. 〔従来の技術〕 非晶質半導体、特にa −Sl薄膜を用いた薄膜太陽電
池は大面積化が容易、原料コストが小さくてすむといっ
た利点をもち、低コスト太陽電池として期待されている
.通常、a −St太陽電池はガラスなどの透光性の基
板にSnOxなどの透明かつ導電性のある透明導電膜に
よって透明電極を形成し、七の上にグロー放電分解を利
用したプラズマCvD法によりp形.i形,n形のa 
−51層を順次形成し、さらにMやAlなどの金属電極
を真空蒸着法やスパッタリング法により形成することに
より製造される. 〔発明が解決しようとする課題〕 しかし、プラズマCVD法により形成されたa一Sl膜
は光照射下において膜質が劣化し、その中でl層の膜質
の劣化が原因となって太陽電池の,効率が低下する、い
わゆるステブラー・ロンスキー効果と呼ばれる現象が問
題となっていた.これに,対し、熱CVD法によって形
成されたa −51膜は光による膜質の劣化が小さく、
このため太陽電池としての効率の低下がない. 熱CVD法は、反応室を大気圧もしくは減圧のHeもし
くはh雰囲気中において450〜500℃の戒膜温度に
昇温させたのち、反応ガスを導入して熱分解させ、支持
台上にセットされた基板上に堆積させる.基板としては
、ステンレス鯛などの金属板を研摩したものか、ガラス
等の絶縁板の上にMやAgの電極を形成したものが用い
られる,a−Sf或膜のための反応ガスとしては、SL
tHhを主ガスとして、H8またはLを希釈ガスとして
用い、n層を形或する場合にはこれにPll.を加え、
p層を形戒する場合には81H&を加える.また、最上
部に形成されるp形もしくはn形のドーピング層は、不
純物の拡散をおさえるため、150〜200℃程度の低
温でプラズマCVD法などにより形成されることもある
. 第2図はそのような薄膜太陽電池の一例を示し、ステン
レス鋼からなる導電性基板11上に熱CVD法により形
成されたn形a−Sl層12,lWiCVD法により形
成されたl形a −51層13およびプラズマCVD法
により形成されたp形a −Sl層14を積層し、さら
に透明導電膜よりなる透明電極15を被着したものであ
る.この太陽電池は、透明電極15を通して入射する光
10により起電力を生じ、基板11に設けられた端子1
6,透明電極15に設けられた端子17から取り出され
る. しかしながら、この方法によって製造された太陽電池は
光による特性の劣化はないものの、戒膜温度が450〜
500℃と高いため、基板を構戒する金属がa−Sl層
中に拡散し、太陽電池としての特性を低下させるという
問題があった. 本発明の目的は、a−Slの戒膜に熱CVD法を適用し
て光による劣化をおさえるとともに、a 一Sl膜への
基板からの金属の拡散をおさえることのできる薄膜太陽
電池を提供することにある.〔課題を解決するための手
段〕 上記の目的を達處するために、本発明の薄膜太陽電池は
、絶縁性基板上に低抵抗で第一導電形の多結晶シリコン
層、熱CVD法で形成されたl形のa−51層およびプ
ラズマCVD法で形成された第二導電形のa−31層を
順次積層してなるものとする. 〔作用〕 l層を熱CVD法で形處するので光による膜質の劣化が
少ない.また、基板に接する低抵抗多結晶シリコン層が
、n形もしくはp形の半導体層としてp−1−n構造の
一部をなすほか、電極としての役割を兼用するため、熱
CVD法の際の温度における汚染源である金属基板を用
いる必要がない.さらに、l層の上のp層もしくはn層
が低温で実施されるプラズマCVD法で形成されるので
、多結晶シリコンに含まれる不純物のl層への拡散も起
こらず、クリーンな半導体接合が実現され、高効率が得
られる. 〔実施例〕 第1図は、本発明の一実施例の薄膜太陽電池を示す.こ
の太陽電池は、ガラス基板l上に電極の役割を兼ねたn
形の多結晶シリコン層2を熱CVD法で形成し、その上
にl形a−Si層3を熱CvD法により、さらにその上
にp形a−Si層4をプラズマCVD法により積層した
p−i−n構造を有する.p層4の上には透明導tM5
が形成され、透明電極の役割をする.この太陽電池も、
上面から入射する光10により起電力を生じ、多結晶シ
リコン層2に設けられた端子16,透明電極5に設けら
れた端子17から取り出される. 第3図は、第1図に示した太陽電池の製造装置の断面図
である.この装置は、熱CVD室61とプラズマCVD
室62を連結したものである.熱CvD室6lは電気炉
63の中に収容されており、プラズマCVD室62には
、高周波電極64とヒータを備えた電極65が対向配置
されている.先ず、この装置の熱CVD室61に支持台
66上に装着したガラス基板1を入れ、h雰囲気で60
0℃に加熱した.排気管7lから真空引きしたのち、ガ
ス導管81から前室67を経てSl!I#およびPal
sを導入し、l Torrの圧力下で熱cvnにより基
板1上に抵抗率sxio−’Ω個のn形多結晶シリコン
層2を1nの厚さに或膜した.この多結晶シリコン層2
のシート抵抗はlOΩ以下であるので、十分電極として
の役割を果たすことができる.次に、このl!icVD
室6lに118ガスを導入し、480℃に降温しさらに
均熱化を行った.均熱終了後真空引きを行い、主ガスS
l!H1希釈ガスHeをガス導管8lから導入し、圧力
を50Torrに保ち、熱CVDによりl形a−31層
3を5000人の厚さに或膜した.その後、熱CVD室
6lを排気管71から、またプラズマCVD室62を排
気管72か?真空引きし、バルブ68を開け、基板1を
プラズマCVD室62に移動した.移動後H,を導入し
、基板温度を200℃に降温し、均熱化を行った.次い
で、排気管72から真空引きを行い、ガス導管82から
SIH■BJhCJ■Htを導入し、圧力を0.5 T
orrに保ち、電極64に高周波電圧を印加し、プラズ
マCVDによりp形a−SIC層4を150人の厚さに
或膜した.さらに、真空引き後、大気にパージし、バル
プ69を開け、基板1を外部に取り出し、n形a−St
層4の上に透明導電膜5を或膜した.第4図は、第1図
に示した本発明の実施例のa一Si太陽電池および第2
図に示した従来のa −Si太陽電池のセル特性をそれ
ぞれ191.92により比較したものである.本発明に
基づく太陽電池の変換効率は9.0%であり、従来法に
よる太陽電池の変換効率は7.3%だった.このことか
ら、本発明の実施例の方法を採用することにより、熱C
VD法による基板からの不純物の拡散がなく、効率の向
上がはかられることがわかった.また、この二つの太陽
電池に100 sW/一の光を100時間照射したが、
共に劣化はみられなかった. 第5図は本発明の他の実施例を示す.ガラス基板1上に
