JPS60200577A - Photoelectric conversion semiconductor device - Google Patents
Photoelectric conversion semiconductor deviceInfo
- Publication number
- JPS60200577A JPS60200577A JP59057713A JP5771384A JPS60200577A JP S60200577 A JPS60200577 A JP S60200577A JP 59057713 A JP59057713 A JP 59057713A JP 5771384 A JP5771384 A JP 5771384A JP S60200577 A JPS60200577 A JP S60200577A
- Authority
- JP
- Japan
- Prior art keywords
- electrode
- electrodes
- semiconductor
- groove
- photoelectric conversion
- 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
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F77/00—Constructional details of devices covered by this subclass
- H10F77/20—Electrodes
- H10F77/206—Electrodes for devices having potential barriers
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F39/00—Integrated devices, or assemblies of multiple devices, comprising at least one element covered by group H10F30/00, e.g. radiation detectors comprising photodiode arrays
- H10F39/10—Integrated devices
- H10F39/107—Integrated devices having multiple elements covered by H10F30/00 in a repetitive configuration, e.g. radiation detectors comprising photodiode arrays
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F39/00—Integrated devices, or assemblies of multiple devices, comprising at least one element covered by group H10F30/00, e.g. radiation detectors comprising photodiode arrays
- H10F39/10—Integrated devices
- H10F39/12—Image sensors
- H10F39/191—Photoconductor image sensors
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F71/00—Manufacture or treatment of devices covered by this subclass
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10F—INORGANIC SEMICONDUCTOR DEVICES SENSITIVE TO INFRARED RADIATION, LIGHT, ELECTROMAGNETIC RADIATION OF SHORTER WAVELENGTH OR CORPUSCULAR RADIATION
- H10F71/00—Manufacture or treatment of devices covered by this subclass
- H10F71/121—The active layers comprising only Group IV materials
-
- 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
- Y02E10/547—Monocrystalline silicon PV cells
-
- 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
- Y02P—CLIMATE CHANGE MITIGATION TECHNOLOGIES IN THE PRODUCTION OR PROCESSING OF GOODS
- Y02P70/00—Climate change mitigation technologies in the production process for final industrial or consumer products
- Y02P70/50—Manufacturing or production processes characterised by the final manufactured product
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- Photovoltaic Devices (AREA)
Abstract
Description
【発明の詳細な説明】
この発明は、光電変換素子またはセル(以下単にセルと
いう)を絶縁表面を有する可曲性の基板上に複合化する
に関し、隣合ったセル間の切断線(開溝)を肉眼では十
分見分けに(い100μ以下好ましくは10〜50μと
し、装置全体としての視覚的商品価値を向上させること
を目的としている。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to composite photoelectric conversion elements or cells (hereinafter simply referred to as cells) on a flexible substrate having an insulating surface. ) can be easily discerned with the naked eye (less than 100μ, preferably 10 to 50μ), with the aim of improving the visual commercial value of the device as a whole.
この発明は、ステンレス基板等のり曲性基板上に絶縁表
面を有する薄膜、例えば有機樹脂薄膜を設け、かかる絶
縁表面を有する基板↓に第1の電極ラステンレス、クロ
ムまたはクロムを主成分とする耐熱性金属(以下単にク
ロムという)薄膜、アルミニュームのごとき反射性金属
とその上面の酸化スズのごとき透光性導電)挨とよりな
る複合電極により設りたものとである。かかる第1の電
極練性薄膜例えば自機樹脂筒13にまった< ti傷を
与えることのない条件が実験的に存在することを見いだ
し、この事実を利用して半導体装置特に光電変換装置を
作製せんとしたものである。This invention provides a thin film having an insulating surface, such as an organic resin thin film, on a bendable substrate such as a stainless steel substrate, and a first electrode made of stainless steel, chromium, or a heat-resistant material mainly composed of chromium, on the substrate ↓ having such an insulating surface. The electrode is made of a composite electrode consisting of a reflective metal (hereinafter simply referred to as chromium) thin film, a reflective metal such as aluminum, and a translucent conductive (conductive) dust such as tin oxide on its upper surface. It has been experimentally found that there are conditions under which no damage is caused to the first electrode-formable thin film, for example, the resin cylinder 13, and this fact is utilized to fabricate semiconductor devices, particularly photoelectric conversion devices. It's a serious thing.
このため、本発明においては、活性領域に設けられたセ
ルにおける有機樹脂薄膜(以下OFという)の基板上に
、第1の電極と、この電極上に光照射により光起電力を
発生ずる非単結晶半導体と、該半導体上の第2の電極と
よりなる複数の素子を直列接続して配設するに関し、隣
合った素子間の電気的連結を活性領域の内部に開孔また
は開/aS(以下単に開fしという)を設け、この開イ
しによりコンタクトを設けて成就したことを特長とする
。For this reason, in the present invention, a first electrode is provided on a substrate of an organic resin thin film (hereinafter referred to as OF) in a cell provided in an active region, and a non-single electrode that generates a photovoltaic force by light irradiation is provided on this electrode. When arranging a plurality of devices consisting of a crystalline semiconductor and a second electrode on the semiconductor in series, electrical connection between adjacent devices is established by opening or opening/aS ( The present invention is characterized in that it has been achieved by providing an opening (hereinafter simply referred to as an opening) and providing a contact using this opening.
光電変換装置の安価、多量生産のための基板として絶縁
表面を有する可曲性の薄膜の使用がめられてきた。2. Description of the Related Art Flexible thin films having an insulating surface have been used as substrates for inexpensive, mass production of photoelectric conversion devices.
本発明はこのため、カールまたは熱処理により延び、縮
のないステンレス薄膜(厚さ50〜150μ)とその上
にポリイミド樹脂(不透明であってよい)の耐熱性OF
を設けたものを基板とし、安価かつ安定性のよい可曲性
基板とした。For this reason, the present invention is a heat-resistant OF film made of a thin stainless steel film (thickness 50-150μ) that can be stretched by curling or heat treatment and has no shrinkage, and a polyimide resin (which may be opaque) on top of it.
The substrate was made into a flexible substrate that was inexpensive and had good stability.
