JPH01181575A - Junction type photoelectric conversion device - Google Patents

Junction type photoelectric conversion device

Info

Publication number
JPH01181575A
JPH01181575A JP63004381A JP438188A JPH01181575A JP H01181575 A JPH01181575 A JP H01181575A JP 63004381 A JP63004381 A JP 63004381A JP 438188 A JP438188 A JP 438188A JP H01181575 A JPH01181575 A JP H01181575A
Authority
JP
Japan
Prior art keywords
layer
semiconductor substrate
thick layer
thin layer
thick
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
Application number
JP63004381A
Other languages
Japanese (ja)
Other versions
JPH0682852B2 (en
Inventor
Yutaka Hayashi
豊 林
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.)
National Institute of Advanced Industrial Science and Technology AIST
Original Assignee
Agency of Industrial Science and Technology
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 Agency of Industrial Science and Technology filed Critical Agency of Industrial Science and Technology
Priority to JP63004381A priority Critical patent/JPH0682852B2/en
Publication of JPH01181575A publication Critical patent/JPH01181575A/en
Publication of JPH0682852B2 publication Critical patent/JPH0682852B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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
    • Y02E10/547Monocrystalline silicon PV cells

Landscapes

  • Photovoltaic Devices (AREA)

Abstract

PURPOSE:To improve a physical strength and the photoelectric conversion characteristics by a method wherein thin layer parts whose thicknesses are thinner than the diffusion length of minority carriers emitting lights in a semiconductor substrate and thick layer parts which have physically sufficient strength are made to coexist and the widths of the thick layer parts are less than two times of the minority carrier diffusion length. CONSTITUTION:Relatively thin thin layer parts 11 and relatively thick thick layer parts 12 coexist in a semiconductor substrate 10. One thick layer part 12 is positioned between a pair of the thin layer parts 11 and 11 facing each other laterally. Each thin layer part 11 has a thickness (d) which is smaller than the diffusion length of minority carriers which emit lights at that part in the semiconductor. On the other hand, the thickness of each thick layer part 12 is larger than the thickness of the thin layer part 11 and large enough to support the device structure mechanically. Further, the dimension W of the thick layer part 12 along the direction parallel to the surface of the semiconductor substrate 10, i.e. the width W, is less than two times of the minority carrier diffusion length. With this constitution, the reciprocity between the photoelectric conversion characteristics and mechanical strength characteristics can be harmonized and a high efficiency can be obtained while a sufficient strength is maintained.

Description

【発明の詳細な説明】 〈産業上の利用分野) 本発明は、太陽電池等の接合型光電変換装置に関し、特
に、そうした装置素子の物理的な強度問題を生起するこ
となく、その開放起電圧V。Cを高め得るようにする改
良に関する。
[Detailed Description of the Invention] (Field of Industrial Application) The present invention relates to a junction type photoelectric conversion device such as a solar cell, and in particular, the present invention relates to a junction type photoelectric conversion device such as a solar cell, and in particular, the open-circuit electromotive voltage can be reduced without causing physical strength problems of such device elements. V. This invention relates to improvements that can increase C.

(従来の技術) 太陽電池等の接合型光電変換装置における開放起電圧V
。Cは、主として光を吸収する半導体層の厚さが、当該
光発生する少数キャリアの拡散長より薄くなると増大し
始め、表面再結合速度が小さければ、薄くなる程、大き
くなる。
(Prior art) Open-circuit electromotive voltage V in junction-type photoelectric conversion devices such as solar cells
. C begins to increase when the thickness of the semiconductor layer that primarily absorbs light becomes thinner than the diffusion length of the minority carriers generated by the light, and increases as the surface recombination rate decreases and becomes thinner.

しかし一般に、大面積の半導体結晶を、全体として上記
のように少数キャリアの拡散長等という極めて薄いオー
ダに作り、これをさらに素子までに加工することは、単
に機械的な強度だけを考えても不可能である。
However, in general, it is difficult to make a large-area semiconductor crystal as a whole into an extremely thin order, such as the diffusion length of minority carriers, as described above, and to further process it into a device, even when considering only mechanical strength. It's impossible.

そこで従来、実現可能な構造として提案されたのは、!
A種基板上に薄い半導体結晶層を成長させ、これを光電
変換機能層とするものである。
Therefore, what was previously proposed as a possible structure was !
A thin semiconductor crystal layer is grown on a type A substrate, and this is used as a photoelectric conversion functional layer.

(発明が解決しようとする問題点〉 しかし、上記従来の構造では、基板との結晶格子間隔の
不整合や熱膨張係数の差等が災いし、結晶欠陥や画を発
生し易く、さらにはまた、基板から結晶薄膜へ不純物が
拡散する等の不都合もあって、良質な半導体薄膜を得る
ことが実際には極めて難しく、薄膜化による光電変換特
性の向上という利点は生かされていなかった。
(Problems to be Solved by the Invention) However, the above-mentioned conventional structure suffers from mismatching of crystal lattice spacing with the substrate, difference in thermal expansion coefficient, etc., and tends to generate crystal defects and patterns. However, it is actually extremely difficult to obtain high-quality semiconductor thin films due to problems such as the diffusion of impurities from the substrate into the crystalline thin film, and the advantage of improved photoelectric conversion characteristics due to thinner films has not been utilized.

本発明はこうした点に鑑みて成されたもので、異種基板
上での結晶成長という技術を用いず、単一種の半導体基
板から構築することができ、それでいて物理的な脆弱性
の問題も生むことなく、光電変換特性の向上を図れる新
たな構成を提案せんとするものである。
The present invention has been made in view of these points, and it is possible to construct a semiconductor substrate from a single type of semiconductor substrate without using the technique of crystal growth on a different type of substrate, but it also creates the problem of physical fragility. Instead, we aim to propose a new configuration that can improve photoelectric conversion characteristics.

