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JPS5910593B2 - Method of manufacturing photovoltaic device - Google Patents
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JPS5910593B2 - Method of manufacturing photovoltaic device - Google Patents

Method of manufacturing photovoltaic device

Info

Publication number
JPS5910593B2
JPS5910593B2 JP54028923A JP2892379A JPS5910593B2 JP S5910593 B2 JPS5910593 B2 JP S5910593B2 JP 54028923 A JP54028923 A JP 54028923A JP 2892379 A JP2892379 A JP 2892379A JP S5910593 B2 JPS5910593 B2 JP S5910593B2
Authority
JP
Japan
Prior art keywords
electrode
layer
power generation
substrate
areas
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP54028923A
Other languages
Japanese (ja)
Other versions
JPS55121686A (en
Inventor
幸徳 桑野
照豊 今井
雅和 梅谷
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.)
Sanyo Electric Co Ltd
Original Assignee
Sanyo 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 Sanyo Electric Co Ltd filed Critical Sanyo Electric Co Ltd
Priority to JP54028923A priority Critical patent/JPS5910593B2/en
Priority to US06/116,402 priority patent/US4281208A/en
Publication of JPS55121686A publication Critical patent/JPS55121686A/en
Publication of JPS5910593B2 publication Critical patent/JPS5910593B2/en
Expired legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F77/00Constructional details of devices covered by this subclass
    • H10F77/20Electrodes
    • H10F77/244Electrodes made of transparent conductive layers, e.g. transparent conductive oxide [TCO] layers
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10FINORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
    • H10F19/00Integrated devices, or assemblies of multiple devices, comprising at least one photovoltaic cell covered by group H10F10/00, e.g. photovoltaic modules
    • H10F19/30Integrated devices, or assemblies of multiple devices, comprising at least one photovoltaic cell covered by group H10F10/00, e.g. photovoltaic modules comprising thin-film photovoltaic cells
    • H10F19/31Integrated devices, or assemblies of multiple devices, comprising at least one photovoltaic cell covered by group H10F10/00, e.g. photovoltaic modules comprising thin-film photovoltaic cells having multiple laterally adjacent thin-film photovoltaic cells deposited on the same substrate
    • 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

Landscapes

  • Photovoltaic Devices (AREA)

Description

【発明の詳細な説明】 本発明は光起電力装置の製造方法に関する。[Detailed description of the invention] The present invention relates to a method for manufacturing a photovoltaic device.

太陽電池や光検出器のような光起電力装置は太陽光線を
直接電気エネルギに変換することができるが、この種装
置の最大の問題として、他の電気エネルギ発生手段と比
較して発電費用が極めて大きいことが言われている。そ
の主な原因は、装置の主体を構成する半導体材料の利用
効率が低いこ5 と、更には斯る材料を製造するに要す
るエネルギが多いことにある。ところが、最近、この様
な欠点を一部に解決する技術として、上記半導体材料に
非晶質シリコンを使用することが提案された。
Photovoltaic devices such as solar cells and photodetectors can directly convert sunlight into electrical energy, but the biggest problem with these devices is that they are expensive compared to other means of generating electrical energy. It is said to be extremely large. The main reasons for this are the low utilization efficiency of the semiconductor materials that constitute the main body of the device, and the large amount of energy required to manufacture such materials. However, recently, as a technique to partially solve these drawbacks, it has been proposed to use amorphous silicon as the semiconductor material.

