JPS60102773A - Amorphous base solar battery - Google Patents

Amorphous base solar battery

Info

Publication number
JPS60102773A
JPS60102773A JP58209080A JP20908083A JPS60102773A JP S60102773 A JPS60102773 A JP S60102773A JP 58209080 A JP58209080 A JP 58209080A JP 20908083 A JP20908083 A JP 20908083A JP S60102773 A JPS60102773 A JP S60102773A
Authority
JP
Japan
Prior art keywords
amorphous
layer
transparent electrode
glass substrate
refractive index
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
JP58209080A
Other languages
Japanese (ja)
Inventor
Kazufumi Azuma
和文 東
Masahiro Tanaka
政博 田中
Mitsuo Nakatani
中谷 光雄
Masaaki Okunaka
正昭 奥中
Akio Saito
昭男 斉藤
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP58209080A priority Critical patent/JPS60102773A/en
Publication of JPS60102773A publication Critical patent/JPS60102773A/en
Pending legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L31/00Semiconductor devices sensitive to infrared radiation, light, electromagnetic radiation of shorter wavelength or corpuscular radiation and specially adapted either for the conversion of the energy of such radiation into electrical energy or for the control of electrical energy by such radiation; Processes or apparatus specially adapted for the manufacture or treatment thereof or of parts thereof; Details thereof
    • H01L31/02Details
    • H01L31/0216Coatings
    • H01L31/02161Coatings for devices characterised by at least one potential jump barrier or surface barrier
    • H01L31/02167Coatings for devices characterised by at least one potential jump barrier or surface barrier for solar cells
    • H01L31/02168Coatings for devices characterised by at least one potential jump barrier or surface barrier for solar cells the coatings being antireflective or having enhancing optical properties for the solar 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

Abstract

PURPOSE:To improve the photoelectric conversion ratio by cutting the light reflecting power down to ideal value by a method wherein an intermediate layer with refractive index different from those of a glass substrate and a transparent electrode is laid between said substrate and electrode. CONSTITUTION:An intermediate layer 5 with refractive index different from those of a glass substrate 1 and a transparent electrode 2 is laid between said substrate 1 and electrode 2 within an amorphous solar battery constituted to intake light into an amorphous layer through the intermediary of the glass substrate 1 and the transparent electrode 2. The intermediate layer 5 may be se lected from a composition of one or two kinds of mixed oxide of e.g. Ti, Si, Ta and Al, etc. making the light reflecting power minimum.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は、アモルファス系太陽電池(例えばアモルファ
スシリコン太it池、アモルファス5i−C層、アモル
ファス51−Gg層などを含むアモルファス太陽電池に
関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Application of the Invention] The present invention relates to an amorphous solar cell (eg, an amorphous solar cell including an amorphous silicon fat cell, an amorphous 5i-C layer, an amorphous 51-Gg layer, etc.).

〔発明の背景〕[Background of the invention]

この種のアモルファス系太陽電池、例エバアモルファス
シリコン太陽電池は、結晶系太陽電池に比べ、低コスト
化・大面積化が可能であり急速に開発が進められてきた
が、変換効率は、まだ結晶系に追いつけない状況である
This type of amorphous solar cell, e.g. EVA amorphous silicon solar cell, is capable of lower costs and larger area than crystalline solar cells, and has been rapidly developed. The situation is such that they cannot catch up with the system.

従来のアモルファスシリコン太陽電池には、金属を基板
としたものと、ガラスを基板としたものとがあり、ガラ
スを基板としたものでは、例えば、ガラス上に透明電極
をつけ、その上にpm、i層、n層のアモルファスシリ
コンを積み、アルミ電極を蒸着した構造となっている。
Conventional amorphous silicon solar cells include those that use metal as a substrate and those that use glass as a substrate. In those that use glass as a substrate, for example, a transparent electrode is attached to the glass, and pm, It has a structure in which i-layer and n-layer amorphous silicon are stacked and aluminum electrodes are deposited.

このガラスを基板としたアモルファスシリコン太陽電池
の光電変換効率を上げるために、以下の例に示すような
様々な工夫がなされている。
In order to increase the photoelectric conversion efficiency of amorphous silicon solar cells using glass as a substrate, various efforts have been made as shown in the following examples.