直列に集積化されたa −31太陽電池が形成されてい
る.先ず、基板1上にn形ポリシリコン層を形成し、レ
ーザパターニングを行うことにより、電極を兼ねたn形
領域21.22.23.24・・・に分割する.その上
に熱CVD法によるl形a −Sl層およびプラズマC
VDによるp形a−SIC層を形成し、レーザバターニ
ングにより、i形領域31,32.33.34・・・お
よびp形領域41.42.43.44・・・に分割する
.その上に透明導電膜を形成し、レーザバターニングに
より透明電極51.52.53.54・・・に分割する
ことによって光10より起電力を生ずる集積型a一St
太陽電池が作製される.従来法で集積型太陽電池を作製
する場合、絶縁基板を用いてその上にまず金属電極を蒸
着する必要がある.この実施例ではこのプロセスが不要
なためより簡単なプロセスで集積型太陽電池を作製する
ことができる.なお、第1図.第5図に示した太陽電池
の導電形を逆にすることも容易にできることは明らかで
ある. 〔発明の効果〕 本発明によれば、a−Stを主材料としたp−1−n構
造の1層を熱CVD法で形成してステプラー・ロンスキ
ー効果による膜質の劣化を低減し、その五層を基板側の
接合を形成する層を低抵抗な多結晶シリコンで形成する
ことにより、金属電極が不要になり、熱CVD時に金属
の拡散により汚染されないp−1−n接合構造が実現す
るため効率が向上し、それによって高効率で高信頼性の
薄膜太陽電池を得ることができた.特に、直列集積形の
太陽電池においては、絶縁基板上に金属電極旗を形成す
る必要がなく、より低コストとすることが可能になった
Detailed Description of the Invention (Industrial Field of Application) The present invention relates to a thin film solar cell that uses amorphous silicon (hereinafter referred to as a-St) as its main material and performs photoelectric conversion using a pin junction structure. [Prior Art] Thin-film solar cells using amorphous semiconductors, especially a-Sl thin films, have the advantages of being easy to increase in area and requiring low raw material costs, and are expected to be used as low-cost solar cells. Normally, a-St solar cells are made by forming a transparent electrode with a transparent conductive film such as SnOx on a transparent substrate such as glass, and using a plasma CVD method using glow discharge decomposition on top of the substrate. p-type.i-type, a of n-type
-51 layers are sequentially formed, and metal electrodes such as M or Al are formed by vacuum evaporation or sputtering. [Problems to be Solved by the Invention] However, the film quality of the a-Sl film formed by the plasma CVD method deteriorates under light irradiation, and the deterioration of the film quality of the l layer causes problems in solar cells. The so-called Stebler-Wronsky effect, which reduces efficiency, has been a problem. On the other hand, the a-51 film formed by thermal CVD has less deterioration in film quality due to light.
Therefore, there is no decrease in efficiency as a solar cell. In the thermal CVD method, the reaction chamber is heated to a film temperature of 450 to 500°C in a He or H atmosphere at atmospheric pressure or reduced pressure, then a reaction gas is introduced to cause thermal decomposition, and the reaction chamber is set on a support. deposited on a substrate. The substrate used is a polished metal plate such as stainless steel or an insulating plate such as glass with M or Ag electrodes formed on it.Reactive gas for the a-Sf film is as follows: SL
When forming an n-layer using thHh as the main gas and H8 or L as the diluent gas, Pll. Add