即ち非晶質シリコ10 ンはシランやフロルシリコンな
どのシリコン化合物雰囲気中でのグロー放電(即ち、こ
れにより雰囲気はプラズマ状態になる)によつて安価か
つ大量に形成することができ、その場合の非晶質シリコ
ン(以下GD−aSiと略記する)では、禁止15帯の
幅中の平均局在状態密度が10”“儂−0以下と小さく
、結晶シリコンと同じ様にP型、N型の不純物制御が可
能となるものである。第1図は、GD−aSiを用いた
典型的な従来の太陽電池を示し、1は可視光を透過する
ガラス20基板、2は該基板上に形成された透明電極、
3、4及び5は夫々透明電極2上に順次形成されたGD
−aSl())P型層、GD−aSiのノンドープ(不
純物無添加)層及びGD−aS1のN型層であり、6は
該N型層上に設けられたオーミツクコ25 ンタクト用
電極である。
That is, amorphous silicon can be formed inexpensively and in large quantities by glow discharge in an atmosphere of a silicon compound such as silane or fluorosilicon (that is, the atmosphere becomes a plasma state). In amorphous silicon (hereinafter abbreviated as GD-aSi), the average localized state density within the width of the forbidden 15 band is as small as 10""2-0 or less, and like crystalline silicon, P-type and N-type This makes it possible to control impurities. FIG. 1 shows a typical conventional solar cell using GD-aSi, in which 1 is a glass 20 substrate that transmits visible light, 2 is a transparent electrode formed on the substrate,
3, 4 and 5 are GDs formed sequentially on the transparent electrode 2, respectively.
-aSl()) P-type layer, GD-aSi non-doped (impurity-free) layer, and GD-aS1 N-type layer, and 6 is an electrode for ohmic contact provided on the N-type layer.

上記太陽電池において、ガラス基板1及び透明電極2を
介して光がGD−aSiからなるP型層3、ノンドープ
層4及びN型層5に入ると、主にノンドープ層4におい
て自由状態の電子及び又は30正孔が発生し、これらは
上記各層の作るPIN接合電界により引かれて移動した
後透明電極2やオーミックコンタクト用電極6に集めら
れ両電極間に電圧が発生する。
In the above solar cell, when light enters the P-type layer 3, non-doped layer 4 and N-type layer 5 made of GD-aSi through the glass substrate 1 and transparent electrode 2, free-state electrons and Or, 30 holes are generated, which are attracted and moved by the PIN junction electric field created by the above-mentioned layers, and are then collected at the transparent electrode 2 or the ohmic contact electrode 6, and a voltage is generated between the two electrodes.

ところで、斯る太陽電池にあつては、その光起35電圧
は約O、8V程度であるため、より大きな電源電圧を必
要とする機器の電源としては上記太陽電池はそのまゝ使
用できない。
By the way, since the photovoltaic voltage of such a solar cell is about 0.8 V, the solar cell cannot be used as it is as a power source for equipment that requires a larger power supply voltage.

第2図は上記の点に鑑み既に提案された光起電力装置を
示し、7は可視光透過可能なガラスなどからなる平坦な
絶縁基板、8,9,10は該絶縁基板上に膜状に形成さ
れた第1、第2、第3の発電区域である。
Fig. 2 shows a photovoltaic device that has already been proposed in view of the above points, where 7 is a flat insulating substrate made of glass or the like that can transmit visible light, and 8, 9, and 10 are films on the insulating substrate. These are the first, second, and third power generation areas formed.

該発電区域の各々はGD−ASl層11と該層を挟んで
対向する第1電極12及び第2電極13から構成されて
いる。GD−ASl層11は図示していないが第1図の
構造と同様に基板7側から順次堆積されたP型層、ノン
ドープ層及びN型層の3層からなり、斯るGD−ASl
層11は第1〜第3の発電区域に連続して延びている。
Each of the power generation areas is composed of a GD-ASl layer 11 and a first electrode 12 and a second electrode 13 facing each other with the layer interposed therebetween. Although not shown, the GD-ASl layer 11 consists of three layers, a P-type layer, a non-doped layer, and an N-type layer, deposited sequentially from the substrate 7 side, similar to the structure shown in FIG.
The layer 11 extends continuously into the first to third power generation areas.