本発明はかかるOFと、その上の昇華性を有する導?l
i股特にクロムを生成分とする金属、酸化インジューム
または酸化スズを生成分とする導電性酸化膜に対して、
レーザ光を照射した時、この叶をtrJ化せずにその上
の導電性薄膜を選択的に除去することができる条件を実
験的に検討したところ、そのレーザ光を1つの場所に長
時間(数十m秒以上)照射することなく、また走査(ス
キャン)スピードを適切化することにより、この電極用
導電月料のみを除去することが可能であることを見いだ
した。The present invention provides such an OF and a conductive material having sublimation properties thereon. l
In particular, for conductive oxide films containing metals containing chromium, indium oxide, or tin oxide,
We experimentally investigated the conditions under which the conductive thin film on the leaves could be selectively removed without turning the leaves into trJ when irradiated with laser light. We have found that it is possible to remove only this conductive material for electrodes by optimizing the scanning speed and without irradiating the electrode for several tens of milliseconds or more.
即ち、レーザ光の照射により叶は熱伝導率が小さい(一
般には1〜7 X 1O−4Cal / sec /
ca! / ℃/cm)ため、同し位置に繰り返しレー
ザパルスを加えると、この有機樹脂内に熱が曹積され、
この熱で樹脂が炭化され切断されてしまう。しかしその
繰り返しを1回または数回とすると、この叶の熱伝導率
が導電性薄膜(以下CFという)例えばクロムまたはア
ルミニュームとCTFとの複合膜の1/10〕であるた
め、逆にCFのみを選択的にレーザ光の照射された場所
のみ除去することができることを見いだした。That is, by irradiation with laser light, the leaf has a low thermal conductivity (generally 1 to 7 x 1O-4 Cal / sec /
ca! / °C/cm), so when laser pulses are repeatedly applied to the same position, heat is accumulated in this organic resin,
This heat carbonizes the resin and causes it to be cut. However, if this process is repeated once or several times, the thermal conductivity of this leaf is 1/10 that of a conductive thin film (hereinafter referred to as CF), such as a composite film of chromium or aluminum and CTF. It has been found that only the areas irradiated with laser light can be selectively removed.
従来、非単結晶半導体特にアモルファスシI/コンを含
む非単結晶シリコンを主成分としたPIN接合により、
光起電力を光照射により発生させんとしていた。しかし
かがる接合を有する半導体の上下の電極は直列接続をす
るため、1つのセルの下側電極と隣のセルの上側電極と
の電気的連結を活性領域のF外側Jでさせなければなら
ず、かつ各セル間は互いに電気的にアイソレイトされて
いることを必要な条件としていた。Conventionally, PIN junctions based on non-single-crystal semiconductors, especially non-single-crystal silicon including amorphous silicon, have been used.
They were trying to generate photovoltaic force through light irradiation. However, since the upper and lower electrodes of a semiconductor having a bending junction are connected in series, the lower electrode of one cell and the upper electrode of the adjacent cell must be electrically connected at the F outer side J of the active region. In addition, it was a necessary condition that each cell be electrically isolated from each other.
第1図は従来構造の代表的な例を示している。FIG. 1 shows a typical example of a conventional structure.
第1図(A)は光電変換装置(1)を透光性のガラス基
板(2)を下側にした背面より見た平面図である。FIG. 1(A) is a plan view of the photoelectric conversion device (1) viewed from the back with the transparent glass substrate (2) facing downward.
図面において、光照射により光起電力を発律する活性領
域(14)と、各セル(11)、<13)を連結する連
結部(12)を有する非活性領域(15)とを有する。In the drawing, it has an active region (14) that generates photovoltaic force upon irradiation with light, and an inactive region (15) having a connecting portion (12) that connects each cell (11), <13).
第1図(A)のA−A’、B−B’の縦断面図を対応さ
せて(B >、< C)に示していることより明らかな
ごとく、活性領域において各セル(11)、(13)は
ガラス基板(2)上の第1の電極の透光性導電n’=
(CTF >の(3)は各セル間で互いに分離されてい
る。また半導体(4)は各セル間にて互いに連結されて
いる・。また非活性領域において、セル(13)の上側
電極は、セル(11)の′F側電極と連結部(6)t(
7)でのコンタクト(18)で連結し、これを繰り返し
5つのセルを外部電極(8)4(9)間にて直列接続を
させている。As is clear from the correspondence between the longitudinal cross-sectional views taken along lines A-A' and B-B' in FIG. (13) is the transparent conductivity n' of the first electrode on the glass substrate (2) =
(CTF > (3) are separated from each other between each cell. Also, the semiconductors (4) are connected to each other between each cell. Also, in the non-active region, the upper electrode of the cell (13) , 'F side electrode of cell (11) and connection part (6) t(
7) is connected by the contact (18), and this is repeated to connect the five cells in series between the external electrodes (8) and 4 (9).
しかしこの従来構造は一見半導体(4)が1枚であるた
め製造歩留りが高いように見える。しかし実際には3種
類(第1の導電膜のパターニング用の第1のマスク、非
活性領域形成のための第2のマスク、第2の導電膜のパ
ターニング用の第3のマスク)のマスクを用いるが、そ
のマスクにおいて第1のマスクと第3のマスクとがセル
ファライン方式でないため、マスクずれを起こしやすい
。However, at first glance, this conventional structure appears to have a high manufacturing yield because there is only one semiconductor (4). However, in reality, three types of masks are used (a first mask for patterning the first conductive film, a second mask for forming a non-active region, and a third mask for patterning the second conductive film). However, since the first mask and the third mask are not of the self-line type, mask misalignment is likely to occur.
このずれ(即ち金属マスクにおいては0.3〜1mmの
ずれはごく当然である)により、セルの有効面積が10
〜20%も実質的に減少してしまうことが判明した。Due to this deviation (i.e., a deviation of 0.3 to 1 mm is quite natural for a metal mask), the effective area of the cell is reduced by 10 mm.
It was found that there was a substantial reduction of ~20%.
さらにマスクを用いるため、第1図(B)の活性領域で
の電極間の開溝であるアイソレイション領域(22)は
、0.2〜1mm例えば0.5 mmを有するため、セ
ル中を10mmとする時、2n+mずれるとするとセル
中(11)は8+nmとなり、アイソレイション中(2
2)は2.5mm となってしまい、20%近くも有効
面積が減少してしまう。またセルの外枠(10)の占め
る面積も5〜7%もある。Furthermore, since a mask is used, the isolation region (22), which is the opening between the electrodes in the active region of FIG. If the shift is 2n+m, the distance in the cell (11) will be 8+nm, and the distance in the isolation (2n+m) will be 8+nm.
2) becomes 2.5 mm, which reduces the effective area by nearly 20%. Further, the area occupied by the outer frame (10) of the cell is also 5 to 7%.
