JP3172368B2 - Photovoltaic device - Google Patents
Photovoltaic deviceInfo
- Publication number
- JP3172368B2 JP3172368B2 JP17017594A JP17017594A JP3172368B2 JP 3172368 B2 JP3172368 B2 JP 3172368B2 JP 17017594 A JP17017594 A JP 17017594A JP 17017594 A JP17017594 A JP 17017594A JP 3172368 B2 JP3172368 B2 JP 3172368B2
- Authority
- JP
- Japan
- Prior art keywords
- photoelectric conversion
- layer
- light
- conversion layer
- conductive film
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Fee Related
Links
- 238000006243 chemical reaction Methods 0.000 claims description 115
- 230000005684 electric field Effects 0.000 claims description 44
- 239000000463 material Substances 0.000 claims description 9
- 239000000126 substance Substances 0.000 claims description 9
- 229910013641 LiNbO 3 Inorganic materials 0.000 claims description 3
- 239000002245 particle Substances 0.000 description 28
- 239000004065 semiconductor Substances 0.000 description 27
- 230000000052 comparative effect Effects 0.000 description 11
- 230000007423 decrease Effects 0.000 description 7
- 238000005215 recombination Methods 0.000 description 5
- 230000006798 recombination Effects 0.000 description 5
- 239000000758 substrate Substances 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 4
- 229910021417 amorphous silicon Inorganic materials 0.000 description 3
- 239000000969 carrier Substances 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 230000000694 effects Effects 0.000 description 3
- 239000011521 glass Substances 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 229910052751 metal Inorganic materials 0.000 description 2
- 239000002184 metal Substances 0.000 description 2
- 238000005268 plasma chemical vapour deposition Methods 0.000 description 2
- 229910052709 silver Inorganic materials 0.000 description 2
- 238000004544 sputter deposition Methods 0.000 description 2
- 229910006404 SnO 2 Inorganic materials 0.000 description 1
- RTAQQCXQSZGOHL-UHFFFAOYSA-N Titanium Chemical compound [Ti] RTAQQCXQSZGOHL-UHFFFAOYSA-N 0.000 description 1
- 239000002253 acid Substances 0.000 description 1
- 229910052788 barium Inorganic materials 0.000 description 1
- DSAJWYNOEDNPEQ-UHFFFAOYSA-N barium atom Chemical compound [Ba] DSAJWYNOEDNPEQ-UHFFFAOYSA-N 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000031700 light absorption Effects 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 238000010248 power generation Methods 0.000 description 1
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 description 1
- 238000002230 thermal chemical vapour deposition Methods 0.000 description 1
- 239000010936 titanium Substances 0.000 description 1
- 229910052719 titanium Inorganic materials 0.000 description 1
Classifications
-
- 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
Landscapes
- Other Surface Treatments For Metallic Materials (AREA)
- Photovoltaic Devices (AREA)
Description
【0001】[0001]
【産業上の利用分野】この発明は、太陽光等の光エネル
ギーを電気エネルギーに変換させる光起電力装置に関す
るものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a photovoltaic device for converting light energy such as sunlight into electric energy.
【0002】[0002]
【従来の技術】従来、太陽光等の光エネルギーを電気エ
ネルギーに変換させる光起電力装置としては、様々な構
造のものが知られており、このような光起電力装置の一
つとして、図1に示すように、ガラス等の絶縁性の透光
性基板1上にTCO等の透光性導電膜2を設け、この透
光性導電膜2上に、例えば、p型(又はn型)の半導体
からなる一導電型半導体層3a(又は3c)と、i型の
半導体からなる光発電層3bと、n型(又はp型)の半
導体からなる他導電型半導体層3c(又は3a)とが積
層された光電変換層3を設け、さらにこの光電変換層3
上にAg,Al等の高反射金属で構成された裏面電極4
を設けたものが知られていた。2. Description of the Related Art Conventionally, various types of photovoltaic devices for converting light energy such as sunlight into electric energy have been known. One of such photovoltaic devices is shown in FIG. As shown in FIG. 1, a light-transmitting conductive film 2 such as TCO is provided on an insulating light-transmitting substrate 1 such as glass, and a p-type (or n-type) is formed on the light-transmitting conductive film 2. A semiconductor layer 3a (or 3c) made of a semiconductor of the type, a photovoltaic layer 3b made of an i-type semiconductor, and a semiconductor layer 3c (or 3a) made of an n-type (or p-type) semiconductor Is provided, and the photoelectric conversion layer 3 is further provided.
Back electrode 4 made of a highly reflective metal such as Ag or Al
Was known.
【0003】そして、このような光起電力装置において
は、光を上記の透光性基板1側から透光性導電膜2を通
して上記の光電変換層3に導き、上記の光発電層3bに
おいてキャリアを発生させて光電変換を行うようになっ
ていた。In such a photovoltaic device, light is guided from the light-transmitting substrate 1 side to the photoelectric conversion layer 3 through the light-transmitting conductive film 2, and the carrier is generated in the photovoltaic layer 3b. Are generated to perform photoelectric conversion.