GD−ASl層11を構成する上記各層において、P型
層は膜厚40〜1000八、ドープ0量0.01〜17
01ノンドープ層は膜厚0.5〜2μM.N型層は膜厚
200〜1000人、ドープ量0.1〜370であり、
各層の形成温度は200〜400℃である。第1電極1
2は可視光透過性を有し、酸化錫、酸化インジウム、酸
化インジウム・錫(In2O3+XsnO2、x≦0.
1)などで構成することができるが、酸化インジウム・
錫が特に好ましい。
In each of the above layers constituting the GD-ASl layer 11, the P-type layer has a thickness of 40 to 1000 mm and a doping amount of 0.01 to 1.7 mm.
01 non-doped layer has a thickness of 0.5 to 2 μM. The N-type layer has a thickness of 200 to 1000, and a doping amount of 0.1 to 370.
The formation temperature of each layer is 200 to 400°C. First electrode 1
2 has visible light transmittance, and contains tin oxide, indium oxide, indium tin oxide (In2O3+XsnO2, x≦0.
1), etc., but indium oxide, etc.
Tin is particularly preferred.

第2電極13はアルミニウム、クロムなどで構成される
。第1〜第3発電区域8〜10の光々の第1電極12及
び第2電極13は基板7上において夫々の発電区域の外
へ延びる延長部14及び15を有し、第1発電区域8の
第2電極13の延長部14と第2発電区域9の第1電極
12の延長部14とが、又第2発電区域9の第2電極1
3の延長部15と第3発電区域10の第1電極12の延
長部14とが夫々互いに重畳して電気的に接続されてい
る。
The second electrode 13 is made of aluminum, chromium, or the like. The first electrode 12 and the second electrode 13 of the first to third power generation areas 8 to 10 have extensions 14 and 15 extending outside the respective power generation areas on the substrate 7, and the extension 14 of the first electrode 12 of the second power generation zone 9 are also connected to the second electrode 1 of the second power generation zone 9.
The extension part 15 of No. 3 and the extension part 14 of the first electrode 12 of the third power generation area 10 overlap each other and are electrically connected.

又第1発電区域8の第1電極12の延長部14には第2
電極13と同材料からなる接続部16が重畳被着されて
いる。上記装置の製造方法を簡単に説明すると、その第
1工程で基板7上に延長部14を含んだ第1電極12の
夫々が選択エツチング手法又は選択スパツタ付着手法に
より形成され、第2工程で第1〜第3発電区域に連続し
てGD−AS!層11が形成される。
Further, the extension part 14 of the first electrode 12 of the first power generation area 8 has a second
A connecting portion 16 made of the same material as the electrode 13 is attached in an overlapping manner. Briefly explaining the manufacturing method of the above device, in the first step each of the first electrodes 12 including the extension portions 14 is formed on the substrate 7 by selective etching or selective sputter deposition, and in the second step GD-AS consecutively in the 1st to 3rd power generation areas! Layer 11 is formed.

このとき、該層は上記延長部14,15に存在してはな
らないので、基板7上全面に上記3層からなるGD−A
Si層を形成した後、選択エツチング手法により不要部
を除去するか、あるいは不要部を覆うマスクを用いるこ
とにより所望部のみに上記3層からなるGD−ASiが
形成される。続く最終工程において延長部15を含む第
2電極13及び接続部16が選択蒸着手法などにより形
成される。上記装置において、基板7及び第1電極12
を介して光がGD−ASi層11に入ると、第1〜第3
発電区域8〜10の夫々において第1図の場合と同様に
起電圧が生じ、各区域の第1、第2電極12,13はそ
の延長部において交互に接続されているので各区域の起
電圧は直列的に相加され、第1発電区域8に連なる接続
部16を+極、第3発電区域10の第2電極13に連な
る延長部15を一極として両極の間に上記の如く相加さ
れた電圧が発生する。
At this time, since this layer must not exist in the extension parts 14 and 15, the GD-A made of the three layers is completely covered on the substrate 7.
After forming the Si layer, the GD-ASi consisting of the three layers described above is formed only in the desired portions by removing unnecessary portions by selective etching or using a mask to cover the unnecessary portions. In the subsequent final step, the second electrode 13 including the extension portion 15 and the connection portion 16 are formed by selective vapor deposition or the like. In the above device, the substrate 7 and the first electrode 12
When light enters the GD-ASi layer 11 through the
In each of the power generation zones 8 to 10, an electromotive force is generated in the same way as in the case of FIG. are added in series, with the connection part 16 connected to the first power generation area 8 being the + pole, and the extension part 15 connected to the second electrode 13 of the third power generation area 10 being one pole, and added between the two poles as described above. A voltage is generated.