このため上下の電極の組合せをセルフレジストレイジョ
ン化することがその効率の向上のために強くめられてい
た。For this reason, it has been strongly recommended that the combination of upper and lower electrodes be made into a self-registration region in order to improve its efficiency.
また第1図の従来例においては、基板に非活性領域(1
5)が設けられ、この非活性領域は基板全体における2
0〜30%も占めてしまう。このためプロセス上の効率
が低くなり、ひいては製造コストの低下を図ることがで
きない。Furthermore, in the conventional example shown in FIG.
5) is provided, and this non-active region covers two parts of the entire substrate.
It accounts for 0-30%. For this reason, process efficiency decreases, and it is not possible to reduce manufacturing costs.
このため非活性領域が存在しない光電変換装置を作るこ
とがきわめて重要であった。For this reason, it is extremely important to create a photoelectric conversion device that does not have non-active regions.
さらに基板がガラス基板であるため、機械ストレスによ
り破mしやすい。このため基板として可曲性の厚さ50
〜200μの薄さの金属薄膜上に絶縁表面を有せしめる
ための叶を形成し、低価格化、耐機械破損防止を成就し
たものである。Furthermore, since the substrate is a glass substrate, it is easy to break due to mechanical stress. For this reason, the thickness of the flexible substrate is 50 mm.
A leaf for providing an insulating surface is formed on a metal thin film with a thickness of ~200μ, achieving low cost and resistance to mechanical damage.
即ち本発明においては、その代表例を第2図に示すが、
光照射(10)面側からは複数の第2の電極の分離用の
肉眼では見えない中の開溝(IIJIO〜70μ代表的
には20〜30μ)(第2図(20) )が存在するの
みである。さらに第1図(A)における領域(15)の
ごとき非活性領域がまったく存在せず、連結部が即ち各
セルのアイソレイション領域を構成せしめている。加え
てLSを用い、かっレーザ光を単に直線状に走査するの
みでのマスクレスプロセスである。ため、第1の開溝を
テレヒモニターで積Jiシて、その開溝を基準として所
定の位置に光学的にパターニングを行ういわゆるコンピ
ュータ・エイデツド・セルフレジストレイジョン方式を
採用することが可能になった。That is, in the present invention, a typical example is shown in FIG.
From the light irradiation (10) surface side, there are open grooves (IIJIO~70μ, typically 20~30μ) (Figure 2 (20)) that are invisible to the naked eye and are used to separate the plurality of second electrodes. Only. Further, there is no non-active region such as the region (15) in FIG. 1(A), and the connecting portion constitutes the isolation region of each cell. In addition, it is a maskless process that uses LS and simply scans the laser beam in a straight line. Therefore, it has become possible to adopt a so-called computer-aided self-registration method in which the first groove is formed using a television monitor and patterning is performed optically at a predetermined position using the first groove as a reference. .
また第1のセルの第1の電極と、第2のセルの第2の電
極との連結部のコンタクトは、基板の半導体「内部」
(この第2図では中央部)に設け、従来例の半導体の外
側でのコンタクトとはその位置がまったく異なる。Further, the contact at the connecting portion between the first electrode of the first cell and the second electrode of the second cell is located inside the semiconductor of the substrate.
The contact is provided at the center (in FIG. 2), and its position is completely different from that of the conventional contact on the outside of the semiconductor.
さらにこの内部コンタクトにより、透光性導電膜の光電
変換装置に与える直列抵抗を小さくできる。この結果、
連結部をセルの外側に設けなかったことにより、著しく
その自効面積の効率の向上を図ることができた。Furthermore, this internal contact can reduce the series resistance of the transparent conductive film applied to the photoelectric conversion device. As a result,
By not providing the connecting portion outside the cell, it was possible to significantly improve the efficiency of its effective area.
さらにこのコンタクトが隣合う′(・セル間の半導体を
すべて切断する構造で開講を作るのではなく、その開溝
(20〜90μφ)を1つまたは複数個不連続に円形状
または長円形状(開溝)に設げる(即ち、この開溝の端
部はそれぞれのセルを構成する半導体が連続している)
ことにより、この開講を実質的に肉眼で見い出し得す、
商品的にスクライブラインが目障りにならないようにで
きたという他の特長を有する。Furthermore, rather than creating an opening with a structure in which all the semiconductor between cells is cut off, one or more open grooves (20 to 90μφ) are discontinuously formed into a circular or elliptical shape ( (In other words, the ends of this open groove are continuous with the semiconductors that make up each cell.)
As a result, this opening can be practically seen with the naked eye.
Another feature of the product is that the scribe line does not become an eyesore.
またコンタクトが開孔であるため、その孔の側周辺のす
べての側面が第1の電極と第2の電極との連結部のコン
タクトを構成させることができ、この部分での接触抵抗
を3Ω以下に下げることができた。In addition, since the contact is an open hole, all the side surfaces around the hole can form the contact of the connecting part between the first electrode and the second electrode, and the contact resistance at this part can be kept below 3Ω. I was able to lower it to
本発明はかかる多(の特長を有するものであって、以下
に図面に従って°その詳細を記す。The present invention has many such features, and the details thereof will be described below with reference to the drawings.
第2図は本発明の光電変換装置の製造工程および装置を
示すものである。FIG. 2 shows the manufacturing process and apparatus of the photoelectric conversion device of the present invention.
図面において、Plさ100μのステンレス薄膜(2′
)上にポリイミド樹脂または+145 (住人ヘークラ
イト社型スミライト)(連続使用温度150〜300℃
、熱伝導率 3−7 Xl0)Cal /sec /c
rA/’C/cm)(2つを1〜lOμの厚さに形−成
し、これをして絶縁表面を有する基板(2)(例えば厚
さ100μ、長さく図面では左右方向) 60cm、1
1120cm)として用いた。In the drawing, a stainless steel thin film (2'
) on top of polyimide resin or +145 (Sumilite, type of Sumilite Co., Ltd.) (continuous use temperature 150-300℃)
, thermal conductivity 3-7 Xl0) Cal /sec /c
rA/'C/cm) (two pieces are formed to a thickness of 1 to lOμ, and then a substrate (2) having an insulating surface (for example, thickness 100μ, length in the horizontal direction in the drawing) 60cm, 1
1120cm).
この針上に電子ビーム蒸′4法またはマグネトスパッタ
法にて耐熱性を有し、かつ昇華性を有する金属であるク
ロム(厚さ2000人)または反射性金属であるアルミ
ニューム(1000人)とその上にスパッタ法にてSn
Oを1100人の厚さに形成させ、知合の導電性薄膜を
用いた。するとそのソート抵抗は3.5Ω/口を有して
いた。Chromium (thickness: 2000 mm), which is a metal with heat resistance and sublimation property, or aluminum (thickness: 1000 mm), which is a reflective metal, is coated on this needle by electron beam evaporation or magneto sputtering. On top of that, Sn is applied by sputtering method.