(1) 受光面側の1層でキャリアを生成しても、表面
再結合の影響が太きいため、光電変換に有効に寄与しな
い。そこで1層での光吸収を抑え、2層に光を多く取入
れるために、P層には光学的バンドギャップの大きいア
モルファス炭化ケイ素を使う。
(1) Even if carriers are generated in one layer on the light-receiving surface side, the influence of surface recombination is large, so they do not contribute effectively to photoelectric conversion. Therefore, in order to suppress light absorption in the first layer and allow more light to enter the second layer, amorphous silicon carbide with a large optical bandgap is used for the P layer.

(2) アモルファスシリコンはキャリア移動度が小さ
く、暗伝導度も小さい。そのため、光のあまり届かない
ル層では、かなり抵抗も大きくなり、太陽電池の効率を
悪くしている。そこでル層を微結晶化し、抵抗を下げ、
加えて4層の吸光度を下げ、裏面のアルミによる光の反
射を利用して透過してきた光を2層にもどすことによっ
て光電変換効率を上けている。
(2) Amorphous silicon has low carrier mobility and low dark conductivity. As a result, the resistance of the solar cell layer, which does not receive much light, increases considerably, reducing the efficiency of the solar cell. Therefore, we microcrystallize the Le layer to lower the resistance.
In addition, the photoelectric conversion efficiency is increased by lowering the absorbance of the four layers and using light reflection from the aluminum on the back to return the transmitted light to the second layer.

(3) 太陽光を有効に吸収させるためには、光電変換
素子の分光感度を太陽光スペクトルに一致させればよい
。そこで、光学的バンドギャップの異なる2種類の半導
体を用いて、pn接合を2重に形成し、その組合わせに
より、幅広い太陽光スペクトルに近い分光感度を有する
光電変換素子を作り、変換効率を上げている。
(3) In order to effectively absorb sunlight, the spectral sensitivity of the photoelectric conversion element should match the spectrum of sunlight. Therefore, we formed a double pn junction using two types of semiconductors with different optical band gaps, and by combining them, we created a photoelectric conversion element with spectral sensitivity close to a wide range of sunlight spectra, increasing conversion efficiency. ing.

(4) 入射光を効率よく素子内に取入れるため、ガラ
ス表面に、反射率を最小にするような反射防止膜を形成
し、ガラス表面での反射を抑え、変換効率を上げている
(4) In order to efficiently introduce incident light into the element, an anti-reflection film is formed on the glass surface to minimize reflectance, suppressing reflection on the glass surface and increasing conversion efficiency.

以上の例のような工夫により、アモルファスシリコン太
陽電池の光電変換効率は向上してきたが、未だ不十分で
ある。
Although the photoelectric conversion efficiency of amorphous silicon solar cells has been improved through efforts such as those in the above examples, it is still insufficient.

そこで更に効率向上のための方法として、ガラス基板と
透明電極の界面での反射を抑えるため、透明電極の膜厚
を調整して、反射率を小さくする工夫がなされている。
Therefore, as a method to further improve efficiency, in order to suppress reflection at the interface between the glass substrate and the transparent electrode, efforts have been made to adjust the film thickness of the transparent electrode to reduce the reflectance.

第1図において、ガラス基板1の屈折率をrL2透明電
極2の屈折率n1、厚さdo、アモルファスシリコン層
6の屈折率をyLoとすると、反射率Rは 光の波長である。この場合、ガラス基板の屈折率は1.
5前後、透明電極の屈折率は20前後であるから、上記
のRを最小にして効率を上げるた0 ・ めには、透明電極の膜厚をうまく選べば良い。
In FIG. 1, the refractive index of the glass substrate 1 is rL2, the refractive index of the transparent electrode 2 is n1, the thickness is do, and the refractive index of the amorphous silicon layer 6 is yLo, then the reflectance R is the wavelength of light. In this case, the refractive index of the glass substrate is 1.
5, and the refractive index of the transparent electrode is around 20, so in order to minimize R and increase efficiency, the thickness of the transparent electrode should be selected appropriately.

ところが、透明電極の膜厚は、自由に選べるわけではな
い。即ち、膜厚が厚いと入射光の透過率が低下してしま
い、薄すぎると電極として抵抗値が高くなりすぎるなど
、制約があったため、反射率Rを理想的な値まで下げる
ことができなかった。
However, the thickness of the transparent electrode cannot be freely selected. In other words, if the film thickness is too thick, the transmittance of incident light will decrease, and if it is too thin, the resistance value as an electrode will be too high.Therefore, it was not possible to lower the reflectance R to the ideal value. Ta.