〈問題点を解決するための手段〉 本発明は上記目的を達成するため、 ■ 所定の面積を有する半導体基板を、その厚さに関し
、該半導体基板の内部で光発生する少数キャリアの拡散
長よりも薄い薄層部と、該薄層部よりも厚く、物理的に
十分な強度を有する厚層部との混在構造から成るように
加工し:■ 上記厚層部を、少なくとも隣合う一対の上
記薄層部間に位置させると共に: ■ 上記半導体基板の一方の表面に沿って上記少数キャ
リアを集める接合形成層を、また他方の表面に沿って上
記少数キャリアを追返す障壁形成層を設け、該接合形成
層か障壁形成層のあるどちらか一方の半導体表面を受光
面、該受光面に対向する他方の表面を反射層付きの反射
面とした上で; ■ 上記厚層部の幅を、上記少数キャリア拡散長の二倍
以下としたこと: を特徴とする接合型光電変換装置を提供する。
<Means for Solving the Problems> In order to achieve the above object, the present invention has the following features: Processed so that it has a mixed structure of a thin layer part and a thick layer part that is thicker than the thin layer part and has sufficient physical strength: and a junction forming layer that collects the minority carriers along one surface of the semiconductor substrate, and a barrier forming layer that repels the minority carriers along the other surface; Either the semiconductor surface with the junction forming layer or the barrier forming layer is used as a light-receiving surface, and the other surface opposite to the light-receiving surface is a reflective surface with a reflective layer; Provided is a junction-type photoelectric conversion device characterized in that the minority carrier diffusion length is less than or equal to twice the minority carrier diffusion length.

(作用および効果) 上記本発明の構成要素中において、半導体基板を薄層化
することで形成され、両表面の一方あてに沿ってそれぞ
れ光発生した少数キャリアを集める接合形成層と、自身
に向かって流れてくる少数キャリアを電気的に追返す障
壁形成層とを有する半導体薄層部は、その厚味が、ここ
の部分で光発生し得る少数キャリアの拡散長以下とされ
ているので、当該薄層部にて得られる開放起電圧は十分
高いものとなる。
(Operations and Effects) Among the above components of the present invention, there is a bonding layer formed by thinning the semiconductor substrate, which collects photogenerated minority carriers along one side of both surfaces, and a bonding layer that collects photogenerated minority carriers along one side of both surfaces. The thickness of the thin semiconductor layer is less than the diffusion length of the minority carriers that can be photogenerated in this part, so that The open circuit voltage obtained in the thin layer portion is sufficiently high.

そして、電気的に少数キャリアを接合形成層の側に追返
す障壁形成層は、まずこの薄層部だけに関しても、その
キャリア濃度自体を濃くする働きを有し、したがって、
単に少数キャリアの拡散長以下にこの薄層部を構成した
だけのときよりも、さらに−層、開放起電圧を向上し得
るものとなる。
The barrier forming layer that electrically repels minority carriers toward the junction forming layer has the function of increasing the carrier concentration itself even in this thin layer portion, and therefore,
The open-circuit electromotive force can be further improved than when the thin layer portion is simply configured to be shorter than the minority carrier diffusion length.

一方、こうした薄層部だけでは、到底、装置素子として
の機械的ないし物理的な強度は期待できないが、本発明
に従って構成された光電変換装置においては、隣合う薄
層部間に、装置素子全体として物理的に十分な強度を得
るために厚くされた(と言っても、一般には供給された
出発部材としての半導体基板の板厚そのものであって良
いが)厚層部があり、この問題を解決している。
On the other hand, such thin layer portions alone cannot be expected to have mechanical or physical strength as a device element, but in a photoelectric conversion device constructed according to the present invention, the entire device element is In order to obtain sufficient physical strength, there is a thick layer (although it can generally be the thickness of the semiconductor substrate as a supplied starting material), and this problem can be solved. It's resolved.

しかし、こうした厚層部自体°は、本来、開放起電圧を
低下させる傾向にあるから、単に上記のように厚層部を
設けただ°けでは、薄層部を設けたことによる光電変換
効率向上効果が大きく損われ、場合によっては何等の効
果を呈し得ないことも考えられる。
However, such thick layer parts themselves inherently tend to reduce the open-circuit electromotive force, so simply providing a thick layer part as described above does not improve the photoelectric conversion efficiency by providing a thin layer part. The effect may be greatly impaired, and in some cases, it may not be possible to exhibit any effect at all.

そこで本発明においては、さらにこの厚層部の幅に関し
、“少数キャリア拡散長の二倍以下”という重要な限定
を施し、そうした危惧を除いている。
Therefore, in the present invention, the width of this thick layer part is further limited to "less than twice the minority carrier diffusion length" to eliminate such concerns.

これは端的に言えば、厚層部の幅をその程度に留める限
り、少なくとも、当該厚層部の両側にある一対の薄層部
の一方の表面に沿って設けられている障壁形成層が、こ
の厚層部に対し、横方向からも作用し得るからである。
Simply put, as long as the width of the thick layer section is kept within that range, at least the barrier forming layer provided along the surface of one of the pair of thin layer sections on both sides of the thick layer section can be This is because it can also act on this thick layer portion from the lateral direction.

つまり、障壁形成層の存在による電気的なキャリア追返
し作用は、当該障壁形成層の端部から少数キャリア拡散
長の距離程度の部分であれば、単に上下方向に限らず、
横方向を含む全方向に及び得る。
In other words, the electrical carrier repulsion effect due to the presence of the barrier forming layer is not limited to the vertical direction, but only in the vertical direction, as long as the distance is about the minority carrier diffusion length from the edge of the barrier forming layer.
It can extend in all directions including the lateral direction.

したがって、各厚層部の幅を上記のように少数キャリア
拡散長の二倍以下として置けば、障壁形成層が横方向や
斜め上方向にもキャリア適過し機能を営む結果、厚層部
中においてもその中に存在し得る少数キャリアは、当該
障壁形成層部分の影響により、望ましい追返し作用を受
は得るのである。ただし、実施例によっては、厚層部自
体に備えられている障壁形成層が、より近い位置から直
接にキャリア適過し作用を発揮することもある。
Therefore, if the width of each thick layer is set to be less than twice the minority carrier diffusion length as described above, the barrier forming layer will function by allowing carriers to flow in the lateral and diagonal upward directions. Minority carriers that may exist therein also receive a desirable repulsion effect due to the influence of the barrier-forming layer portion. However, depending on the embodiment, the barrier forming layer provided in the thick layer part itself may exert its effect by directly passing through carriers from a closer position.