A known conductive thin film was used. The sort resistance then had 3.5 Ω/port.
この図面は4つのセルを直列接続せしめた場合である。This drawing shows a case where four cells are connected in series.
即ち本発明の光電変換装置は、活性領域(14)を同一
基板に100〜2000ケ同時に有するより大きい20
cm X 60cm(7)基体を用いた。That is, the photoelectric conversion device of the present invention has a larger 20 to 2000 active regions (14) on the same substrate.
A cm x 60 cm (7) substrate was used.
各セルでは、第1の導電膜を基体全面に形成した。さら
にこの導電膜を所定の形状にし〜ザ(ここでは1.06
μまたは0.53μの波長のYAG レーザ)スクライ
ブをマイクロコンピュータにより記憶され制御されたバ
クーンに従って行って第1の開講(16)を形成した。In each cell, a first conductive film was formed over the entire surface of the base. Furthermore, this conductive film is shaped into a predetermined shape (here, 1.06
A first opening (16) was formed by scribing (YAG laser) with a wavelength of .mu. or 0.53 .mu. according to a vacuum stored and controlled by a microcomputer.
さらにセルの外側でのリークを除去するため、分別用開
溝(2G>、(26’>を形成させた。そしてセル領域
(11人(13)および外部接続用電極部(8>、<
9 )を形成させた。Furthermore, in order to eliminate leakage outside the cell, separation grooves (2G>, (26'>) were formed. Then, the cell area (11 people (13)) and the external connection electrode part (8>, <
9) was formed.
即ち、ここにYAG レーザ(発光波長0.53μ、焦
点距離50mm、光(¥20μ)を照射した。その条件
として、繰り返し同時に(iKllz、平均出力0.2
W、スキャンスピード(走査速度、以下SSという)
30cm/分とした。That is, a YAG laser (emission wavelength 0.53μ, focal length 50mm, light (¥20μ) was irradiated here.The conditions were to repeatedly and simultaneously (iKllz, average output 0.2
W, scan speed (scan speed, hereinafter referred to as SS)
The speed was set at 30 cm/min.
スクライビングにより形成された開?t!1(16)は
巾約25μ、長さ20cm (図面では1 cm)、深
さは針上それぞれの第1の電極を完全に切断分離した。Opening formed by scribing? T! 1 (16) had a width of about 25 μm, a length of 20 cm (1 cm in the drawing), and a depth where each first electrode on the needle was completely cut and separated.
第1の素子(11)および第2の素子(13)を構成す
る中は10mmとした。The diameter of the first element (11) and the second element (13) was 10 mm.
この時電子顕微鏡にて調べた範囲では、畦表面には何等
のtn傷もまた部分的な劣化も見られなかった。このレ
ーザ光は1600℃以上の温度を有すると推察されるが
、連続使用上限温度が180°C程度の低い耐熱性しか
有さない叶に何等損傷を与えなかった。At this time, when examined using an electron microscope, no tn scratches or local deterioration were observed on the ridge surface. Although this laser beam is estimated to have a temperature of 1,600°C or higher, it did not cause any damage to the leaf, which has a low heat resistance with an upper limit for continuous use of about 180°C.
即ち、01+上のCFに対し、選択的に開溝(16)を
作製することができることがわかった。その上、2つの
プローブ間にはIMΩ以上の抵抗(中は1cmとする)
を得ることができた。In other words, it was found that the open groove (16) could be selectively created for the CF on 01+. Moreover, there is a resistance of IMΩ or more between the two probes (the inside is 1cm).
I was able to get
第3図はレーザ光の繰り返し周波数をaJ変にしたもの
で、開溝が形成される場合の電気抵抗を示す。FIG. 3 shows the electrical resistance when an open groove is formed, with the repetition frequency of the laser beam changed to aJ.
M面において、スキャンスピード30cm/分、平均出
力0.21光径25μのYAG (波長0.53μ)レ
ーザを用いた。するとその周波数を】υ旧1zより士げ
てゆくと、曲線(45)は7Kllz以下で不連続にI
MΩ以上(45’)となって電気的にアイソレイション
を行うことができるようになったことが判明した。In the M plane, a YAG (wavelength: 0.53 μm) laser with a scanning speed of 30 cm/min and an average output of 0.21 and a light diameter of 25 μm was used. Then, when the frequency is lowered from ]υold 1z, the curve (45) becomes I discontinuously below 7Kllz.
It was found that it became possible to electrically isolate the resistance at MΩ or more (45').
しかしこの周波数が4KIIzE下ではこのCFに加え
て下地のOFをもその中心部(ガウス分布のエネルギ密
度の最も高い領域)でto傷してしまった。However, when this frequency was 4KIIzE, in addition to this CF, the underlying OF was also damaged at its center (the region where the energy density of the Gaussian distribution was highest).
このことにより、針上のCFのLS (レーザスクライ
ブ)には(44)に示す範囲が通していた。As a result, the range shown in (44) was passed through the LS (laser scribe) of the CF on the needle.
さらに、この下地のOFlこtn(IAを与えることな
く導電性薄膜のみを除去する領域を調べたところ、第4
図を得た。Furthermore, when we investigated the area where only the conductive thin film was removed without applying IA, we found that the fourth
I got the diagram.
即ち、SSを0〜120cmZ分、平均出力0〜0.5
tV、繰り返し周波数6KIIz、波長0253μ、レ
ーザ光の直i¥21μのYAG レーザとすると、領域
(49)即ち点A、B、C,D、E、Fで囲まれる範囲
はOFの損傷がなく金属を一部または全部にをする薄膜
(CF)を選択的に除去することができた。That is, the SS is 0 to 120 cmZ, the average output is 0 to 0.5
Assuming a YAG laser with tV, repetition frequency 6KIIz, wavelength 0253μ, and laser beam directivity ¥21μ, the region (49), that is, the range surrounded by points A, B, C, D, E, and F, is a metal without damage to the OF. It was possible to selectively remove part or all of the thin film (CF) containing the CF.