〔発明の目的〕[Purpose of the invention]

本発明は、光の反射率を理想的な値まで下は光電変換率
が向上させたアモルファス系太陽電池を提供することを
目的とする。
An object of the present invention is to provide an amorphous solar cell in which the light reflectance is reduced to an ideal value and the photoelectric conversion rate is improved.

〔発明の概要〕[Summary of the invention]

本発明は、ガラス基板と透明電極とを介してアモルファ
ス属へ光を取り入れる構造のアモルファス系太陽電池に
おいて、ガラス基板と透明電極との間に、両者と異なる
屈接率を有する中間層を介在させて構成する。
The present invention provides an amorphous solar cell having a structure in which light is introduced into the amorphous layer through a glass substrate and a transparent electrode, in which an intermediate layer having a refractive index different from that of the glass substrate and the transparent electrode is interposed between the glass substrate and the transparent electrode. Configure.

これにより、光の反射率を理想的な値まで下げ、光電変
換率を向上させることができる。すなわち、入射光がガ
ラスから透明電極を通過す、4 。
Thereby, the light reflectance can be lowered to an ideal value and the photoelectric conversion rate can be improved. That is, the incident light passes through the transparent electrode from the glass, 4.

る際に、ガラス、透明電極界面での光の反射があり、こ
れが太きいと、有効に使える光量が減少してしまうため
、ガラスと透明電極の間に異なる屈折率を有する中間層
を入れて、入射光の層間での反射をできるだけ小さくす
る。
During the process, light is reflected at the interface between the glass and the transparent electrode, and if this is too thick, the amount of light that can be used effectively will be reduced. Therefore, an intermediate layer with a different refractive index is inserted between the glass and the transparent electrode. , to minimize the reflection of incident light between layers.

ガラス基板の屈折率をル8、中間層の屈折率をTL2、
膜厚をdt、透明電極の屈折率をルい膜厚をdl、アモ
ルファスシリコン等のアモルファス層の屈折率を町とす
ると反射率Rは次の式で示される。
The refractive index of the glass substrate is Le 8, the refractive index of the intermediate layer is TL2,
When the film thickness is dt, the refractive index of the transparent electrode is dl, and the refractive index of an amorphous layer such as amorphous silicon is dl, the reflectance R is expressed by the following formula.

R= [l (yb(、−TL3)001iδICxB
δ。
R= [l (yb(,-TL3)001iδICxB
δ.

((さユールり房δ1山δ! 2 TL(1ル3 +(yJ)sinδ1coSδ!)2〕n。((Sayuru Ribo δ1 mountain δ! 2 TL (1 le 3 +(yJ)sinδ1coSδ! )2]n.

/〔((rLo十rL3)cosδ1cOsδ。/[((rLo×rL3)cosδ1cOsδ.

、 (nQ n、−+ルりμsδ1thδ2LR TLOrL8 +(−+rL、) 出 δ菫 α四 δ2 )2 〕n
, (nQ n, -+Ruri μsδ1thδ2LR TLOrL8 +(-+rL,) Out δ Sum α4 δ2 )2 ] n
.

λは入射光の波長である。λ is the wavelength of the incident light.

この式において中間層の屈折率rL2、膜厚d2を適当
に選ぶことにより反射率Rを理想的な値まで小さくする
ことが可能となる。
In this equation, by appropriately selecting the refractive index rL2 and film thickness d2 of the intermediate layer, it is possible to reduce the reflectance R to an ideal value.

本発明で用いる中間層としては、例えば、Tt。As the intermediate layer used in the present invention, for example, Tt.

Si 、Ta、M、 pb等の酸化物を1種又は2種以
上混合した組成のものが用いられる。
The composition used is one or a mixture of two or more oxides such as Si, Ta, M, and PB.

成膜方法としては、上記金属を含む化合物をスピンナ塗
布後、焼成する方法、あるいは蒸着法、スパッタ法、C
VD法などが例としてあけられる。
Film formation methods include a method of coating a compound containing the above metal with a spinner and then baking it, a vapor deposition method, a sputtering method, a carbon
An example is the VD method.