Add 81H& when p-layer formalization is required. Further, the p-type or n-type doped layer formed at the top is sometimes formed by plasma CVD or the like at a low temperature of about 150 to 200° C. in order to suppress diffusion of impurities. FIG. 2 shows an example of such a thin film solar cell, showing an n-type a-Sl layer 12 formed by thermal CVD on a conductive substrate 11 made of stainless steel, and an l-type a-Sl layer 12 formed by WiCVD. 51 layer 13 and a p-type a-Sl layer 14 formed by the plasma CVD method, and further covered with a transparent electrode 15 made of a transparent conductive film. This solar cell generates an electromotive force by light 10 incident through a transparent electrode 15, and a terminal 1 provided on a substrate 11 generates an electromotive force.
6. Taken out from the terminal 17 provided on the transparent electrode 15. However, although the solar cells manufactured by this method do not deteriorate in characteristics due to light, the film temperature is 450~450℃.
Because the temperature was as high as 500°C, there was a problem in that the metal that contained the substrate was diffused into the a-Sl layer, degrading the characteristics of the solar cell. An object of the present invention is to provide a thin-film solar cell in which the thermal CVD method is applied to an a-Sl film to suppress deterioration due to light, and the diffusion of metal from the substrate into the a-Sl film can be suppressed. There is a particular thing. [Means for Solving the Problems] In order to achieve the above object, the thin film solar cell of the present invention includes a low resistance polycrystalline silicon layer of the first conductivity type formed on an insulating substrate by a thermal CVD method. The A-51 layer of the L-type formed by A-51 and the A-31 layer of the second conductivity type formed by the plasma CVD method are sequentially laminated. [Function] Since the L layer is formed by thermal CVD, there is little deterioration of the film quality due to light. In addition, the low-resistance polycrystalline silicon layer in contact with the substrate forms part of the p-1-n structure as an n-type or p-type semiconductor layer, and also serves as an electrode. There is no need to use a metal substrate, which is a source of temperature contamination. Furthermore, since the p-layer or n-layer above the l-layer is formed by plasma CVD, which is carried out at low temperatures, impurities contained in polycrystalline silicon do not diffuse into the l-layer, resulting in a clean semiconductor junction. and high efficiency can be obtained. [Example] Figure 1 shows a thin film solar cell according to an example of the present invention. This solar cell consists of a glass substrate with a n
A p-type polycrystalline silicon layer 2 is formed by a thermal CVD method, an l-type a-Si layer 3 is deposited on top of it by a thermal CVD method, and a p-type a-Si layer 4 is deposited thereon by a plasma CVD method. -i-n structure. A transparent conductor tM5 is formed on the p layer 4.