【0004】また、近年においては、上記のような光起
電力装置において、図2に示すように、透光性導電膜2
と光電変換層3とが接する界面をテクスチャー化させて
凹凸形状にし、光が上記の透光性導電膜2を通して光電
変換層3に導かれる際に、透光性導電膜2と光電変換層
3との界面で光が反射されるのを抑制すると共に、光電
変換層3に導かれる光を散乱させて、光電変換層3内を
通過する光の光路長を長くするようにしたものが開発さ
れた。In recent years, in a photovoltaic device as described above, as shown in FIG.
The interface between the light-transmitting conductive film 2 and the photoelectric conversion layer 3 is textured so that the light-transmitting conductive film 2 is guided to the photoelectric conversion layer 3 through the light-transmitting conductive film 2. In addition to suppressing the reflection of light at the interface with, the light guided to the photoelectric conversion layer 3 is scattered to increase the optical path length of light passing through the photoelectric conversion layer 3. Was.
【0005】ここで、図2に示す光起電力装置のように
透光性導電膜2と光電変換層3とが接する界面を凹凸形
状にした場合、透光性導電膜2と光電変換層3とが接す
る界面が平坦になった図1の光起電力装置に比べて、光
電変換層3の光発電層3b内を通過する光の光路長が長
くなるため、多くのキャリアが発生して短絡電流が増加
した。Here, when the interface between the light-transmitting conductive film 2 and the photoelectric conversion layer 3 is made uneven as in the photovoltaic device shown in FIG. 2, the light-transmitting conductive film 2 and the photoelectric conversion layer 3 The optical path length of light passing through the photovoltaic layer 3b of the photoelectric conversion layer 3 is longer than that of the photovoltaic device of FIG. The current has increased.
【0006】しかし、このように透光性導電膜2と光電
変換層3とが接する界面を凹凸形状にした場合、その界
面が平坦なものに比べて曲線因子(F.F.)が低下
し、変換効率を十分に向上させることができないという
問題が生じた。However, when the interface at which the light-transmitting conductive film 2 and the photoelectric conversion layer 3 are in contact with each other is made uneven, the fill factor (FF) is reduced as compared with a case where the interface is flat. However, there has been a problem that the conversion efficiency cannot be sufficiently improved.
【0007】[0007]
【発明が解決しようとする課題】この発明は、光起電力
装置における上記のような問題を解決することを課題と
するものであり、透光性導電膜と光電変換層とが接する
界面を凹凸形状にした場合においても、曲線因子が低下
するということがなく、変換効率のよい光起電力装置が
得られるようにすることを目的とするものである。SUMMARY OF THE INVENTION It is an object of the present invention to solve the above-mentioned problems in a photovoltaic device, and an uneven interface between a light transmitting conductive film and a photoelectric conversion layer is provided. It is an object of the present invention to provide a photovoltaic device having high conversion efficiency without a decrease in fill factor even when the photovoltaic device is formed.
【0008】ここで、本発明者等は、図2に示す光起電
力装置のように透光性導電膜2と光電変換層3とが接す
る界面を凹凸形状にした場合に曲線因子が低下する原因
について研究を行った。Here, the present inventors have found that the fill factor is reduced when the interface where the translucent conductive film 2 and the photoelectric conversion layer 3 come into contact with each other is made uneven as in the photovoltaic device shown in FIG. The cause was studied.
【0009】この結果、上記のように透光性導電膜2と
光電変換層3とが接する界面を凹凸形状にすると、これ
により光電変換層3における内部電界がその面方向にお
いて不均一になり、図3に示すように、光の吸収が多く
行われる部分である透光性導電膜2の凹部2aと接する
光電変換層3の部分においては、破線で示した電気力線
の密度が透光性導電膜2に向かうに従い低くなって、一
点鎖線で示した等電位線の間隔が透光性導電膜2に向か
うに従って次第に大きくなり、透光性導電膜2の凹部2
aと接する光電変換層3の透光性導電膜2側の部分にお
ける内部電界が弱くなっていることが分かった。そし
て、このように内部電界が弱くなった光電変換層3の部
分においてキャリアの再結合が多く発生し、これにより
光起電力装置における曲線因子が低下して、変換効率の
向上が妨げられるということがわかった。As a result, when the interface at which the translucent conductive film 2 and the photoelectric conversion layer 3 are in contact with each other is made uneven, as described above, the internal electric field in the photoelectric conversion layer 3 becomes non-uniform in the plane direction, As shown in FIG. 3, in the portion of the photoelectric conversion layer 3 that is in contact with the concave portion 2 a of the light-transmitting conductive film 2, which is a portion where light absorption is large, the density of the electric flux lines indicated by the broken line is higher than the light-transmitting property. The distance between the equipotential lines indicated by the alternate long and short dash line gradually increases toward the light-transmitting conductive film 2, and the distance between the equipotential lines indicated by the dashed line increases.