いずれにしろこのようにして、厚層部を設けたにもかか
わらず、その存在に基づく開放起電圧の低下は無視し得
る程度にでき、悪い場合ても、従来に比せば十分高い値
に維持し得る。
In any case, in this way, even though a thick layer is provided, the drop in open circuit voltage due to its presence can be ignored, and even in the worst case, it can be reduced to a sufficiently high value compared to the conventional one. Can be maintained.

結局、本発明の効果としてまとめれば、光電変換特性と
機械的強度特性との間に横たわる相反性を良く調和し、
十分に丈夫でありながら高効率の光電変換装置を提供し
得るもの、と言える。
In summary, the effects of the present invention can be summarized as: well harmonizing the contradiction between photoelectric conversion characteristics and mechanical strength characteristics;
It can be said that it is possible to provide a highly efficient photoelectric conversion device while being sufficiently durable.

また、これを逆に言えば、高効率効果を幾分か抑え目と
しても、それでなお十分である場合には、本発明装置に
用いる半導体材質は、従来よりも低品質なものであって
良いこともあり、これはこれで、現実的に極めて望まし
い効果となる。
Conversely, if the high efficiency effect is somewhat suppressed but still sufficient, the semiconductor material used in the device of the present invention may be of lower quality than conventional ones. In some cases, this is actually an extremely desirable effect.

(実 施 例) 第1図には、本発明に従って構成された一実施例である
接合型光電変換装置の要部断面構成が概略的に示されて
いる。
(Example) FIG. 1 schematically shows a cross-sectional configuration of a main part of a junction type photoelectric conversion device which is an example constructed according to the present invention.

図示の状態は素子完成状態であるから、もちろん、出発
材料として一般的な適当なる材質の半導体ウェハに対し
、すでに幾何的な形態加工を終えた状態で示しており、
当該半導体基板lOは、相対的に薄い薄層部11と相対
的に厚い厚層部12との混在状態となっており、特に、
本発明要旨に従い、厚層部12は、少なくとも横方向に
対向する一対の薄層部11.11間に位置している。
Since the state shown in the figure is a completed state of the device, it is of course shown in a state in which a semiconductor wafer made of a general appropriate material as a starting material has already been processed into a geometric shape.
The semiconductor substrate IO has a relatively thin thin layer portion 11 and a relatively thick thick layer portion 12 in a mixed state, and in particular,
In accordance with the subject matter of the invention, the thicker section 12 is located between at least a pair of laterally opposed thinner sections 11.11.

図示実施例においては、半導体基板10の図中、上方の
表面は一連に平らな面となっており、これとは反対側の
表面(裏面)が、薄層部11と厚層部12の厚味の差に
応じた凸凹な面となっている。
In the illustrated embodiment, the upper surface of the semiconductor substrate 10 in the drawing is a series of flat surfaces, and the opposite surface (back surface) has a thickness of the thin layer portion 11 and the thick layer portion 12. The surface is uneven to accommodate different tastes.

そして、各薄層部11は、その部分に右ける半導体内部
にて光発生した少数キャリアの拡散長よりも薄い厚さd
とされており、一方、厚層部12の厚さは、上記薄層部
11より厚いことはもちろん、機械的に図示の素子構造
を支持し得るように、十分な厚さに設定される。
Each thin layer portion 11 has a thickness d that is thinner than the diffusion length of minority carriers photogenerated inside the semiconductor in that portion.
On the other hand, the thickness of the thick layer portion 12 is not only thicker than the thin layer portion 11 but also set to a sufficient thickness so as to mechanically support the illustrated element structure.

しかし、本発明の趣旨に従い、この厚層部12の半導体
基板表面に平行な方向の寸法W、すなわち幅Wは、当該
少数キャリア拡散長の二倍以下の寸法とされている。
However, in accordance with the spirit of the present invention, the dimension W of the thick layer portion 12 in the direction parallel to the semiconductor substrate surface, that is, the width W, is set to be twice or less the minority carrier diffusion length.

本発明の光電変換装置においては、受光面は半導体基板
の二表面のいずれにも設定することができるが、ここに
示されている実施例では、図中で上方に位置する平らな
側の面としている。
In the photoelectric conversion device of the present invention, the light-receiving surface can be set on either of the two surfaces of the semiconductor substrate, but in the embodiment shown here, the light-receiving surface is set on the flat surface located above in the figure. It is said that

この表面側には、接合形成層13が設けられているが、
これは半導体基板lOと同一材料で、逆導電型の不純物
を含む薄層であっても良いし、半導体基板とは異なる材
料で、ペテロ接合を形成する関係にある材質製であって
も良い。
A bonding layer 13 is provided on this surface side,
This may be a thin layer made of the same material as the semiconductor substrate IO and containing impurities of the opposite conductivity type, or may be made of a material different from the semiconductor substrate and having a relationship to form a Peter junction.

要は、半導体基板lOの薄層部11にて光発生した少数
キャリアを集める機能を示せれば良く、場合によっては
光を透過し得る程度に薄い限り、この接合形成層13と
して適゛当なる金属層を選択することも可能である。
In short, it is sufficient to show the function of collecting minority carriers photogenerated in the thin layer portion 11 of the semiconductor substrate IO, and in some cases, any suitable metal may be used as the junction forming layer 13 as long as it is thin enough to transmit light. It is also possible to select layers.

図示の場合には、この接合形成層13の上にさらに、保
護膜を兼ねた反射防止膜31が設けられているが、これ
は必要に応じて設ければ良く、反射防止機能を営む層と
保護機能を営む層とを別個な層とし、多層構造にする等
しても良い。
In the case shown in the figure, an antireflection film 31 that also serves as a protective film is further provided on the bonding layer 13, but this may be provided as necessary, and may be used as a layer that performs an antireflection function. The layer that performs the protective function may be a separate layer, resulting in a multilayer structure.

なお、便宜的に、この接合形成層13のある方の半導体
基板表面を図示実施例の場合、そのままに″表面”と呼
び、他面側を“裏面”と呼ぶ。
For convenience, the surface of the semiconductor substrate on which the bonding layer 13 is located is simply referred to as the "front surface" in the illustrated embodiment, and the other surface is referred to as the "back surface".