さらに領域(47)ばこの薄膜ずらも除去することがで
きない領域であり、領域(46)はパルス光が01・上
で連続せず、また残存物を多量に開講に残してしまった
。領域(48)はC’TFのみならず下地の叶に対して
も損傷を与えてしまった領域であった。Further, the area (47) is an area in which the thin film shift of the tobacco cannot be removed, and in the area (46), the pulsed light is not continuous above 01. Furthermore, a large amount of residue remains in the area. Area (48) was an area where damage was caused not only to the C'TF but also to the underlying leaf.
このことにより下地のOFに対して損傷を与えることな
く、CFのみを選択的に開溝として除去することのでき
る領域(19)があることがわかった。This revealed that there is a region (19) where only the CF can be selectively removed as an open groove without damaging the underlying OF.
第2図(A)の平面図またA−A’、F−F”における
縦断面図を(A−IO(A−2)にそれぞれ示す。A plan view of FIG. 2(A) and longitudinal sectional views along lines AA' and FF'' are shown in (A-IO(A-2)), respectively.
次に第2図(B)の平面図に示すごとく、光擦躬により
光起電力を発生ずる水素または弗素が添加された非単結
晶半導体を、この電極(3)、開講(16)のすべての
上面に均質の膜厚に形成させる。Next, as shown in the plan view of Fig. 2 (B), a non-single crystal semiconductor doped with hydrogen or fluorine that generates photovoltaic force by light friction is connected to all electrodes (3) and (16). A uniform film thickness is formed on the upper surface of the film.
この半導体(4)は例えば5ixC+−x (0〈X
< 1一般にはx =0.7〜0.8 )のP型を約1
50人の厚さに、さらに1型の水素またはハロゲン元素
が添加された珪素を主成分とする半導体を0.4〜0.
8μの厚さに、さらにN型の微結晶化した珪素またはN
型のSixC1−x (0< x < 1 x 〜0.
9 )を主成分とする半導体の門N接合構造とした。も
らろんこれをP (SixC1−x x=0.7〜0.
8 ) I (Si)−N (、UCSi ) P (
SixC+−x x=0.7〜0.8 )−I (Si
xGe l−X X =0.6〜0.8 ) −N (
微結晶化(iisi または5ixC1−XO<x<1
)といった自NPIN構造のタンデム構造としてもよい
。This semiconductor (4) is, for example, 5ixC+-x (0<X
< 1 In general, the P type with x = 0.7 to 0.8) is about 1
A semiconductor whose main component is silicon to which type 1 hydrogen or halogen element is added is 0.4 to 0.50 mm thick.
In addition to the 8μ thickness, N-type microcrystalline silicon or N
SixC1-x (0< x < 1 x ~ 0.
9) was used as a gate-N junction structure of a semiconductor whose main component is P (SixC1-x x=0.7~0.
8) I (Si)-N (, UCSi) P (
SixC+-x x=0.7~0.8 )-I (Si
xGel-XX=0.6~0.8)-N(
Microcrystallization (iisi or 5ixC1-XO<x<1
) may be a tandem structure of the own NPIN structure.
さらに第2の開孔(15)をレーザ光により形成させ、
第2図(B)におけるB−B’ 、(、−C’の縦断面
図を(B−1)、(B−2)に対応して示している。Furthermore, a second aperture (15) is formed using a laser beam,
Vertical cross-sectional views of lines BB', (, -C' in FIG. 2(B) are shown corresponding to (B-1) and (B-2).
かくして第2の開化(■5)は叶の表面にはti傷を与
えずに第1の電極の側面(17)を露出させた。Thus, the second clarification (■5) exposed the side surface (17) of the first electrode without causing any scratches on the surface of the leaf.
この時、導電性薄膜の」二端部をO〜5μのIで露呈さ
セる結果、連結は導電性薄膜(3)の側面および上面が
連結部のコンタクトを構成した。また出力を少なくする
とレーザ光の0.53μの波長は珪素の高い吸収係数の
ため珪素のみを除去することができる。この場合は上面
のコンタクトとすることができる。At this time, the two ends of the conductive thin film were exposed with an I of 0 to 5 μm, so that the side and top surfaces of the conductive thin film (3) formed contacts of the connecting portion. Furthermore, if the output is reduced, only silicon can be removed because the wavelength of 0.53 μ of the laser beam has a high absorption coefficient of silicon. In this case, the contact can be made on the top surface.
この第2の開孔(15)の形成条件は、第1の開溝を形
成する条件とレーザ光をパルスを不連続に(15)の位
置のみに加える以外は同一である。即も、半導体の存在
は実質的に無視しても差支えなく、第3図、第4図の特
性を用いることができた。The conditions for forming the second opening (15) are the same as the conditions for forming the first opening groove, except that pulses of laser light are discontinuously applied only to the position (15). For now, the presence of the semiconductor can be virtually ignored, and the characteristics shown in FIGS. 3 and 4 can be used.
次に第2図(C)のパターンを形成させた。第2図(C
)のD−D’ 、 E−E’ 、 G−G’に対応した
縦断面図を(C−2)、(C−3>、< C−1)に示
している。Next, the pattern shown in FIG. 2(C) was formed. Figure 2 (C
) are shown in (C-2), (C-3>, <C-1).
即ち、半導体(4)上に第2の電極を電子ビーム蒸着法
によりITOを400〜1000人例えば700人のI
!J:さに形成させた。That is, a second electrode is formed on the semiconductor (4) by electron beam evaporation using ITO by 400 to 1,000 people, for example, 700 people.
! J: It was made to form.
すると、開口(15)において、第1の導電膜(3)の
側面または上面(17)に対し、ITOの導電性酸化物
がコンタクトし、オーム接触をさせることができた。Then, the conductive oxide of ITO came into contact with the side surface or top surface (17) of the first conductive film (3) at the opening (15), making ohmic contact possible.
このコンタクトは第1の電極を構成する連成として酸化
して絶縁膜を作りやすい。アルミニュームのみではコン
タクト部で長期使用においてアルミナが形成され、その
接触抵抗が30Ω以上となり好ましくなかった。このた
めアルミニュームを用いる場合に必ずその上面に酸化物
である酸化スズまたはITOが必要である。かかるため
、第2の電極を構成するITOを酸化物としてコンタク
トを構成するため、長期使用に対し接触抵抗は30以下
で変化がなく、好ましかった。さらに他の構造としては
、第1の電極を耐熱性のクロム、ステンレス等の酸化物
絶縁物を作らない金泥が用いられた。This contact is easily oxidized to form an insulating film as a compound constituting the first electrode. If only aluminum was used, alumina would be formed in the contact portion during long-term use, resulting in a contact resistance of 30Ω or more, which was undesirable. For this reason, when aluminum is used, an oxide such as tin oxide or ITO is always required on its upper surface. Therefore, since the contact is formed by using ITO, which forms the second electrode, as an oxide, the contact resistance is 30 or less and does not change during long-term use, which is preferable. In yet another structure, the first electrode was made of heat-resistant chromium, stainless steel, or other gold mud that does not contain oxide insulators.