It was found that the internal electric field in the portion of the photoelectric conversion layer 3 in contact with the light-transmitting conductive film 2 side was weakened. Then, a large amount of carrier recombination occurs in the portion of the photoelectric conversion layer 3 in which the internal electric field has been weakened, thereby decreasing the fill factor in the photovoltaic device and hindering improvement in conversion efficiency. I understood.
【0010】そこで、本発明者等は、上記の研究結果に
基づいて更に研究を行い、透光性導電膜2と光電変換層
3とが接する界面を凹凸形状に形成する等の原因で、光
電変換層3内における内部電界がその層面の面方向に不
均一になった場合に、これを是正し、光起電力装置にお
ける曲線因子の低下を抑制して、変換効率を向上させる
手段を開発し、この発明を完成するに至ったのである。Therefore, the present inventors conducted further research based on the above research results, and found that the photoelectric conversion layer 3 had an uneven interface at the interface between the transparent conductive film 2 and the photoelectric conversion layer 3. In the case where the internal electric field in the conversion layer 3 becomes non-uniform in the plane direction of the layer surface, this is corrected, and a means for suppressing the decrease of the fill factor in the photovoltaic device and improving the conversion efficiency has been developed. Thus, the present invention has been completed.
【0011】[0011]
【課題を解決するための手段】この発明においては、上
記のような課題を解決するため、内部に光発電層が設け
られた光電変換層と透光性導電膜とが接触する光起電力
装置において、光電変換層における内部電界がその層面
の面方向に不均一である場合に、内部電界が弱くなった
光電変換層の部分における光発電層に強誘電体を含有さ
せるようにしたのである。According to the present invention, in order to solve the above-mentioned problems, a photovoltaic device in which a photoelectric conversion layer having a photovoltaic layer provided therein and a light-transmitting conductive film are in contact with each other. In the above, when the internal electric field in the photoelectric conversion layer is non-uniform in the plane direction of the layer surface, the photovoltaic layer in the portion of the photoelectric conversion layer where the internal electric field is weakened contains a ferroelectric substance.
【0012】また、この発明においては、内部に光発電
層が設けられた光電変換層と透光性導電膜とが接触する
界面が凹凸形状に形成され、透光性導電膜の凹部と接す
る光電変換層の凸部における内部電界が弱くなった光起
電力装置において、透光性導電膜の凹部と接する光電変
換層の部分における光発電層の透光性導電膜側の部分に
強誘電体を含有させるようにしたのである。Further, in the present invention, the interface between the photoelectric conversion layer having the photovoltaic layer provided therein and the light-transmitting conductive film is formed in an uneven shape, and the photoelectric conversion layer is in contact with the concave portion of the light-transmitting conductive film. In a photovoltaic device in which the internal electric field in the convex portion of the conversion layer is weakened, a ferroelectric substance is formed in a portion of the photoelectric conversion layer on the light-transmitting conductive film side in a portion of the photoelectric conversion layer in contact with the concave portion of the light-transmitting conductive film. It was made to contain.
【0013】ここで、上記の強誘電体としては、例え
ば、BaTiO3 ,PbTiO3 ,LiNbO3 ,Li
TaO3 ,SbSI等の比誘電率が20以上の物質を用
いるようにした。Here, as the ferroelectric, for example, BaTiO 3 , PbTiO 3 , LiNbO 3 , Li
A substance having a relative dielectric constant of 20 or more, such as TaO 3 or SbSI, is used.
【0014】[0014]
【作用】この発明においては、内部に光発電層が設けら
れた光電変換層と透光性導電膜とが接触する光起電力装
置において、光電変換層における内部電界がその層面の
面方向に不均一である場合に、内部電界が弱くなった光
電変換層の部分における光発電層に強誘電体を含有させ
たため、内部電界が弱くなった光電変換層の部分におけ
る電気力線がこの強誘電体に引き付けられて、この部分
における電気力線の密度が高くなる。そして、これによ
り内部電界が弱くなった光電変換層の部分における電界
強度が上昇して、他の部分との内部電界の差が少なくな
って内部電界が均一化し、従来のように内部電界が弱く
なった部分でキャリアが再結合するということが少なく
なり、光起電力装置における曲線因子の低下が抑制され
て変換効率が向上する。According to the present invention, in a photovoltaic device in which a photoelectric conversion layer having a photovoltaic layer provided therein and a light-transmitting conductive film come into contact with each other, an internal electric field in the photoelectric conversion layer does not extend in a plane direction of the layer surface. In the case of uniformity, since the ferroelectric substance was included in the photovoltaic layer in the part of the photoelectric conversion layer where the internal electric field was weakened, the lines of electric force in the part of the photoelectric conversion layer where the internal electric field was weakened were , The density of the lines of electric force in this portion increases. This increases the electric field strength in the portion of the photoelectric conversion layer where the internal electric field is weakened, reduces the difference in the internal electric field from other portions, makes the internal electric field uniform, and weakens the internal electric field as in the related art. The recombination of carriers at the distorted portion is reduced, and a decrease in the fill factor in the photovoltaic device is suppressed, thereby improving the conversion efficiency.