尚上記装置において第1電極12に連なる延長部14に
は電極材料の性質により外部リード線を超音波ボテンテ
イングなどにより接続するのが困難であるが、接続部1
6の存在はこれを容易になすものである。
In the above device, it is difficult to connect an external lead wire to the extension part 14 connected to the first electrode 12 by ultrasonic buttoning etc. due to the properties of the electrode material.
The presence of 6 facilitates this.

上記装置によれば、非晶質シリコンを用い、同一基板上
にて複数の発電区域を直列接続したものであつて、小型
にしてかつ任意の起電圧を発生する装置が得られ、又斯
る装置は非晶質シリコンを用いたが故に実現されたもの
であり、その製造に際しても第1図に示す従来の製造工
程とほとんど変るところなく簡単な膜形成工程のみで製
造することができ、量産的にも極めて優れたものである
According to the above-described device, a plurality of power generation areas are connected in series on the same substrate using amorphous silicon, and a device can be made compact and generate any desired electromotive voltage. The device was realized because it uses amorphous silicon, and its manufacturing process is almost the same as the conventional manufacturing process shown in Figure 1, with only a simple film formation process, making mass production possible. It is also extremely excellent.

ところで、上記装置において、各発電区域の隣接間隔が
小さいと、隣り合う区域の第1電極12どうし、あるい
は第2電極13どうしの間で直接電流が流れる現象、即
ち漏れ電流の発生が認められるが、本発明は斯る漏れ電
流を実質的に抑止し得る構造を提供するものである。第
3図は本発明実施例を示し、その特徴とするところは、
各発電区域の隣接区間にあるGDaSl層11の少なく
とも一部が第2電極13を形成後絶縁層20に変質され
ていることにある。
By the way, in the above device, if the distance between adjacent power generation areas is small, a phenomenon in which current flows directly between the first electrodes 12 or between the second electrodes 13 in the adjacent areas, that is, leakage current occurs. The present invention provides a structure that can substantially suppress such leakage current. FIG. 3 shows an embodiment of the present invention, and its features are as follows:
At least a portion of the GDaSl layer 11 in an area adjacent to each power generation area is transformed into an insulating layer 20 after the second electrode 13 is formed.

その他の構成は第2図と同一である。即ち本実施例によ
ると絶縁層20の存在により上記隣接区間のGD−AS
l層11の実質的厚みが小となるため隣り合う区域の第
1電極12どうし、あるいは第2電極13どうしの間の
抵抗が増大し上記電極間の漏れ電流が抑制されるのであ
る。上記絶縁層20を形成する方法の具体例は、既に形
成済みの第2電極13をマスクとして酸素や窒素を当該
領域にイオン注入法により選択的に注入し、その領域の
GD−ASlを絶縁体化することである。このとき注入
原子が酸素の場合GD−ASiはSiOxに、又窒素の
場合SiNxの夫々変質する。注入原子はこのはかフツ
素も使用できる。上記絶縁層形成のための他の方法は、
酸素ガスや水蒸気等の雰囲気で熱酸化することにより当
該領域を酸化物に変えたり、あるいは窒素ガスやアンモ
ニアガス雰囲気での加熱により当該領域を窒化物に変え
ることである。
The other configurations are the same as in FIG. 2. That is, according to this embodiment, due to the presence of the insulating layer 20, the GD-AS in the adjacent section
Since the substantial thickness of the L layer 11 is reduced, the resistance between the first electrodes 12 or the second electrodes 13 in adjacent areas increases, and leakage current between the electrodes is suppressed. A specific example of the method for forming the insulating layer 20 is to selectively implant oxygen or nitrogen into the region by ion implantation using the already formed second electrode 13 as a mask, and convert the GD-ASl in the region into an insulator. It is to become At this time, when the implanted atoms are oxygen, GD-ASi is transformed into SiOx, and when nitrogen is implanted, the GD-ASi is transformed into SiNx. This fluorine element can also be used as the implanted atom. Another method for forming the above insulating layer is
This means converting the region into an oxide by thermal oxidation in an atmosphere of oxygen gas, water vapor, etc., or converting the region into a nitride by heating in a nitrogen gas or ammonia gas atmosphere.