半導体基板表面側にはまた、当該表面に沿って形成され
た接合形成層13に電気的な導通を採るための引き出し
端子14も適宜に設けられるが、特にこの場合は、厚層
部12の上に位置する個所に各設けられている。
On the surface side of the semiconductor substrate, a lead-out terminal 14 is also appropriately provided for establishing electrical continuity with the bonding layer 13 formed along the surface. Each location is located in the same location.

これは、光電変換特性的に最も優れた結果の得られる薄
層部11の面積部分をできるだけ有効利用し、至上、そ
の全面積部分を全て光の入射領域とし得るようにする意
味もあり、また、当該引き出し端子の製造工程後、これ
ら端子群に外部回路の接続を採る工程において、仮に大
きな外力が印加されることがあっても、機械的に強度の
高い厚層部12上であれば、これに少しでも良く抵抗し
得るようになるとの意図からでもある。
This also means that the area of the thin layer section 11 that provides the best results in terms of photoelectric conversion characteristics can be used as effectively as possible, and that the entire area can be used as the light incident area. Even if a large external force is applied in the process of connecting external circuits to these terminal groups after the manufacturing process of the extraction terminals, as long as the thick layer part 12 has high mechanical strength, This is also with the intention of being able to resist this as much as possible.

半導体基板10の裏面は、先に述べたように、薄層部1
1の部分の底と厚層部12の部分の底が連続することか
ら、結果として凸凹な面となるが、とにかくもこの裏面
に沿い(したがって同様に凸凹になるが)、障壁形成層
20が設けられている。
As mentioned earlier, the back surface of the semiconductor substrate 10 has the thin layer portion 1.
Since the bottom of the thick layer portion 12 is continuous with the bottom of the thick layer portion 12, the resulting surface is uneven, but the barrier forming layer 20 is formed along this back surface (therefore, it is also uneven). It is provided.

この障壁形成層20は、半導体基板lOと同一導電型で
、より高濃度な不純物層として形成されても良いし、異
種材料層であっても良い。
This barrier forming layer 20 may be formed as an impurity layer having the same conductivity type as the semiconductor substrate IO and having a higher concentration, or may be a layer of a different material.

この障壁形成層20についても、要は、薄層部llで発
生した少数キャリアに対して障壁を形成し、この層の側
に流れてくる少数キャリアを電気的に追返すような機能
が見込めれば良く、例えば薄層部11に対する異種材料
層としても、当該少数キャリアに対して障壁を形成し得
るように、薄層部11よりもさらにワイド・ギャップな
半導体または絶縁膜を選択することができる。
The barrier forming layer 20 is also expected to have the function of forming a barrier against the minority carriers generated in the thin layer section 11, and electrically repelling the minority carriers flowing toward this layer. For example, a semiconductor or insulating film with a wider gap than the thin layer portion 11 can be selected as a different material layer for the thin layer portion 11 so as to form a barrier against the minority carriers. .

特にこの障壁形成層20として、上記のように適当なる
絶縁膜を選択した場合には、この実施例でこれを覆うよ
うに設けられている保護層41は、当該絶縁膜自体で兼
用することもできる。
In particular, when a suitable insulating film is selected as the barrier forming layer 20 as described above, the protective layer 41 provided to cover it in this embodiment may also be used as the insulating film itself. can.

また、望ましくは設けられる保護層41の上には(と言
っても、図中ではさらに下方の位置になるが)、一般に
適当なる金属層で成る反射層42も設けられており、こ
の実施例ではやはり、端子14に関して述べたと同様の
理由で、厚層部12のある所でこの反射層42が保護層
41を貫通し、半導体基板lOに対する電気的接触部分
21を構成している。
Further, on the protective layer 41 which is desirably provided (although it is located further down in the figure), a reflective layer 42 generally made of a suitable metal layer is also provided, and this embodiment Again, for the same reason as stated regarding the terminal 14, the reflective layer 42 penetrates the protective layer 41 at a certain point in the thick layer portion 12 and constitutes an electrical contact portion 21 with respect to the semiconductor substrate IO.

このような構造において、本発明の有意性を考えて見る
と、半導体薄層部11の厚さdは、先に述べたように少
数キャリア拡散長よりも薄いので。
In such a structure, considering the significance of the present invention, the thickness d of the semiconductor thin layer portion 11 is thinner than the minority carrier diffusion length as described above.

この部分で発生する開放起電圧VOCは、望ましい程に
十分高くし得る。従来にあけるように、厚さの均一性を
保ったまま、機械的に耐え得る限界にまで、半導体基板
を葎<シて得られた光電変換装置に比しても、なお十分
に高い値となる。
The open circuit voltage VOC generated in this portion can be made sufficiently high as desired. Even compared to photoelectric conversion devices obtained by peeling a semiconductor substrate to its mechanically durable limit while maintaining uniformity of thickness, the value is still sufficiently high. Become.

換言すれば、従来の光電変換装置では、特に低品位の半
導体基板を使した場合、当該基板の全面積領域に関し、
その厚さを少数キャリア拡散長以下とすること等は到底
できなかったのに対し、本発明に従って構成された光電
変換装置においては、上記のように少数キャリア拡散長
以下の部分を作っても、厚層部12の存在により、全体
としての機械強度を満足な程度に維持し得るのである。
In other words, in conventional photoelectric conversion devices, especially when a low-quality semiconductor substrate is used, the total area of the substrate is
While it was impossible to reduce the thickness to less than the minority carrier diffusion length, in the photoelectric conversion device constructed according to the present invention, even if the thickness is made to be less than the minority carrier diffusion length as described above, Due to the presence of the thick layer portion 12, the overall mechanical strength can be maintained to a satisfactory level.

しかしもし、このように機械的な強度を稼ぐために設け
た厚層部12の存在により、向上し得る筈の光電変換特
性が大きく損われたのでは、せつかくにして薄層部11
を設けた意味も失われてしまう可能性があるが、本発明
の場合には、当該厚層部12の幅Wに関し、少数キャリ
ア拡散長の二倍以下という重要な限定を施しているため
、そうした危惧は回避できるのである。
However, if the presence of the thick layer portion 12 provided to increase mechanical strength greatly impairs the photoelectric conversion characteristics that could be improved, we would like to apologize for any inconvenience caused by removing the thin layer portion 11.
However, in the case of the present invention, an important limitation is imposed on the width W of the thick layer portion 12 to be less than or equal to twice the minority carrier diffusion length. Such concerns can be avoided.