【0015】また、内部に光発電層が設けられた光電変
換層と透光性導電膜とが接触する界面が凹凸形状に形成
され、透光性導電膜の凹部と接する部分における光電変
換層の内部電界が弱くなった光起電力装置において、透
光性導電膜の凹部と接する光電変換層の部分における光
発電層の透光性導電膜側の部分に強誘電体を含有させる
と、上記のように内部電界が弱くなった光電変換層の部
分における電界強度が上昇して、他の部分との内部電界
の差が少なくなって内部電界が均一化し、この部分にお
けるキャリアの再結合が少なくなって曲線因子の低下が
抑制され、短絡電流の増加と合わせて変換効率がさらに
向上する。The interface between the photoelectric conversion layer having the photovoltaic layer provided therein and the light-transmitting conductive film is formed in an uneven shape, and the portion of the photoelectric conversion layer in contact with the concave portion of the light-transmitting conductive film is formed. In a photovoltaic device in which the internal electric field is weakened, when a ferroelectric substance is contained in a portion of the photovoltaic layer on the light-transmitting conductive film side in a portion of the photoelectric conversion layer in contact with the concave portion of the light-transmitting conductive film, As described above, the electric field strength in the portion of the photoelectric conversion layer where the internal electric field is weakened increases, the difference in the internal electric field from the other portions decreases, the internal electric field becomes uniform, and the recombination of carriers in this portion decreases. As a result, a decrease in the fill factor is suppressed, and the conversion efficiency is further improved along with an increase in the short-circuit current.
【0016】[0016]
【実施例】以下、この発明の実施例に係る光起電力装置
を添付図面に基づいて具体的に説明すると共に、この実
施例の光起電力装置が従来の光起電力装置に比べて優れ
ていることを明らかにする。DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Hereinafter, a photovoltaic device according to an embodiment of the present invention will be specifically described with reference to the accompanying drawings, and the photovoltaic device of this embodiment will be superior to a conventional photovoltaic device. Make it clear.
【0017】この実施例における光起電力装置において
は、図4に示すように、ガラス等の絶縁性の透光性基板
1上に、テクスチャー化されてその表面が凹凸形状にな
ったSnO2 からなる透光性導電膜2を形成し、この透
光性導電膜2上に光電変換を行う光電変換層3として、
p型の非晶質シリコンカーバイドで構成されたp型半導
体層3aと、i型の非晶質シリコンで構成された光発電
層3bと、n型の非晶質シリコンで構成されたn型半導
体層3cとを順々に積層させ、更にこの光電変換層3上
にAg又はAl等の高反射金属で構成された裏面電極4
を設けた。In the photovoltaic device according to this embodiment, as shown in FIG. 4, on an insulating translucent substrate 1 made of glass or the like, a textured SnO 2 having an uneven surface is used. A light-transmitting conductive film 2 is formed, and a photoelectric conversion layer 3 that performs photoelectric conversion on the light-transmitting conductive film 2
p-type semiconductor layer 3a made of p-type amorphous silicon carbide, photovoltaic layer 3b made of i-type amorphous silicon, and n-type semiconductor made of n-type amorphous silicon And a back electrode 4 made of a highly reflective metal such as Ag or Al on the photoelectric conversion layer 3.
Was provided.
【0018】ここで、この実施例における光起電力装置
においては、上記透光性導電膜2の凹部2aと接する光
電変換層3において、光発電層3bの適当な位置に強誘
電体5としてチタン酸バリウム(BaTiO3 )粒子5
を含有させた。Here, in the photovoltaic device of this embodiment, in the photoelectric conversion layer 3 in contact with the concave portion 2a of the translucent conductive film 2, titanium is used as a ferroelectric material 5 at an appropriate position of the photovoltaic layer 3b. Barium acid (BaTiO 3 ) particles 5
Was contained.
【0019】そして、上記のような光起電力装置を製造
するにあたり、この実施例においては、まず、図5
(A)に示すように、上記の透光性基板1上に熱CVD
法等によってテクスチャー化されてその表面が凹凸形状
になった透光性導電膜2を形成した。In manufacturing the photovoltaic device as described above, in this embodiment, first, FIG.
As shown in FIG. 2A, thermal CVD is performed on the light-transmitting substrate 1.