透明電極の屈折率、膜厚に応じて、中間層の材質は上述
の金属酸化物の組合せから適当な屈折率のものを選び、
適当な膜厚に制御することにより、反射率Rを最小値に
おさえることが可能である。
Depending on the refractive index and film thickness of the transparent electrode, a material with an appropriate refractive index is selected from the above-mentioned combinations of metal oxides as the material for the intermediate layer.
By controlling the film thickness to an appropriate value, it is possible to suppress the reflectance R to a minimum value.

本発明に用いるガラス基板は、ソーダガラス。The glass substrate used in the present invention is soda glass.

・ 7 ・ 白色ガラス、パイレックス等特に制限はない。・ 7 ・ There are no particular restrictions, such as white glass or Pyrex.

また、本発明に用いる透明電極は、ITO、5n02あ
るいはこれらの組合せなどが用いられる。
Further, the transparent electrode used in the present invention is made of ITO, 5n02, or a combination thereof.

〔発明の実施例〕[Embodiments of the invention]

以下に本発明の実施例の若干につき、図面に基づいて説
明する。
Some embodiments of the present invention will be described below based on the drawings.

第2図は本発明のアモルファス系太陽電池の一構造例を
示す断面図である。このアモルファス系太陽電池には、
そのガラス基板1と透明電極2との間に、両者の屈折率
とは異なる屈折率を有する中間層5を介在させである。
FIG. 2 is a sectional view showing an example of the structure of the amorphous solar cell of the present invention. This amorphous solar cell has
An intermediate layer 5 having a refractive index different from those of the glass substrate 1 and the transparent electrode 2 is interposed between the glass substrate 1 and the transparent electrode 2.

これにより光の反射率を理想的な値まで下げ、光電変換
率を向上させることができる。
This makes it possible to lower the light reflectance to an ideal value and improve the photoelectric conversion rate.

以下に本発明のより詳細な実施例を説明1−る。More detailed examples of the present invention will be described below.

下記の各実施例は、本発明をアモルファスシリコン太陽
電池に適用して具体化したものである。
Each of the following examples embodies the present invention by applying it to an amorphous silicon solar cell.

実施例1 厚さ11mのソーダガラス上に、テトラブチルチタネー
トとオルトケイ酸エチルの混合液をスピンナ塗布し、4
80’Oで60分間加熱し、約−3。
Example 1 A mixed solution of tetrabutyl titanate and ethyl orthosilicate was applied with a spinner onto soda glass with a thickness of 11 m, and
Heat at 80'O for 60 minutes, about -3.

1200Aの膜を形成し中間層5をした。エリプンメー
タでこの膜の屈折率を沖]定すると1.90であった。
A film of 1200A was formed and an intermediate layer 5 was formed. The refractive index of this film was determined using an ellipse meter and was found to be 1.90.

この上に透明電極11としてITOをEB蒸着で200
0.(の膜厚で形成した。この基板を用いて以下に述べ
る方法でPtn層を形成し、アモルファスシリコン太陽
電池を作成した。
On top of this, ITO was deposited as a transparent electrode 11 by EB evaporation to a thickness of 200 mm.
0. Using this substrate, a Ptn layer was formed by the method described below to create an amorphous silicon solar cell.

成膜装置は、6室分離型のプラズマCVD装置を用いた
。1層はSiE46sccM 、 CM414sccM
As a film forming apparatus, a six-chamber separation type plasma CVD apparatus was used. 1st layer is SiE46sccM, CM414sccM
.

He希釈の2.0 % B2.B62 zccMを流し
、0,5Torrのガス圧で、基板温度300’0、r
fパワー4Wで60秒放電した。ついで2層はHe希釈
の10%Si2B6500zccMを流し、350 ’
01.2 T orrでrfパワー80Wで2分間放電
した。最後にル層は、SiE、 i sccM 、 E
2希釈1007Pi pH3を20zccM流し、25
0 ’01. OT orrでrfバ’7−80Fで1
5分放電した。こうして、第3図に示すように、1層1
2をBドープのSiC膜、を層16をα−5i:H膜、
ル層14をPドープの微結晶化Si膜として形成した。
2.0% of He dilution B2. B62 zccM was flowing, the gas pressure was 0.5 Torr, and the substrate temperature was 300'0, r.
It was discharged for 60 seconds at f power of 4W. Next, 10% Si2B6500zccM diluted with He was poured into the second layer, and the layer was heated for 350'
The battery was discharged for 2 minutes at 0.01.2 T orr with an RF power of 80 W. Finally, the layer is SiE, i sccM , E
Flow 20zccM of 2 diluted 1007Pi pH3, 25
0 '01. OT orr and rf bar '7-80F 1
It was discharged for 5 minutes. In this way, as shown in FIG.
2 is a B-doped SiC film, layer 16 is an α-5i:H film,
The layer 14 was formed as a P-doped microcrystalline Si film.