その理由はすでに作用の項でも述べているが、念のため
、この実施例に即しても触れて置くと、図示実施例の場
合、半導体基板!Oの裏面側に設けられている障壁形成
層20は、まずもって薄層部11のキャリア濃度自体を
濃くする働きを有し、したがって、単に少数キャリアの
拡散長以下にこの半導体薄層部11を構成しただけのと
きよりも、さらに−層の開放起電圧向上効果を期待し得
る。
The reason for this has already been stated in the operation section, but just to be sure, I will mention it in connection with this embodiment.In the case of the illustrated embodiment, the semiconductor substrate! The barrier forming layer 20 provided on the back side of the semiconductor layer 20 has the function of increasing the carrier concentration of the thin layer portion 11 itself, and therefore simply makes the semiconductor thin layer portion 11 less than the diffusion length of minority carriers. It can be expected that the open-circuit electromotive force of the negative layer will be further improved compared to when the structure is simply configured.

一方、この障壁形成層20の存在による電気的なキャリ
ア適過し作用は、当該障壁形成層の端部から少数キャリ
ア拡散長の距離程度の部分であれば、単に上下方向に限
らず、横方向を含む全方向(ただしもちろん、半導体領
域のない所は除く)に及ぶものとなる。
On the other hand, the electrical carrier suitability effect due to the existence of this barrier forming layer 20 is not limited to the vertical direction but is also effective in the lateral direction as long as the distance of the minority carrier diffusion length from the edge of the barrier forming layer 20 is approximately the same. It extends in all directions including (however, of course, excluding areas where there is no semiconductor region).

したがって、各厚層部12の幅Wを既述のように少数キ
ャリア拡散長の二倍以下として置けば、この厚層部12
に関し、図中で左右方向の両端部分を見ると明らかなよ
うに、当該両端には右隣り、左隣りの各薄層部11.1
1の下面に備わっている障壁形成層部分の折れ下がる端
部が臨んでおり、したがってここから、当該厚層部12
の幅Wの半分づつにわたり、それら障壁形成層20の端
部が横方向や斜め上方向にも影響を及ぼし得るのである
Therefore, if the width W of each thick layer section 12 is set to twice the minority carrier diffusion length or less as described above, this thick layer section 12
As is clear from looking at both ends in the left and right direction in the figure, there are thin layer parts 11.1 on the right and on the left at both ends.
The folded end of the barrier forming layer portion provided on the lower surface of 1 is facing, and therefore, from here, the thick layer portion 12
The end portions of the barrier forming layer 20 can also have an influence in the lateral direction and diagonally upward direction over half of the width W of the barrier forming layer 20 .

言い換えれば、厚層部12の実効厚味が、こと、少数キ
ャリアに関しては、薄層部11の厚味dと余り変わらな
い厚味となったに等価と見ても良く、厚層部12中にお
いても、その中に存在し得る少数キャリアは、特に表面
から深さdの範囲内で顕著に、当該厚層部両側の薄層部
下の障壁形成層部分の影響を横方向から受けて、望まし
い追返し作用を受は得るようになる。
In other words, the effective thickness of the thick layer portion 12 can be considered to be equivalent to the thickness d, which is not much different from the thickness d of the thin layer portion 11 in terms of minority carriers. Also, the minority carriers that may exist therein are influenced laterally by the barrier-forming layer portions under the thin layer on both sides of the thick layer, particularly within the depth d from the surface, which is desirable. Uke begins to receive a repelling effect.

このようにして、厚層部+2があるにもかかわらず、そ
の存在に基づく開放起電圧V。Cの低下は無視し得る程
度とし得るし、悪い場合でも、従来に比せば十分高い値
に維持し得る。
In this way, even though there is a thick layer part +2, the open circuit voltage V based on its existence. The decrease in C can be made negligible, and even in the worst case, it can be maintained at a sufficiently high value compared to the conventional case.

さらに言うなら、本発明のように、障壁形成層20との
関係において厚層部12の幅を上記のように規定して始
めて、少数キャリア拡散長以下にまで薄くした薄層部1
1の存在と、それによる開放起電圧向上作用が大きな意
味を持ってくるのである。
Furthermore, as in the present invention, the width of the thick layer portion 12 is defined as described above in relation to the barrier forming layer 20, and then the thin layer portion 1 is thinned to be less than the minority carrier diffusion length.
The existence of 1 and its effect of improving the open circuit voltage are of great significance.

なお、この実施例においては、受光面ないし光入射面の
側に接合形成層13が、裏面側に障壁形成層20が設け
られていたが、これらは相対的に逆の位置関係とするこ
ともできる。
In this example, the bonding layer 13 was provided on the light-receiving surface or light-incident surface side, and the barrier-forming layer 20 was provided on the back side, but these may be placed in a relatively reverse positional relationship. can.

さらに、この第1図示実施例のように、半導体基板を全
体として見て平らな面の方を入射面ないし受光面とする
のではなく、薄層部11と厚層部12の厚味の差が表れ
て凸凹している方の面を受光面とすることもできるので
、そうした場合の一例を第2図に挙げ、説明する。
Furthermore, as in the first illustrated embodiment, the flat surface of the semiconductor substrate as a whole is not used as the incident surface or the light-receiving surface, but the thickness difference between the thin layer portion 11 and the thick layer portion 12 is Since it is also possible to use the surface with the uneven surface as the light-receiving surface, an example of such a case will be described with reference to FIG. 2.

ただし、本図中において第1図中と同一の符号を付した
構成子は、当該第1図中の対応する構成子と同一または
同様な機能を営むものてあり、場合により先の説明を援
用するものとして、以下での説明は省略するものもある
However, constructors in this figure with the same reference numerals as in Figure 1 have the same or similar functions as the corresponding constructors in Figure 1, and the previous explanation may be referred to in some cases. There are some cases in which the description below will be omitted.