The light-transmitting conductive film 2 was textured by a method or the like to form an uneven surface.
【0020】次いで、上記のように形成された透光性導
電膜2の上にプラズマCVD法等により、図5(B)に
示すように、ホウ素がドーピングされたp型半導体層3
aを下記の表1に示す成膜条件で形成した。なお、この
p型半導体層3aの膜厚が50〜200Åの範囲になる
ようにした。Next, as shown in FIG. 5B, the boron-doped p-type semiconductor layer 3 is formed on the light transmitting conductive film 2 formed as described above by a plasma CVD method or the like.
a was formed under the film forming conditions shown in Table 1 below. The thickness of the p-type semiconductor layer 3a was set to be in the range of 50 to 200 °.
【0021】その後、このp型半導体層3a上にプラズ
マCVD法等により下記の表1に示す成膜条件で、図5
(C)に示すように、上記の光発電層3bを当初はその
膜厚が約500Å程度になるように形成した。Thereafter, on the p-type semiconductor layer 3a, by the plasma CVD method or the like, under the film forming conditions shown in Table 1 below, FIG.
As shown in (C), the photovoltaic layer 3b was formed so that its thickness was about 500 ° at first.
【0022】そして、このように形成された光発電層3
bの表面に対して、下記の表2に示すスパッタリング条
件でBaTiO3 のスパッタリングを行い、図5(D)
に示すように、この光発電層3bの表面にBaTiO3
粒子5を供給した後、このようにBaTiO3 粒子5が
供給されたものに超音波を印加させて、光発電層3bの
表面に分散されて供給されたBaTiO3 粒子5を、図
5(E)に示すように、上記透光性導電膜2の凹部2a
に対応して凹んだ光発電層3bの凹み部分に集めた。The photovoltaic layer 3 formed as described above
On the surface of b, sputtering of BaTiO 3 was performed under the sputtering conditions shown in Table 2 below, and FIG.
As shown in FIG. 3 , BaTiO 3 is formed on the surface of the photovoltaic layer 3b.
After feeding particles 5, thus by applying ultrasonic waves to that BaTiO 3 particles 5 is supplied, the BaTiO 3 particles 5 supplied is distributed on the surface of the photovoltaic layer 3b, FIG. 5 (E As shown in FIG.
In the photovoltaic layer 3b.
【0023】そして、このように光発電層3bの凹み部
分にBaTiO3 粒子5を集めた状態で、この光発電層
3b上に更に同じ条件で光発電層3bを形成し、この光
発電層3b全体の膜厚が1000〜10000Å程度に
なるようにした後、この光発電層3b上に下記の表1に
示す成膜条件でn型半導体層3cをその膜厚が100〜
500Å程度になるように形成し、更にこのn型半導体
層3cの上に裏面電極4を形成して、図4に示したこの
実施例の光起電力装置を製造した。In a state where the BaTiO 3 particles 5 are collected in the recesses of the photovoltaic layer 3b, a photovoltaic layer 3b is further formed on the photovoltaic layer 3b under the same conditions. After the total film thickness is about 1000 to 10000 °, the n-type semiconductor layer 3c is formed on the photovoltaic layer 3b under the film forming conditions shown in Table 1 below to have a film thickness of 100 to 10,000 °.
The photovoltaic device of this embodiment shown in FIG. 4 was manufactured by forming the back electrode 4 on the n-type semiconductor layer 3c.
【0024】[0024]
【表1】 [Table 1]
【0025】[0025]
【表2】 [Table 2]
【0026】ここで、この実施例の光起電力装置のよう
に、透光性導電膜2の凹部2aと接する光電変換層3の
部分において、この光電変換層3内における光発電層3
bの透光性導電膜2側の部分にBaTiO3 粒子5から
なる強誘電体5を含有させると、図6に示すように、光
電変換層3内において破線で示した電気力線がこのよう
に含有された強誘電体5に引き付けられて、この部分に
おける電気力線の密度が高くなり、これにより透光性導
電膜2の凹部2aと接する光電変換層3の部分におい
て、透光性導電膜2側の部分における等電位線の間隔が
狭くなり、その部分における内部電界が上昇して他の部
分と均一化した。Here, as in the photovoltaic device of this embodiment, in the portion of the photoelectric conversion layer 3 which is in contact with the concave portion 2a of the translucent conductive film 2, the photovoltaic layer 3 inside the photoelectric conversion layer 3
When the ferroelectric material 5 composed of BaTiO 3 particles 5 is contained in the portion b of the light-transmitting conductive film 2 side, as shown in FIG. Is attracted to the ferroelectric material 5 contained in the transparent conductive film 2, and the density of the lines of electric force in this portion is increased. The interval between the equipotential lines in the portion on the side of the film 2 was narrowed, and the internal electric field in that portion was increased to be uniform with other portions.