これらの場合にも第2電極13は領域選択のためのマス
クとして利用できる。上記絶縁層形成のための更に他の
方法は、酸素ガスあるいは窒素ガスを含むプラズマ状態
の雰囲気に装置を曝すことである。
In these cases as well, the second electrode 13 can be used as a mask for region selection. Yet another method for forming the insulating layer is to expose the device to a plasma atmosphere containing oxygen gas or nitrogen gas.

これらの場合同様にGD−ASlは酸化物や窒化物に変
質する。又第2電極13は同様に領域選択のためのマス
クとなる。絶縁層20の深さは必要に応じて決められ、
場合によつては基板7に達する深さでも良い。
Similarly in these cases, GD-ASl changes into oxides and nitrides. Similarly, the second electrode 13 serves as a mask for region selection. The depth of the insulating layer 20 is determined as necessary,
In some cases, the depth may reach the substrate 7.

しかし、GD−ASl層11のN型層5の不純物濃度が
高いので該層を断ち切る深さでも十分有効である。以下
に上述の如き不純物濃度が高いGD−ASi層11のN
型層5を絶縁層20に変質する製造条件の一例を記す。
However, since the impurity concentration of the N-type layer 5 of the GD-ASl layer 11 is high, a depth that cuts this layer is sufficiently effective. Below, N of the GD-ASi layer 11 with high impurity concentration as described above is shown.
An example of manufacturing conditions for transforming the mold layer 5 into the insulating layer 20 will be described.

尚、以上の条件により酸化せしめられるN型層5の不純
物濃度はPH3/SlH4−170、膜厚は500八で
あつた。
The impurity concentration of the N-type layer 5 oxidized under the above conditions was PH3/SlH4-170, and the film thickness was 500.

次に斯るN型層5のSlOXの絶縁層20に変質せしめ
た際の漏れ電流を測定したところ、従来2.5μAの漏
れ電流が1nA以下に減少した。
Next, when the leakage current was measured when the N-type layer 5 was transformed into the SlOX insulating layer 20, the leakage current was reduced from 2.5 μA to 1 nA or less.

以上の説明から明らかな如く、本発明によれば構成に不
可欠な第2電極を形成後、相隣り合う第2電極間に位置
する非晶質半導体層の少なくとも一部を絶縁層に変質せ
しめたので、斯る絶縁層は発電区域の隣接間隔部に確実
に配置され、上記隣接間隔部に於ける漏れ電流を有効に
抑えることができ、発電効率の向上が図れる。
As is clear from the above description, according to the present invention, after forming the second electrode essential to the structure, at least a portion of the amorphous semiconductor layer located between adjacent second electrodes is transformed into an insulating layer. Therefore, such an insulating layer is reliably disposed in the adjacent spacing portions of the power generation area, and leakage current in the adjacent spacing portions can be effectively suppressed, thereby improving power generation efficiency.