is formed and acts as a transparent electrode. This solar cell also
The light 10 incident from the top surface generates an electromotive force, which is extracted from the terminal 16 provided on the polycrystalline silicon layer 2 and the terminal 17 provided on the transparent electrode 5. FIG. 3 is a sectional view of the solar cell manufacturing apparatus shown in FIG. 1. This device consists of a thermal CVD chamber 61 and a plasma CVD chamber 61.
This is a combination of chambers 62. The thermal CVD chamber 6l is housed in an electric furnace 63, and in the plasma CVD chamber 62, a high frequency electrode 64 and an electrode 65 equipped with a heater are arranged facing each other. First, the glass substrate 1 mounted on the support stand 66 was placed in the thermal CVD chamber 61 of this apparatus, and heated for 60 hours in an atmosphere of
It was heated to 0°C. After evacuating from the exhaust pipe 7l, the gas conduit 81 passes through the front chamber 67 to Sl! I# and Pal
An n-type polycrystalline silicon layer 2 having a resistivity sxio-'Ω and a thickness of 1n was formed on the substrate 1 by thermal CVN under a pressure of 1 Torr. This polycrystalline silicon layer 2
Since its sheet resistance is less than 10Ω, it can sufficiently function as an electrode. Next, this l! icVD
118 gas was introduced into a 6L chamber, the temperature was lowered to 480°C, and the temperature was further soaked. After soaking, vacuum the main gas S.
l! H1 diluent gas He was introduced through an 8L gas conduit, the pressure was maintained at 50 Torr, and an L-type A-31 layer 3 was deposited to a thickness of 5000 mm by thermal CVD. After that, the thermal CVD chamber 6l is connected to the exhaust pipe 71, and the plasma CVD chamber 62 is connected to the exhaust pipe 72? After evacuation, the valve 68 was opened, and the substrate 1 was moved to the plasma CVD chamber 62. After the transfer, H was introduced, the substrate temperature was lowered to 200°C, and the temperature was soaked. Next, the exhaust pipe 72 is evacuated, SIH BJhCJHt is introduced from the gas conduit 82, and the pressure is increased to 0.5 T.
A high frequency voltage was applied to the electrode 64, and a p-type a-SIC layer 4 was formed to a thickness of 150 nm by plasma CVD. Furthermore, after evacuation, the air is purged, the valve 69 is opened, the substrate 1 is taken out to the outside, and the n-type a-St
A transparent conductive film 5 was formed on the layer 4. FIG. 4 shows the a-Si solar cell of the embodiment of the present invention shown in FIG.
The cell characteristics of the conventional a-Si solar cells shown in the figure are compared by 191.92. The conversion efficiency of the solar cell based on the present invention was 9.0%, and the conversion efficiency of the solar cell using the conventional method was 7.3%. From this, by adopting the method of the embodiment of the present invention, it is possible to
It was found that there is no diffusion of impurities from the substrate due to the VD method, and efficiency can be improved. In addition, these two solar cells were irradiated with light of 100 sW/1 for 100 hours,
No deterioration was observed in either case. FIG. 5 shows another embodiment of the present invention. A-31 solar cells integrated in series are formed on a glass substrate 1. First, an n-type polysilicon layer is formed on a substrate 1, and laser patterning is performed to divide the layer into n-type regions 21, 22, 23, 24, . . . which also serve as electrodes. On top of that, an l-type a-Sl layer and a plasma C layer are formed by thermal CVD.