【0027】この結果、この実施例の光起電力装置にお
いては、透光性導電膜2と光電変換層3とが接する界面
をテクスチャー化させて凹凸形状にし、光が透光性導電
膜2を通して光電変換層3に導かれる際に、透光性導電
膜2と光電変換層3との界面で光が反射されるのを抑制
すると共に、光電変換層3に導かれる光を散乱させて光
電変換層3内を通過する光の光路長を長くするようにし
た場合においても、従来のように透光性導電膜2の凹部
と接する光電変換層3の部分における内部電界が弱くな
って、この部分でキャリアが再結合して曲線因子の低下
ということが少なく、変換効率のよい光起電力装置が得
られるようになった。As a result, in the photovoltaic device of this embodiment, the interface between the light-transmitting conductive film 2 and the photoelectric conversion layer 3 is textured to have an uneven shape, and light passes through the light-transmitting conductive film 2. When guided to the photoelectric conversion layer 3, the reflection of light at the interface between the translucent conductive film 2 and the photoelectric conversion layer 3 is suppressed, and the light guided to the photoelectric conversion layer 3 is scattered to perform photoelectric conversion. Even when the optical path length of the light passing through the layer 3 is increased, the internal electric field in the portion of the photoelectric conversion layer 3 that is in contact with the concave portion of the translucent conductive film 2 is weakened as in the related art. As a result, the photovoltaic device with good conversion efficiency can be obtained with less reduction of the fill factor due to recombination of carriers.
【0028】次に、上記のように透光性導電膜2と光電
変換層3とが接する界面が凹凸形状に形成され、透光性
導電膜2の凹部2aと接する光電変換層3内における光
発電層3bに強誘電体5を含有させたこの実施例の光起
電力装置と、図2に示すように透光性導電膜2の凹部2
aと接する光電変換層3内における光発電層3bに強誘
電体5を含有させなかった比較例1の光起電力装置と、
図1に示すように透光性導電膜2と光電変換層3とが接
する界面が平坦になった比較例2の光起電力装置とにお
いて、それぞれ光発電層3bとp型半導体層3aとが接
する界面から光発電層3bの内部に進むに従って光発電
層3bにおける電界強度がどのように変化するかを調
べ、その結果を図7に示した。なお、同図においては、
それぞれの電界強度の変化を、上記実施例のものについ
ては実線で、比較例1のものについては一点鎖線で、比
較例2のものについては破線で示した。Next, as described above, the interface between the light-transmitting conductive film 2 and the photoelectric conversion layer 3 is formed in an uneven shape, and the light in the photoelectric conversion layer 3 contacting the concave portion 2a of the light-transmitting conductive film 2 is formed. The photovoltaic device of this embodiment in which the power generation layer 3b contains the ferroelectric material 5 and the concave portion 2 of the translucent conductive film 2 as shown in FIG.
a photovoltaic device of Comparative Example 1 in which the photovoltaic layer 3b in the photoelectric conversion layer 3 in contact with a did not contain the ferroelectric substance 5,
As shown in FIG. 1, in the photovoltaic device of Comparative Example 2 in which the interface at which the translucent conductive film 2 and the photoelectric conversion layer 3 are in contact with each other is flat, the photovoltaic layer 3b and the p-type semiconductor layer 3a are respectively It was investigated how the electric field intensity in the photovoltaic layer 3b changes as it proceeds from the contacting interface to the inside of the photovoltaic layer 3b, and the results are shown in FIG. In the figure,
The changes in the respective electric field intensities are shown by the solid line in the above-described embodiment, by the one-dot chain line in the comparative example 1, and by the broken line in the comparative example 2.
【0029】この結果、透光性導電膜2と光電変換層3
とが接する界面が平坦になった比較例2の光起電力装置
においては、p型半導体層3aと接触する界面からの距
離が変化しても光発電層3bにおける電界強度は殆ど変
化しなかったが、透光性導電膜2と光電変換層3とが接
する界面が凹凸形状になった比較例1の光起電力装置に
おいては、p型半導体層3aの界面から約2000Åの
範囲において電界強度が著しく弱くなっていた。これに
対し、この実施例の光起電力装置においては、比較例1
の光起電力装置と同様に透光性導電膜2と光電変換層3
とが接する界面を凹凸形状に形成したにも拘らず、p型
半導体層3aの界面から約2000Åの範囲における電
界強度の低下がかなり少なくなり、透光性導電膜2と光
電変換層3とが接する界面が平坦になった比較例2の光
起電力装置に近づいた状態になった。As a result, the translucent conductive film 2 and the photoelectric conversion layer 3
In the photovoltaic device of Comparative Example 2 in which the interface in contact with was flat, the electric field intensity in the photovoltaic layer 3b hardly changed even when the distance from the interface in contact with the p-type semiconductor layer 3a changed. However, in the photovoltaic device of Comparative Example 1 in which the interface at which the translucent conductive film 2 and the photoelectric conversion layer 3 are in contact has an uneven shape, the electric field intensity is within a range of about 2000 ° from the interface of the p-type semiconductor layer 3a. It was significantly weaker. On the other hand, in the photovoltaic device of this embodiment, Comparative Example 1
Transparent conductive film 2 and photoelectric conversion layer 3 as in the photovoltaic device of FIG.