薄層部11と厚層部12とが混在した結果、凸凹した面
の方が半導体基板】Oの表面となってあり、この表面側
に必要に応じて設けられる反射防止膜31を介し、接合
形成層13が設けられている。
As a result of the thin layer portion 11 and the thick layer portion 12 being mixed together, the uneven surface becomes the surface of the semiconductor substrate ]O, and bonding is performed via an anti-reflection film 31 provided as necessary on this surface side. A forming layer 13 is provided.

半導体基板全体として見た平らな裏面側には、これも先
の実施例と同様、障壁形成層20と、必要に応じて別途
設けられる保護層41を挟み、反射層42が設けられて
いる。
On the flat back side of the semiconductor substrate as a whole, as in the previous embodiment, a reflective layer 42 is provided with a barrier forming layer 20 and a protective layer 41, which is separately provided as required, sandwiched therebetween.

もちろん、薄層部Hの厚さdはここで光発生し得る少数
キャリアの拡散長以下とされており、厚層部12の横方
向寸法ないし幅Wは6、当該少数キャリア拡散長の二倍
以下とされている。
Of course, the thickness d of the thin layer portion H is set to be less than the diffusion length of minority carriers that can be photogenerated here, and the lateral dimension or width W of the thick layer portion 12 is 6, which is twice the minority carrier diffusion length. The following is considered.

こうした構成により、先に説明したとほぼ同様の理由に
より、機械的な強度と電気的な光電変換特性の双方を共
に良く満足した光電変換装置が提供されるが、ただこの
実施例の場合、一つ一つの各厚層部12に関し、その両
側の薄層部11 、11下の障壁形成層が横方向から少
数キャリア適過し機能を営み得るのみならず、自身の下
に設けられている障壁形成層部分も併せて同様の機能を
営む。
This configuration provides a photoelectric conversion device that satisfies both mechanical strength and electrical photoelectric conversion characteristics for almost the same reason as explained above, but in the case of this embodiment, one Regarding each thick layer portion 12, the thin layer portions 11 on both sides of each thick layer portion 12, and the barrier forming layer under the layer 11, can not only carry out minority carrier functions from the lateral direction but also act as a barrier forming layer provided under itself. The cambium layer also performs the same function.

特にこの実施例で望ましいのは、厚層部!2の突き出た
部分の側面が斜面とされていること、そしてこの斜面部
分には反射膜50が設けられていることである。
What is particularly desirable in this example is the thick layer! The side surface of the protruding portion 2 is a slope, and a reflective film 50 is provided on this slope.

このようになっていると、図示されているように、受光
面中に当該厚層部12が突き出ていて、この突出部分に
当たってしまった光があっても、この光は斜めの反射膜
50により、薄層部11の表面方向に反射され、光電変
換エネルギの生成に寄与し得るものとなる。つまり、突
出物12があっても、これが“影”を作らないのである
In this case, as shown in the figure, even if the thick layer portion 12 protrudes into the light-receiving surface and some light hits this protrusion, this light is reflected by the oblique reflective film 50. , is reflected toward the surface of the thin layer portion 11, and can contribute to the generation of photoelectric conversion energy. In other words, even if there is a protrusion 12, it does not create a "shadow".

また、この反射膜50を、第2図中、左手の部分で一ケ
所、仮想線で模式的に示すように、接合形成層13の引
き出し端子14として兼用すれば、こうした引き出し端
子が作るであろう“影”の問題も解消することができる
Furthermore, if this reflective film 50 is also used as the lead terminal 14 of the bonding layer 13 at one place on the left hand side in FIG. 2, as schematically shown by the phantom line, such a lead terminal can be created. The problem of wax “shadow” can also be solved.

もっとも、実際上、第1図示のように、各厚層部12の
側面をほぼ完全に切り立った側面として形成することの
方が難しいので、第1図示のように平らな方の半導体基
板表面側を受°光面とする場合にはともかく、この第2
図示実施例にあけるように、凸凹面を受光面とする場合
には、上記のような反射膜50の付与構成を採用するこ
とが実際的にも望ましい。
However, in practice, it is more difficult to form the side surfaces of each thick layer part 12 as almost completely steep sides as shown in the first figure, so the flat side surface of the semiconductor substrate as shown in the first figure is Regardless of when the light-receiving surface is
As shown in the illustrated embodiment, when a concavo-convex surface is used as a light-receiving surface, it is practically desirable to adopt the above-mentioned configuration for applying the reflective film 50.

もちろん、この第二の実施例においても、接合形成層1
3と障壁形成層20の位置的な置換は可能である。
Of course, also in this second embodiment, the bonding layer 1
3 and barrier forming layer 20 are possible.

なお、本発明によると、薄層部11をそれこそ薄くでき
るということは、逆に余りに薄過ぎて光の吸収が不十分
にならないかとの恐れも生じるが、先のように、受光面
と反対側の面に反射層42を形成することにより、この
点は部分と改善され得るし、また、いわゆるテクスチャ
構造ないし微細凸凹面形状を受光面や反射面側に形成す
れば、薄層部11への光入射経路は斜めとなり、光路が
長くなるので、十分な光吸収を得ることができる。
According to the present invention, the fact that the thin layer portion 11 can be made thinner also raises the fear that the thin layer portion 11 will be too thin and the light absorption will be insufficient. By forming the reflective layer 42 on the side surface, this point can be partially improved, and if a so-called textured structure or finely uneven surface shape is formed on the light receiving surface or reflective surface side, the thin layer portion 11 can be improved. Since the light incident path is oblique and the optical path becomes long, sufficient light absorption can be obtained.

第3図は、第1図示の実施例構造ないしそれに近い構造
を実際に得た場合の製作工程例を示している。
FIG. 3 shows an example of the manufacturing process in the case where the embodiment structure shown in FIG. 1 or a structure similar to it is actually obtained.

順を追って説明すると、まず第3図(A)に示されるよ
うに、 (100)面シリコン基板lOの表裏面を酸化
し、それぞれ約1障厚の酸化シリコン膜を成長させる。
To explain step by step, first, as shown in FIG. 3(A), the front and back surfaces of a (100)-plane silicon substrate 10 are oxidized to grow silicon oxide films each having a thickness of about 1 cm.