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

第1図は従来装置を示す側面図、第2図Aは既に提案さ
れた装置を示す平面図、第2図B及びCは夫々第2図A
におけるB−B及びC−C断面図、第3図は本発明実施
例を示す要部断面図である。 7・・・・・・絶縁基板、8,9,10・・・・・・第
1、第2、第3発電区域、11・・・・・・非晶質シリ
コン層、20・・・・・・絶縁層。
Figure 1 is a side view showing a conventional device, Figure 2A is a plan view showing an already proposed device, and Figures 2B and C are respectively Figure 2A.
FIG. 3 is a cross-sectional view of essential parts showing an embodiment of the present invention. 7... Insulating substrate, 8, 9, 10... First, second, third power generation areas, 11... Amorphous silicon layer, 20... ...Insulating layer.

Claims (1)

【特許請求の範囲】[Claims] 1 絶縁基板上に形成された膜状の複数の発電区域を有
し、該区域の各々は光照射により発電に寄与する電子及
び又は正孔を発生する非晶質半導体層と該層を挾んで対
向する上記基板側の第1電極及び表面側の第2電極とを
含む光起電力装置の製造方法であつて、上記複数の発電
区域の各々に連続して非晶質半導体層を形成すると共に
、各発電区域の間にある上記半導体の少なくとも一部を
上記第2電極を形成後絶縁層に変質することを特徴とし
た光起電力装置の製造方法。
1. It has a plurality of film-like power generation areas formed on an insulating substrate, and each of the areas is sandwiched between an amorphous semiconductor layer that generates electrons and/or holes that contribute to power generation when irradiated with light. A method for manufacturing a photovoltaic device including a first electrode on the substrate side and a second electrode on the front side facing each other, the method comprising forming an amorphous semiconductor layer continuously in each of the plurality of power generation areas, and . A method for manufacturing a photovoltaic device, characterized in that at least a portion of the semiconductor between the power generation areas is transformed into an insulating layer after forming the second electrode.
JP54028923A 1979-02-09 1979-03-12 Method of manufacturing photovoltaic device Expired JPS5910593B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP54028923A JPS5910593B2 (en) 1979-03-12 1979-03-12 Method of manufacturing photovoltaic device
US06/116,402 US4281208A (en) 1979-02-09 1980-01-29 Photovoltaic device and method of manufacturing thereof

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP54028923A JPS5910593B2 (en) 1979-03-12 1979-03-12 Method of manufacturing photovoltaic device

Publications (2)

Publication Number Publication Date
JPS55121686A JPS55121686A (en) 1980-09-18
JPS5910593B2 true JPS5910593B2 (en) 1984-03-09

Family

ID=12261913

Family Applications (1)

Application Number Title Priority Date Filing Date
JP54028923A Expired JPS5910593B2 (en) 1979-02-09 1979-03-12 Method of manufacturing photovoltaic device

Country Status (1)

Country Link
JP (1) JPS5910593B2 (en)

Families Citing this family (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6095980A (en) * 1983-10-31 1985-05-29 Semiconductor Energy Lab Co Ltd Photoelectric conversion device
JPS607778A (en) * 1983-06-27 1985-01-16 Semiconductor Energy Lab Co Ltd Photoelectric conversion semiconductor device
JPS59155973A (en) * 1983-02-25 1984-09-05 Semiconductor Energy Lab Co Ltd Photoelectric conversion semiconductor device
JPS6014479A (en) * 1983-07-04 1985-01-25 Semiconductor Energy Lab Co Ltd Photoelectric conversion device manufacturing method
JPS60211881A (en) * 1984-04-05 1985-10-24 Semiconductor Energy Lab Co Ltd Manufacture of semiconductor device
JPS60211817A (en) * 1984-04-05 1985-10-24 Semiconductor Energy Lab Co Ltd Apparatus for photoelectric conversion
JPS61139072A (en) * 1984-12-11 1986-06-26 Agency Of Ind Science & Technol Method of manufacturing photovoltaic device
KR100416139B1 (en) * 2001-04-04 2004-01-31 삼성에스디아이 주식회사 Solar battery module

Also Published As

Publication number Publication date
JPS55121686A (en) 1980-09-18

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