Despite the fact that the interface in contact with is formed in an uneven shape, the decrease in the electric field strength in the range of about 2000 ° from the interface of the p-type semiconductor layer 3a is considerably reduced, and the light-transmitting conductive film 2 and the photoelectric conversion layer 3 The contacting interface became flat and approached the photovoltaic device of Comparative Example 2.
【0030】なお、比較例2の光起電力装置の場合、p
型半導体層3aと接触する界面からの距離が変化しても
光発電層3bにおける電界強度は殆ど変化しなかった
が、この比較例2の光起電力装置においては、透光性導
電膜2と光電変換層3とが接する界面を凹凸形状に形成
した場合の効果、例えば、光が透光性導電膜2を通して
光電変換層3に導かれる際に、透光性導電膜2と光電変
換層3との界面で光が反射するのが抑制されて光電変換
層3に導かれる光の量が増加したり、光電変換層3に導
かれた光が散乱されて光電変換層3内を通過する光の光
路長が長くなって短絡電流が増加する等の効果がないた
め、上記実施例のものに比べて、光が有効に利用され
ず、変換効率が悪くなっていた。In the case of the photovoltaic device of Comparative Example 2, p
Although the electric field intensity in the photovoltaic layer 3b hardly changed even when the distance from the interface in contact with the type semiconductor layer 3a changed, the photovoltaic device of Comparative Example 2 The effect when the interface in contact with the photoelectric conversion layer 3 is formed in an uneven shape, for example, when light is guided to the photoelectric conversion layer 3 through the light-transmitting conductive film 2, the light-transmitting conductive film 2 and the photoelectric conversion layer 3 The amount of light guided to the photoelectric conversion layer 3 is increased by suppressing the reflection of light at the interface with the light, or the light guided to the photoelectric conversion layer 3 is scattered and passes through the inside of the photoelectric conversion layer 3. Since there is no effect such as an increase in the short-circuit current due to an increase in the optical path length, light is not used effectively and the conversion efficiency is deteriorated as compared with the embodiment.
【0031】次に、上記のように透光性導電膜2の凹部
2aと接する光電変換層3内における光発電層3bにB
aTiO3 粒子5を含有させるにあたって、光発電層3
bに含有させるBaTiO3 粒子5の平均粒径を変化さ
せるようにした。そして、光発電層3bに含有させるB
aTiO3 粒子5の平均粒径と光起電力装置における開
放電圧(Voc),短絡電流(Isc),曲線因子
(F.F.)及び変換効率(η)との関係を求め、その
結果を図8に示した。Next, as described above, the photovoltaic layer 3b in the photoelectric conversion layer 3 in contact with the concave portion 2a of the translucent conductive film 2 has B
When the aTiO 3 particles 5 are contained, the photovoltaic layer 3
The average particle diameter of the BaTiO 3 particles 5 contained in b was changed. And B contained in the photovoltaic layer 3b.
The relationship between the average particle size of the aTiO 3 particles 5 and the open-circuit voltage (Voc), short-circuit current (Isc), fill factor (FF), and conversion efficiency (η) in the photovoltaic device was determined, and the results were plotted. 8 is shown.
【0032】この結果、平均粒径が10〜80Åの範囲
になったBaTiO3 粒子5を含有させた場合に、光起
電力装置における曲線因子(F.F.)や変換効率
(η)が向上し、この範囲の粒径のBaTiO3 粒子5
を用いることが好ましかった。As a result, when BaTiO 3 particles 5 having an average particle diameter in the range of 10 to 80 ° are contained, the fill factor (FF) and the conversion efficiency (η) in the photovoltaic device are improved. And BaTiO 3 particles 5 having a particle size in this range.
Was preferred.
【0033】また、上記のように透光性導電膜2の凹部
2aと接する光電変換層3の部分において、光発電層3
b内にBaTiO3 粒子5を含有させるにあたり、この
BaTiO3 粒子5を含有させる位置を変更させ、p型
半導体層3aと接する面からの距離と光起電力装置にお
ける変換効率との関係を求め、その結果を図9に示し
た。なお、ここでは光発電層3b全体の膜厚を約500
0Åにした。In the portion of the photoelectric conversion layer 3 which is in contact with the concave portion 2a of the light transmitting conductive film 2 as described above, the photovoltaic layer 3
Upon incorporating the BaTiO 3 particles 5 in b, then change the position of incorporating the BaTiO 3 particles 5, obtains the relationship between the conversion efficiency at a distance and the photovoltaic device from the surface in contact with the p-type semiconductor layer 3a, The result is shown in FIG. Here, the total thickness of the photovoltaic layer 3b is set to about 500
0 °.