次いで、表面の酸化シリコン膜15はそのままにし、裏
面の酸化シリコン膜を、将来形成されるべき厚層部】2
の二次元平面パターンに応じてフォト・リソグラフィ工
程によりパターニングし、エツチング・マスク16とす
る。
Next, the silicon oxide film 15 on the front surface is left as is, and the silicon oxide film on the back surface is formed into a thick layer to be formed in the future]2
The etching mask 16 is patterned by a photolithography process according to a two-dimensional plane pattern.

このマスク16の存在の下に、KOHまたはヒドラジン
によって、面指数依存性のエツチングを行なう。
In the presence of this mask 16, surface index-dependent etching is performed using KOH or hydrazine.

エツチング後、マスクとして用いた酸化シリコン膜16
にはアルカリ溶液からの汚染の危険があるため、これを
バッフアートHF (buffered HF )等、
適当なる溶液で除去すると、第3図(B)に示されるよ
うに、本発明の趣旨に従い、薄層部11と厚層部I2と
が入れ子、ないし井桁状に組合された基本構造が得られ
る。
After etching, silicon oxide film 16 used as a mask
Since there is a risk of contamination from alkaline solutions, it should be treated with buffered HF, etc.
When removed with an appropriate solution, a basic structure is obtained in which the thin layer portion 11 and the thick layer portion I2 are combined in a nested or cross-shaped pattern, as shown in FIG. 3(B), in accordance with the spirit of the present invention. .

明らかなように、厚層部12の厚味は、意図的に調整さ
れたものではなく、上記酸化工程等における板厚変動を
考慮しなければ、供給された半導体基板の板厚自体と言
って良い。実際にもこのように、厚層部12に関しては
特にその意図的な厚味加工をしない方が経済的、−数的
であると思われるが、要すれば、適当なエツチング手法
ないしスライシング手法を採用することにより、この厚
層部12の厚味自体も所望の値に調整して良い。
As is clear, the thickness of the thick layer portion 12 is not intentionally adjusted, and unless changes in the thickness during the oxidation process etc. are taken into account, the thickness of the supplied semiconductor substrate itself is not adjusted. good. In fact, it seems to be more economical and numerically effective not to intentionally process the thick layer 12 to make it thicker, but if necessary, an appropriate etching method or slicing method can be used. By employing this, the thickness itself of the thick layer portion 12 may be adjusted to a desired value.

一方、少数キャリアの拡散長の二倍以下という厚層部1
2の幅Wに関する限定は、当該厚層部12が隣の薄層部
Uに交わる部分での寸法として規定され、もちろん、上
記エツチングに際するマスク寸法に応じ、実現される。
On the other hand, the thick layer 1 is less than twice the diffusion length of minority carriers.
The limitation regarding the width W of 2 is defined as the dimension at the portion where the thick layer portion 12 intersects with the adjacent thin layer portion U, and is of course realized depending on the mask size for the etching.

なお、本図から明らかなように、第1.2図示の実施例
は、単に平面方向で一方向にのみ、厚層部と薄層部とが
混在していることに限らず(そうであっても良いが)、
二次元平面の互いに直交する二方向に、共に同様の断面
構造となっていることを含むものである。あたかもこの
第3図(B)に示されている構造は、−昔前からの“板
チョロ”のようである。
As is clear from this figure, the embodiment shown in Figures 1 and 2 is not limited to the case where thick layer portions and thin layer portions coexist only in one direction in the plane (although this is not the case). ),
This includes having similar cross-sectional structures in two mutually orthogonal directions on a two-dimensional plane. The structure shown in Fig. 3 (B) looks like a "board cholo" from a long time ago.

第3図(B)の工程からは、先に少し述べたように、必
要に応じては表面をテクスチャ化した後、第3図(C)
に示されているように、CVDないし熱酸化技術等によ
り、表面に拡散マスク17を形成した状態で裏面に半導
体基板IOと同一導電型の不純物を拡散し、障壁形成層
20を形成する。
From the process shown in Figure 3 (B), the surface is textured if necessary as mentioned above, and then the process shown in Figure 3 (C) is performed.
As shown in FIG. 1, impurities having the same conductivity type as the semiconductor substrate IO are diffused onto the back surface with a diffusion mask 17 formed on the front surface by CVD or thermal oxidation technology, to form a barrier forming layer 20.

こうした拡散技術による形成に代え、CVDにより、同
一導電型であるが、よりワイド・ギャップな半導体層を
形成し、これをして障壁形成層20としても良い。
Instead of forming by such a diffusion technique, a semiconductor layer of the same conductivity type but with a wider gap may be formed by CVD, and this may be used as the barrier forming layer 20.

この後、第3図(D)に示されるように、CVDまたは
熱酸化によりて障壁形成層20を覆う拡散マスク兼パッ
シベイションyA41を設けた上で、表面側で半導体基
板とは逆導電型の不純物拡散を行ない、接合形成層13
を形成する。ただし、この接合形成層13についても、
要すればCVDでの形成も可能である。
After this, as shown in FIG. 3(D), after providing a diffusion mask and passivation layer yA41 covering the barrier forming layer 20 by CVD or thermal oxidation, the surface side is of a conductivity type opposite to that of the semiconductor substrate. The impurity diffusion is performed to form the bonding layer 13.
form. However, regarding this bonding layer 13 as well,
If necessary, formation by CVD is also possible.

このようにした後、表面に反射防止膜31と引き出し端
子(電極)11を、裏面に反射層兼用き出し端子(電極
)42を公知既存の適当なる方法により形成すれば、本
発明光電変換装置の第一実施例に近い基本構造が完成す
る。
After this, if an antireflection film 31 and an extraction terminal (electrode) 11 are formed on the front surface, and an extraction terminal (electrode) 42 serving as a reflective layer is formed on the back surface by a known and existing appropriate method, the photoelectric conversion device of the present invention can be used. A basic structure similar to that of the first embodiment is completed.