こうして作成したアモルファスシリコン太陽電池の効率
を測定したところ、025−の面積で開放電圧0.78
0V、短絡電流14.77 mA /ctA、フィルフ
ァクター0550であり、6.35%の変換効率が得ら
れた。
When the efficiency of the amorphous silicon solar cell created in this way was measured, the open circuit voltage was 0.78 with an area of 025-
0V, short circuit current 14.77 mA/ctA, fill factor 0550, and a conversion efficiency of 6.35% was obtained.

比較例として、中間層を有しない同様のITO基板を用
いて同じ条件で太陽電池を作成したところ、O,2S=
の面積で変換効率は6.05%であり本実施例のそれに
比べ小さかった。
As a comparative example, when a solar cell was created under the same conditions using a similar ITO substrate without an intermediate layer, O,2S=
The conversion efficiency was 6.05% for the area of , which was smaller than that of this example.

実施例2 実施例1と同様の方法で、中間層として、屈折率2.2
のTatOs膜を240OAになるように形成膜した。
Example 2 In the same manner as in Example 1, a refractive index of 2.2 was prepared as an intermediate layer.
A TatOs film of 240 OA was formed.

このガラス基板上に1層として、5tR4(5zccM
 、 CM414sccM 、 B、1162.0 %
 (He希釈)2sccMを流し、300’0.0,5
Torrでrfパワー4Wで35秒間放電し、a−5i
C膜を形成した。
5tR4 (5zccM
, CM414sccM, B, 1162.0%
(He dilution) Flow 2sccM, 300'0.0,5
Discharge for 35 seconds with rf power 4W at Torr, a-5i
A C film was formed.

ついで、2層は、SiH4を1105ec流し、0.5
Torr 350°0でrfパワー4Wで30分間放電
しα−5i:H膜を形成した。最後にル層として、Si
H,1gccM 、 PR,100ppm (E!希釈
)20sccMを流し、1.OTorr 、250°0
でγfパワーsoFで15分間放電し、微結晶化Si膜
を形成した。この上にM電極を蒸着により形成し、実施
例1と同様にして効率を測定したところ、025−の面
積で変換効率8.90%を得た。比較例として同条件で
Ta2O,の中間層がない場合を測定すると、8.40
%の変換効率であり、中間層の形成により、1.06倍
の効率向上が達成できた。
Next, the second layer was made by flowing SiH4 for 1105 ec and 0.5
An α-5i:H film was formed by discharging at 350° Torr and RF power of 4 W for 30 minutes. Finally, as a layer, Si
Flowing 20sccM of H, 1gccM, PR, 100ppm (E! dilution), 1. OTorr, 250°0
A microcrystalline Si film was formed by discharging at γf power soF for 15 minutes. When an M electrode was formed on this by vapor deposition and the efficiency was measured in the same manner as in Example 1, a conversion efficiency of 8.90% was obtained for an area of 025-. As a comparative example, a case without the intermediate layer of Ta2O was measured under the same conditions, and the result was 8.40.
% conversion efficiency, and by forming the intermediate layer, an efficiency improvement of 1.06 times could be achieved.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、入射光に対する反射が理想的に小さく
できるため、アモルファス系太陽電池において、光電変
換効率を向上させる効果がある。
According to the present invention, since reflection of incident light can be ideally reduced, there is an effect of improving photoelectric conversion efficiency in an amorphous solar cell.

また、中間層は、ガラス基板からのNa+の拡散を防止
するための下地膜ともなるため、本発明によれば太陽電
池の品質に対する信頼性を向上させ得るという効果も生
ずる。
Further, since the intermediate layer also serves as a base film for preventing Na+ diffusion from the glass substrate, the present invention also has the effect of improving the reliability of the quality of the solar cell.