特にレーザ加工にはクロムが接触抵抗も少なく、かつレ
ーザ加工性に優れ、好ましかった。In particular, chromium was preferable for laser processing because it has low contact resistance and excellent laser processability.
さらに第2の電極がITOのみよりなるため、レーザ光
が透過し、第3の開溝はITOとその下の半導体とを実
質的にスクライブしてしまった。Furthermore, since the second electrode was made only of ITO, the laser light was transmitted through it, and the third groove substantially scribed the ITO and the semiconductor underneath.
この後、第2図(C)においてレーザスクライブ(19
)を行った。これはYAG レーザ(tgL長0.53
μ)をテレビモニターにて第1の開溝をモニターしつつ
、それより50〜200μ第2のセル側(13)にはい
った位置にて開溝を作った。レーザ光の平均出力0.1
〜0.鵠とし、ビーム径10〜30μφ、ビーム走査ス
ピード0.1 =1m/分、一般には0.3m/めで大
きい0.6μ以下の波長即ち0.53μのQ−スイッチ
がかけられたレーザ光が特に優れていた。After this, the laser scribe (19
) was carried out. This is a YAG laser (tgL length 0.53
While monitoring the first groove (μ) on a television monitor, an open groove was created at a position 50 to 200μ deeper into the second cell side (13). Average output of laser light 0.1
~0. Q-switched laser beams with a beam diameter of 10 to 30 μΦ, a beam scanning speed of 0.1 = 1 m/min, generally 0.3 m/m, and a wavelength of 0.6 μ or less, that is, 0.53 μ, are particularly effective. It was excellent.
かくするとSi (水素またはハロゲン元素が添加され
た0、5μ以上の厚さを有する半導体)が本来昇華性で
あり、かつ0.53μの波長の吸収係数が大きいためレ
ーザ光により速やかに昇温し、半導体とその上のITO
とを同時に気化して除去させることができた。In this way, Si (semiconductor with a thickness of 0.5μ or more to which hydrogen or halogen elements are added) is inherently sublimable and has a large absorption coefficient at a wavelength of 0.53μ, so it can be rapidly heated by laser light. , semiconductor and ITO on it
could be vaporized and removed at the same time.
かくして、連結部(12)において、セル(13)の第
1の電極(23’)と、セル(11)の第2の電極(2
5)とが酸化物コンタクトによりオーム接触を第2の開
溝(18)を介してしている。特に連結部(12)にお
けるコンタクl−(17)は、第2の開化(15)によ
り作られた第1の電極の側面または側面と0〜5μの中
の第1の電極の上端面とで成就され、いわゆるサイトコ
ンタクト構造をイJしている。即も2つのセルはわずか
10〜70μφの第2の開化のサイI−コンククi−で
1−分であり、この部分に第2の電極を構成する祠料を
密接させて電気的に直列接続をさせている。(C−1>
、< C−2)の縦W1面図より明らかなごとく、半導
体(4)上に第2の電極(5)が形成されているにすぎ
ない。Thus, in the connecting part (12), the first electrode (23') of the cell (13) and the second electrode (23') of the cell (11)
5) is in ohmic contact with an oxide contact through the second open groove (18). In particular, the contact l-(17) in the connecting part (12) is formed by the side surface or side surface of the first electrode made by the second opening (15) and the upper end surface of the first electrode within 0 to 5μ. This has been accomplished, creating the so-called site contact structure. Immediately, the two cells are electrically connected in series by bringing the abrasive material constituting the second electrode into close contact with this part. I'm letting you do that. (C-1>
, <C-2), the second electrode (5) is simply formed on the semiconductor (4).
そしてこの第3の開溝(20)はその下の半導体とを除
去し、開溝を設け、さらに第1の電極をえくることな(
各素子の第2の電極間を電気的にアイソレイトさせるこ
とができた。The third trench (20) is formed by removing the underlying semiconductor, forming an trench, and then removing the first electrode (20).
It was possible to electrically isolate the second electrodes of each element.
さらにff12図(C)において、これらの上面に透光
性有機樹脂(28)を2Pプロセス(特に昇温させるこ
となく紫外光により硬化する液体を用いて透光性絶縁膜
をはりつりるプロセス)によりコーティングして完成さ
せている。Furthermore, in Fig. ff12 (C), a translucent organic resin (28) is applied to these upper surfaces using a 2P process (a process in which a translucent insulating film is attached using a liquid that is cured by ultraviolet light without raising the temperature). It is completed by coating.
その結果、1cm X5cmの光電変換装置を金属薄膜
上の絶縁表面を有する針上に1つ作るのではなく 、2
0cmx20cmまたは20cm X 60cmまたは
40cm X 40cmの大きな基板上に一度に多数の
光電変換装置を作ることがβJ能とな−、た。As a result, instead of making one 1 cm x 5 cm photovoltaic device on a needle with an insulating surface on a thin metal film, two
It was possible to fabricate a large number of photoelectric conversion devices at once on a large substrate of 0 cm x 20 cm, 20 cm x 60 cm, or 40 cm x 40 cm.
そして最後にこれらを(70)の境界で裁IIi法によ
り切L41iL、それぞれの光電変換装置Gこした。こ
のためには、従来より知られた光電変換装置のごとく活
性領域と非活性領域とを作るのではなく、すべて実質的
に活性領域とし、かつレーザ光による開溝をα1111
から端まで作り、レーザ光の走査スビー1′を大きなO
F上で當に一定にさせていることが重要である。さもな
いと、SSが遅い部分では叶に損傷がおきてしまうから
である。Finally, these were cut L41iL at the boundary (70) by the method IIi, and each photoelectric conversion device G was cut. For this purpose, instead of creating an active region and a non-active region as in conventionally known photoelectric conversion devices, it is necessary to make the entire active region substantially, and to open the grooves by laser light into α1111
from the end to the end, and set the scanning beam 1' of the laser beam to a large O.
It is important to keep it constant on F. Otherwise, the leaves will be damaged in the parts where the SS is slow.