A p-type a-SIC layer is formed by VD and divided into i-type regions 31, 32, 33, 34, . . . and p-type regions 41, 42, 43, 44, . . . by laser patterning. An integrated type a-St that generates an electromotive force from the light 10 by forming a transparent conductive film thereon and dividing it into transparent electrodes 51, 52, 53, 54, etc. by laser patterning.
A solar cell is created. When fabricating integrated solar cells using conventional methods, it is necessary to first deposit metal electrodes on an insulating substrate. In this example, this process is not necessary, so an integrated solar cell can be fabricated using a simpler process. In addition, Fig. 1. It is clear that the conductivity type of the solar cell shown in Figure 5 can be easily reversed. [Effects of the Invention] According to the present invention, one layer with a p-1-n structure made of a-St as the main material is formed by thermal CVD to reduce the deterioration of film quality due to the Stepler-Wronski effect. By forming the layer that forms the bond on the substrate side with low-resistance polycrystalline silicon, a metal electrode is no longer required, and a p-1-n junction structure that is not contaminated by metal diffusion during thermal CVD is realized. The efficiency was improved, and as a result, we were able to obtain highly efficient and highly reliable thin-film solar cells. In particular, in series-integrated solar cells, there is no need to form metal electrode flags on an insulating substrate, making it possible to lower costs.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の一実施例の薄膜太陽電池の断面図、第
2図は従来の薄膜太陽電池の断面図、第3図は第l図の
太陽電池の製造に用いる装置の断面図、第4図は第1図
および第2図に示した太陽電池の出力特性線図、第5図
は本発明の別の実施例の集積型太陽電池の断面図である
. 1:ガラス基板、2+n形多結晶シリコン層、3+l形
a−Sl層、4:p形a−SiC層、5=透明電極、6
1:熱CVD室、62=プラズマCvD室.第1 図 第2図 1l 第3図 第4図 1 第5図
FIG. 1 is a sectional view of a thin film solar cell according to an embodiment of the present invention, FIG. 2 is a sectional view of a conventional thin film solar cell, and FIG. 3 is a sectional view of an apparatus used for manufacturing the solar cell shown in FIG. FIG. 4 is an output characteristic diagram of the solar cell shown in FIGS. 1 and 2, and FIG. 5 is a sectional view of an integrated solar cell according to another embodiment of the present invention. 1: Glass substrate, 2+n-type polycrystalline silicon layer, 3+l-type a-Sl layer, 4: p-type a-SiC layer, 5=transparent electrode, 6
1: Thermal CVD chamber, 62 = Plasma CVD chamber. Figure 1 Figure 2 Figure 1 l Figure 3 Figure 4 Figure 1 Figure 5

Claims (1)

【特許請求の範囲】[Claims] 1)絶縁性基板上に低抵抗で第一導電形の多結晶シリコ
ン層、熱CVD法で形成されたi形の非晶質シリコン層
およびプラズマCVD法で形成された第二導電形の非晶
質シリコン層を順次積層してなることを特徴とする薄膜
太陽電池。
1) A low-resistance polycrystalline silicon layer of the first conductivity type on an insulating substrate, an i-type amorphous silicon layer formed by thermal CVD, and a second conductivity type amorphous silicon layer formed by plasma CVD. A thin film solar cell characterized by being formed by sequentially stacking high quality silicon layers.
JP1306013A 1989-11-25 1989-11-25 Thin film solar cell Pending JPH03166771A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1306013A JPH03166771A (en) 1989-11-25 1989-11-25 Thin film solar cell

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1306013A JPH03166771A (en) 1989-11-25 1989-11-25 Thin film solar cell

Publications (1)

Publication Number Publication Date
JPH03166771A true JPH03166771A (en) 1991-07-18

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JP1306013A Pending JPH03166771A (en) 1989-11-25 1989-11-25 Thin film solar cell

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Country Link
JP (1) JPH03166771A (en)

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