なお当然のことではあるが本発明は上記実施例に限定さ
れるものではない。例えば、実施例ではアモルファスシ
リコン太陽電池を代表的な11 。
Note that, as a matter of course, the present invention is not limited to the above embodiments. For example, in the example, an amorphous silicon solar cell is representatively used.

ものとして示したが、5i−Geを用いたもの、その他
の太陽電池にも本発明は適用可能である。
Although shown as a solar cell, the present invention is also applicable to those using 5i-Ge and other solar cells.

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

第1図は、従来のアモルファスシリコン太陽電池の断面
図、第2図及び第3図は本発明の実施例に係る太陽電池
の断面図である。 1・・・・・・・・・・ガラス基板 2・・・・・・・・・・・透明電極(ITO)3・・・
・・・・・・・・・アモルファス層(アモルファスシリ
コン層) 5・・・・・・・・・・・・中間層 8・・・・・・・・・・・・M電極 12・・・・・11層 16・曲・・・・を層 14・・−・・・・・ル層 、12 。 第1図 ↑ 届 第3図 廟2図 第1頁の続き [相]発 明 者 斉 藤 昭 男 横浜市戸塚区吉術
研究所内
FIG. 1 is a sectional view of a conventional amorphous silicon solar cell, and FIGS. 2 and 3 are sectional views of a solar cell according to an embodiment of the present invention. 1...Glass substrate 2...Transparent electrode (ITO) 3...
......Amorphous layer (amorphous silicon layer) 5...Intermediate layer 8...M electrode 12... ... 11 layers 16 songs... layer 14... le layer, 12. Figure 1 ↑ Continued from Figure 2, Page 1 of Notification Figure 3 [Phase] Inventor Akio Saito Inside the Kijutsu Research Institute, Totsuka-ku, Yokohama City

Claims (1)

【特許請求の範囲】 1、 ガラス基板と透明電極とを介してアモルファス層
へ光を取り入れる構造のアモルファス系太ist池にお
いて、該ガラス基板と該透明電極との間に、該ガラス基
板の油接率及び該透明基板の油接率と異なる油接率を有
する中間層を介在させたことを特徴とするアモルファス
系太陽電池。 2、前記アモルファス層が、アモルファスシリコン、ア
モルファス5i−C,アモルファス51−Ggの内、少
なくともいずれか1種類を含有して成ることを特徴とす
る特許請求の範囲第1項記載のアモルファス系太陽電池
[Claims] 1. In an amorphous film having a structure in which light is introduced into an amorphous layer through a glass substrate and a transparent electrode, an oil contact layer of the glass substrate is provided between the glass substrate and the transparent electrode. 1. An amorphous solar cell characterized in that an intermediate layer having an oil contact ratio different from that of the transparent substrate is interposed. 2. The amorphous solar cell according to claim 1, wherein the amorphous layer contains at least one of amorphous silicon, amorphous 5i-C, and amorphous 51-Gg. .
JP58209080A 1983-11-09 1983-11-09 Amorphous base solar battery Pending JPS60102773A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58209080A JPS60102773A (en) 1983-11-09 1983-11-09 Amorphous base solar battery

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58209080A JPS60102773A (en) 1983-11-09 1983-11-09 Amorphous base solar battery

Publications (1)

Publication Number Publication Date
JPS60102773A true JPS60102773A (en) 1985-06-06

Family

ID=16566929

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58209080A Pending JPS60102773A (en) 1983-11-09 1983-11-09 Amorphous base solar battery

Country Status (1)

Country Link
JP (1) JPS60102773A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6424865U (en) * 1987-07-31 1989-02-10
JPH01171050U (en) * 1988-05-20 1989-12-04
JPH02164077A (en) * 1988-12-19 1990-06-25 Hitachi Ltd Amorphous silicon solar cell
JPH02164079A (en) * 1988-12-19 1990-06-25 Hitachi Ltd Amorphous silicon solar cell

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6424865U (en) * 1987-07-31 1989-02-10
JPH01171050U (en) * 1988-05-20 1989-12-04
JPH02164077A (en) * 1988-12-19 1990-06-25 Hitachi Ltd Amorphous silicon solar cell
JPH02164079A (en) * 1988-12-19 1990-06-25 Hitachi Ltd Amorphous silicon solar cell
JPH0583199B2 (en) * 1988-12-19 1993-11-25 Hitachi Ltd

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