第2図(C)での開溝(20)、(27)、<27 ’
)がα1111から端まで直線状走査されているのは、
v産性を考えた時車間である。特にレーザ光の装置のし
始め、し終わりの走査スピードの変化している領域では
照射部におIJるエネルギ密度が人きくな−、でしまう
。このため一定速度領域のみを用いζLSを行うことが
必要となり、そのため、直線的なしSによる開溝形成は
きわめて重要なプロセスである。もらろんこれらの開溝
は入射光側からはま−2た(見られないため、tl」商
晶価値化を妨げない。Open grooves (20), (27), <27' in Figure 2 (C)
) is linearly scanned from α1111 to the end because
This is the time-to-vehicle distance considering productivity. Particularly in areas where the scanning speed at the beginning and end of the laser beam device changes, the energy density applied to the irradiation section becomes unsatisfactory. For this reason, it is necessary to perform ζLS using only a constant speed region, and therefore, forming grooves in a linear manner by S is an extremely important process. Of course, these grooves cannot be seen from the incident light side, so they do not hinder commercial value.
また第2図(C)において明らかなごとく、セルの有効
面積は連結部(12)のlO〜300 μ中のきわめて
わJ゛かな部分を除いて他のすm:でが自助であり、実
りJ面積は92%以上を得ることかでき、従来例の80
%に比べ不発ツ]構造は格段に優れたものであった。Also, as is clear in Fig. 2 (C), the effective area of the cell is large, except for a very odd part of the connecting part (12) between 10 and 300 μm; It is possible to obtain J area of 92% or more, which is 80% of the conventional example.
%] The structure was much superior.
これらのことを考慮すると、本発明は以ト″の大きな特
長を有することが判明した。Taking these things into consideration, it has been found that the present invention has the following major features.
即ち、本発明は(1)絶縁表面をfrする大面積基板に
同時に多数の光電変換装置を作り、これを分割して各基
板上に1つの光電変換装置を作る方式を採用することが
i=J能となった。このため、従来の1/3〜115の
価格での製造がIJ能である。That is, the present invention adopts a method (1) to simultaneously fabricate a large number of photoelectric conversion devices on a large-area substrate with an insulating surface fr, and to divide the photoelectric conversion devices into one photoelectric conversion device on each substrate. It became J-Noh. Therefore, it is possible to manufacture the IJ at a price of 1/3 to 115 that of the conventional method.
〔2〕第1の開溝と第2の開孔、第3の開溝とがコンピ
ュータにより制御されたセルフレシストレインヨン方式
のため、セルの有効面積が大きく、かつその間−ハノチ
で作られた各光電変換装置間のバラツキが少ない〔3〕
直線走査方式のLSによるマスクレス工程であるため、
製造歩留りがIJい〔4〕各セル間分別の第1、第3の
開溝のスクライブラインの中が10〜70μときわめて
小さく、かつ第2の開(’Lも10〜50μψときわめ
て小さく、また第1の開溝は光照射面側からはま−2た
く見えない。その結果肉眼によりハイブリノ1−化がさ
れていることを確認され得す、尚付加前品(IllI値
を与えることができた。[2] Since the first opening groove, the second opening groove, and the third opening groove are self-resisting rain type controlled by a computer, the effective area of the cell is large, and the area between them is made of Hanochi. There is little variation between each photoelectric conversion device [3]
Because it is a maskless process using linear scanning LS,
The manufacturing yield is low [4] The inside of the scribe line of the first and third opening grooves for separation between each cell is extremely small at 10 to 70μ, and the second opening ('L is also extremely small at 10 to 50μψ, In addition, the first groove is not clearly visible from the light irradiation surface side.As a result, it can be confirmed with the naked eye that hybridization has been performed. did it.
第2図において、第2の開イしく15)は1つのみを半
導体内部の特に中央付近に存在させた。しかしこの開孔
は、複数ケ(2〜4ケ)を破線的にまたは長円構造をさ
せY方向に第1および第3の開溝の間に作製しても、ま
た櫛目形状に半導体(3)の内部に第1の開溝(16)
にそって形成させてもよい。In FIG. 2, only one second opening 15) is present inside the semiconductor, particularly near the center. However, even if a plurality of holes (2 to 4 holes) are formed in a broken line or elliptical structure between the first and third grooves in the Y direction, or in a comb-shaped semiconductor (3 holes) ) inside the first open groove (16)
It may be formed along the
以上の説明は本発明の第2図のパターンには限定されな
い。セルの数、大きさはその設a1仕様によって定めら
れるものである。また半導体はプラズマCVD法、減圧
CVD法、光CVD法または光プラズマCVD法を用い
た。The above description is not limited to the pattern of FIG. 2 of the present invention. The number and size of cells are determined by the A1 specifications. Further, for the semiconductor, a plasma CVD method, a low pressure CVD method, a photo CVD method, or a photo plasma CVD method was used.
非単結晶シリコンを主成分とするPIN接合、ヘテロ接
合、クンデム接合のめに限らず多くの構造への応用が可
能である。Applications are possible not only to PIN junctions, heterojunctions, and Kundem junctions, but also to many structures whose main component is non-single-crystal silicon.
なお本発明は有機樹脂上に集積化さ一已た構造を示した
。しかし本発明は、金属薄股上に窒化珪素、酸化珪素ま
たは酸化クロム等の絶縁膜を300〜3000人の厚さ
にバリア1−として形成し、または基体自体が絶縁表面
(非透光性でよい)であってその上に第1の電極用の導
電性薄膜を形成してもよいことはいうまでもない。Note that the present invention shows a slightly integrated structure on an organic resin. However, in the present invention, an insulating film of silicon nitride, silicon oxide, chromium oxide, etc. is formed on a thin metal layer to a thickness of 300 to 3,000 mm as a barrier 1-, or the substrate itself has an insulating surface (which may be non-transparent). ), and it goes without saying that a conductive thin film for the first electrode may be formed thereon.