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

第1図は本発明に従って構成された光電変換装置の要部
概略構成図、第2図は本発明の他の実施例の概略構成図
、第3図は製作工程を追いながら本発明の実施例を示す
説明図、である。 図中、lOは半導体基板、11は半導体薄層部1,12
は半導体厚層部、13は接合形成層、20は障壁形成層
、42は反射層、50は厚層部の突出した側面部に備え
られる反射膜、である。 第1区 第2図
Fig. 1 is a schematic block diagram of the main parts of a photoelectric conversion device constructed according to the present invention, Fig. 2 is a schematic block diagram of another embodiment of the present invention, and Fig. 3 is an embodiment of the present invention following the manufacturing process. FIG. In the figure, lO is a semiconductor substrate, 11 is a semiconductor thin layer portion 1, 12
13 is a semiconductor thick layer portion, 13 is a junction forming layer, 20 is a barrier forming layer, 42 is a reflective layer, and 50 is a reflective film provided on the protruding side surface of the thick layer portion. District 1, Figure 2

Claims (1)

【特許請求の範囲】  所定の面積を有する半導体基板を、その厚さに関し、
該半導体基板の内部で光発生する少数キャリアの拡散長
よりも薄い薄層部と、該薄層部よりも厚く、物理的に十
分な強度を有する厚層部との混在構造から成るように加
工し; 上記厚層部を、少なくとも隣合う一対の上記薄層部間に
位置させると共に; 上記半導体基板の一方の表面に沿って上記少数キャリア
を集める接合形成層を、また他方の表面に沿って上記少
数キャリアを追返す障壁形成層を設け、該接合形成層か
障壁形成層のあるどちらか一方の半導体表面を受光面、
該受光面に対向する他方の表面を反射層付きの反射面と
した上で;上記厚層部の幅を、上記少数キャリア拡散長
の二倍以下としたこと; を特徴とする接合型光電変換装置。
[Claims] A semiconductor substrate having a predetermined area, with respect to its thickness,
Processed to have a mixed structure of a thin layer portion thinner than the diffusion length of minority carriers photogenerated inside the semiconductor substrate and a thick layer portion thicker than the thin layer portion and having sufficient physical strength. the thick layer portion is located between at least a pair of adjacent thin layer portions; and the junction forming layer that collects the minority carriers is placed along one surface of the semiconductor substrate and along the other surface. A barrier forming layer for repelling the minority carriers is provided, and the semiconductor surface of either the junction forming layer or the barrier forming layer is a light-receiving surface;
A junction photoelectric conversion characterized in that the other surface facing the light-receiving surface is a reflective surface with a reflective layer; and the width of the thick layer portion is not more than twice the minority carrier diffusion length. Device.
JP63004381A 1988-01-12 1988-01-12 Junction type photoelectric conversion device Expired - Lifetime JPH0682852B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63004381A JPH0682852B2 (en) 1988-01-12 1988-01-12 Junction type photoelectric conversion device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63004381A JPH0682852B2 (en) 1988-01-12 1988-01-12 Junction type photoelectric conversion device

Publications (2)

Publication Number Publication Date
JPH01181575A true JPH01181575A (en) 1989-07-19
JPH0682852B2 JPH0682852B2 (en) 1994-10-19

Family

ID=11582780

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63004381A Expired - Lifetime JPH0682852B2 (en) 1988-01-12 1988-01-12 Junction type photoelectric conversion device

Country Status (1)

Country Link
JP (1) JPH0682852B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0371677A (en) * 1989-08-10 1991-03-27 Sharp Corp Processing of substrate for photoelectric conversion device
JP2007281447A (en) * 2006-04-06 2007-10-25 Samsung Sdi Co Ltd Solar cell

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57124483A (en) * 1980-12-16 1982-08-03 Siemens Ag High efficiency solar battery

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57124483A (en) * 1980-12-16 1982-08-03 Siemens Ag High efficiency solar battery

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0371677A (en) * 1989-08-10 1991-03-27 Sharp Corp Processing of substrate for photoelectric conversion device
JP2007281447A (en) * 2006-04-06 2007-10-25 Samsung Sdi Co Ltd Solar cell
US8558104B2 (en) 2006-04-06 2013-10-15 Samsung Sdi Co., Ltd. Solar cell

Also Published As

Publication number Publication date
JPH0682852B2 (en) 1994-10-19

Similar Documents

Publication Publication Date Title
EP4593555B1 (en) Back contact solar cell and method for manufacturing the same
US4131984A (en) Method of making a high-intensity solid-state solar cell
KR100847741B1 (en) A point contact heterojunction silicon solar cell having a passivation layer at a VII-n junction interface and a method of manufacturing the same
JP2867983B2 (en) Photodetector and method of manufacturing the same
US20250176308A1 (en) Solar cell and manufacturing method therefor
JP2025115940A (en) Back-contact solar cells and solar modules
JPH0795602B2 (en) Solar cell and manufacturing method thereof
JPH09172196A (en) Structure and fabrication of aluminum alloy bonded self-aligned back electrode type silicon solar cell
JP2011507246A (en) Back electrode type solar cell having wide backside emitter region and method for manufacturing the same
JPH05110121A (en) Solar cell
CN110828583A (en) Crystalline silicon solar cell with front-side local passivation contact and preparation method thereof
CN115188837A (en) Back contact solar cell, preparation method and cell module
EP4300600B1 (en) Photovoltaic cell, method for preparing same, and photovoltaic module
JP2025096191A (en) Solar cell and its manufacturing method, photovoltaic module
US20100288346A1 (en) Configurations and methods to manufacture solar cell device with larger capture cross section and higher optical utilization efficiency
US20090014063A1 (en) Method for production of a single-sided contact solar cell and single-sided contact solar cell
JPH0797653B2 (en) Photoelectric conversion element
CN103890961B (en) Interdigitated back-contact photovoltaic cells with floating front-emitter regions
TW201318030A (en) Semiconductor light detecting device and method of preparing same
JP2878031B2 (en) Thin solar cell and manufacturing method
CN222088623U (en) Solar cells and photovoltaic modules
KR102010390B1 (en) Method for manufacturing solar cell and dopant region thereof
WO2025260895A1 (en) Back contact cell, photovoltaic module, and method for manufacturing back contact cell
US4956685A (en) Thin film solar cell having a concave n-i-p structure
JP2003224289A (en) Solar cell, solar cell connection method, and solar cell module

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term