第1図は従来の光電変換装置の縦断面図である。
第2図は本発明の光電変換装置の平面図および縦断面図
を製造工程に従って示したものである。
第3図は本発明のステンレス草根上の有機樹脂上の導電
性薄膜をレーザスクライブした時のレーザスクライブに
よる電気抵抗の変化を示す。
第4図は本発明の有機樹脂表面上に導電性薄膜を設け、
この薄膜にレーザスフライフした時のレーザスクライブ
の可能な領域を示す。
特許出願人
輩//辺
2MFIG. 1 is a longitudinal sectional view of a conventional photoelectric conversion device. FIG. 2 shows a plan view and a longitudinal sectional view of the photoelectric conversion device of the present invention according to the manufacturing process. FIG. 3 shows the change in electrical resistance caused by laser scribing when the conductive thin film on the organic resin on the stainless steel base of the present invention was laser scribed. FIG. 4 shows that a conductive thin film is provided on the surface of the organic resin of the present invention,
The area where laser scribing is possible when this thin film is fly-fried with a laser is shown. Patent applicant//side 2M
Claims (1)
電極、該第1の電極および該電極間の開溝上に設けられ
た光照射により光起電力を発生させる非単結晶半導体、
およびiiI記第1の電極に対応して前記半導体上に設
けられた複数−0)第2の電極とを有する複数の光電変
換素子を備え、隣合う素子の第1および第2の電極は前
記非単結晶半導体内部に設けられた開孔または開溝によ
り電気的に直列に連結した連結部を有することを特徴と
する光電変換半導体装置。 2、絶縁表面を自する基板上に配列された反射性金属電
極と該電極上の酸化物導電膜とよりなる複数の第1の電
極、該第1の電極および該電極間の開溝上に設けられた
光照射により光起電力を発生させる非単結晶半導体、お
よび前記第1の電極に対応して前記半導体上に設けられ
た透光性酸化物導電膜とよりなる複数の第2の電極とを
有する複数の光電変換素子を備え、隣合う素子の第1お
よび第2の電極は前記非単結晶半導体内部に設げられた
開孔またば開溝にて酸化物導電膜同志により電気的に連
結した連結部を有することを特徴とする光電変換半導体
装置。 3、特許請求の範囲第1項または第2項において、連結
部は非単結晶半導体に設けられた開孔または開溝と前記
開孔または開溝下の絶縁物表面を露呈して概略同一形状
の開孔または開溝が第1の導電性電極に設けられ、該第
1の電極の上部、側部または側部と上部とに第2の電極
を構成する導電性酸化物材料が密接して設けられたこと
を特徴とする光電変換半導体装置。[Claims] (1) A plurality of first electrodes arranged on a substrate having an insulating surface, a photovoltaic force generated by light irradiation provided on the first electrodes and the grooves between the electrodes. non-single crystal semiconductor,
and iii) a plurality of photoelectric conversion elements having a plurality of second electrodes provided on the semiconductor in correspondence with the first electrode, and the first and second electrodes of adjacent elements are 1. A photoelectric conversion semiconductor device comprising a connecting portion electrically connected in series by an opening or a groove provided inside a non-single crystal semiconductor. 2. A plurality of first electrodes consisting of reflective metal electrodes arranged on a substrate having an insulating surface and an oxide conductive film on the electrodes, on the first electrodes and the grooves between the electrodes; a plurality of second electrodes comprising a non-single crystal semiconductor that generates a photovoltaic force when irradiated with light; and a transparent oxide conductive film provided on the semiconductor in correspondence with the first electrode; The first and second electrodes of adjacent elements are electrically connected to each other by oxide conductive films through openings or grooves provided inside the non-single crystal semiconductor. A photoelectric conversion semiconductor device characterized by having a connecting portion connected to. 3. In claim 1 or 2, the connecting portion has an opening or an opening provided in the non-single crystal semiconductor and a surface of the insulator under the opening or opening is exposed and has approximately the same shape. a hole or groove is provided in the first conductive electrode, and the conductive oxide material constituting the second electrode is in close contact with the upper part, the side part, or the side part and the upper part of the first electrode. A photoelectric conversion semiconductor device characterized by being provided.
Priority Applications (11)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59057713A JPH065775B2 (en) | 1984-03-26 | 1984-03-26 | Photoelectric conversion semiconductor device |
| US06/630,063 US4594471A (en) | 1983-07-13 | 1984-07-12 | Photoelectric conversion device |
| EP84304808A EP0134669B1 (en) | 1983-07-13 | 1984-07-13 | Photoelectric conversion device and its manufacturing method |
| DE8484304808T DE3470819D1 (en) | 1983-07-13 | 1984-07-13 | Photoelectric conversion device and its manufacturing method |
| GB08417904A GB2146173B (en) | 1983-07-13 | 1984-07-13 | Photoelectric conversion device and manufacture thereof |
| KR1019840004120A KR900005126B1 (en) | 1983-07-13 | 1984-07-13 | Photoelectric conversion device and manufacturing method thereof |
| US06/720,291 US4603470A (en) | 1983-07-13 | 1985-04-05 | Method of making plurality of series connected solar cells using multiple groove forming processes |
| US08/005,170 US5332680A (en) | 1983-07-12 | 1993-01-15 | Method of making photoelectric conversion device |
| US08/013,209 US5332450A (en) | 1983-07-13 | 1993-02-01 | Photoelectric conversion device |
| US08/222,954 US5500051A (en) | 1983-07-13 | 1994-04-05 | Photoelectric conversion device |
| US08/505,960 US5567249A (en) | 1983-07-13 | 1995-07-24 | Photoelectric conversion device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP59057713A JPH065775B2 (en) | 1984-03-26 | 1984-03-26 | Photoelectric conversion semiconductor device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60200577A true JPS60200577A (en) | 1985-10-11 |
| JPH065775B2 JPH065775B2 (en) | 1994-01-19 |
Family
ID=13063584
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP59057713A Expired - Lifetime JPH065775B2 (en) | 1983-07-12 | 1984-03-26 | Photoelectric conversion semiconductor device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH065775B2 (en) |
Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6018973A (en) * | 1983-07-13 | 1985-01-31 | Semiconductor Energy Lab Co Ltd | Photoelectric conversion semiconductor device |
| JPS6095978A (en) * | 1983-10-31 | 1985-05-29 | Semiconductor Energy Lab Co Ltd | Photoelectric conversion semiconductor device |
| JPS60100481A (en) * | 1983-11-05 | 1985-06-04 | Semiconductor Energy Lab Co Ltd | Photoelectric converting semiconductor device |
-
1984
- 1984-03-26 JP JP59057713A patent/JPH065775B2/en not_active Expired - Lifetime
Patent Citations (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6018973A (en) * | 1983-07-13 | 1985-01-31 | Semiconductor Energy Lab Co Ltd | Photoelectric conversion semiconductor device |
| JPS6095978A (en) * | 1983-10-31 | 1985-05-29 | Semiconductor Energy Lab Co Ltd | Photoelectric conversion semiconductor device |
| JPS60100481A (en) * | 1983-11-05 | 1985-06-04 | Semiconductor Energy Lab Co Ltd | Photoelectric converting semiconductor device |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH065775B2 (en) | 1994-01-19 |
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| EXPY | Cancellation because of completion of term |