【0034】この結果、p型半導体層3aと接する面か
らの距離が1000〜1200Åの範囲にBaTiO3
粒子5を含有させた場合に、光起電力装置における変換
効率が5%程度向上した。[0034] BaTiO 3 result, the distance from the surface in contact with the p-type semiconductor layer 3a is in the range of 1000~1200Å
When the particles 5 were contained, the conversion efficiency in the photovoltaic device was improved by about 5%.
【0035】そして、この実施例の光起電力装置におい
ては、このような結果に基づいてBaTiO3 粒子5を
p型半導体層3aと接する面から約500Åの位置に含
有させるようにしたが、BaTiO3 粒子5を含有させ
る位置は最初に堆積させる光発電層3bの膜厚を変更す
ることによって自由に調整することができ、例えば、透
光性導電膜2と光電変換層3とが接する界面の凹凸状態
や、光発電層3b全体の膜厚が変化して、光電変換層3
内における内部電界の弱い位置が変化したような場合に
は、最初に堆積させる光発電層3bの膜厚を変更させて
BaTiO3 粒子5を含有させる位置を変更させるよう
にした。In the photovoltaic device of this embodiment, the BaTiO 3 particles 5 are contained at a position of about 500 ° from the surface in contact with the p-type semiconductor layer 3a based on such a result. The position at which the three particles 5 are contained can be freely adjusted by changing the thickness of the photovoltaic layer 3b to be deposited first. For example, the position of the interface where the translucent conductive film 2 and the photoelectric conversion layer 3 are in contact with each other can be adjusted. The unevenness and the thickness of the entire photovoltaic layer 3b change, and the photoelectric conversion layer 3
When the position where the internal electric field is weak in the inside changes, the thickness of the first photovoltaic layer 3b is changed to change the position where the BaTiO 3 particles 5 are contained.
【0036】なお、この実施例においては、強誘電体5
として、BaTiO3 粒子5を用いた場合の例だけを示
したが、このBaTiO3 粒子5にかえてPbTiO
3 ,LiNbO3 ,LiTaO3 ,SbSI等の比誘電
率が20以上で透明な強誘電体5を用いた場合もほぼ同
様の効果が得られる。In this embodiment, the ferroelectric 5
As an example, only an example in which the BaTiO 3 particles 5 are used is shown, but instead of the BaTiO 3 particles 5, PbTiO 3 is used.
Almost the same effects can be obtained when a transparent ferroelectric material 5 having a relative dielectric constant of 20 or more such as 3 , LiNbO 3 , LiTaO 3 , SbSI or the like is used.
【0037】また、この実施例においては、凹凸形状に
なった透光性導電膜2の上に光電変換層3として、p型
半導体層3aと光発電層3bとn型半導体層3cとを順
々に積層させた構造のものを示したが、透光性導電膜2
の上に形成する光電変換層3をn型半導体層3c,光発
電層3b,p型半導体層3aの順に積層した構造のもの
であってもよく、この場合には光発電層3bのn型半導
体層3c側の部分に上記のような強誘電体5を含有させ
るようにする。In this embodiment, a p-type semiconductor layer 3a, a photovoltaic layer 3b, and an n-type semiconductor layer 3c are sequentially formed as a photoelectric conversion layer 3 on a light-transmitting conductive film 2 having an uneven shape. Although the structure having the laminated structure is shown, the light-transmitting conductive film 2
May have a structure in which the photoelectric conversion layer 3 formed thereon is stacked in the order of the n-type semiconductor layer 3c, the photovoltaic layer 3b, and the p-type semiconductor layer 3a. In this case, the n-type The ferroelectric 5 as described above is contained in the portion on the semiconductor layer 3c side.
【0038】さらに、この実施例の光起電力装置におい
ては、光電変換層3と透光性導電膜2とが接合する界面
が凹凸形状に形成されて、光電変換層3における内部電
界がその層面の面方向に不均一になった場合の例を示し
ただけであるが、他の原因で光電変換層3における内部
電界がその層面の面方向に不均一になった場合であって
も、上記のように内部電界が弱い光電変換層3における
光発電層3bの部分に上記のような強誘電体5を含有さ
せることにより、光電変換層3における内部電界をある
程度均一化させて、光起電力装置における曲線因子を改
善させることができる。Further, in the photovoltaic device of this embodiment, the interface at which the photoelectric conversion layer 3 and the translucent conductive film 2 are joined is formed in an uneven shape, and the internal electric field in the photoelectric conversion layer 3 is reduced by the surface of the layer. Although only an example in which the non-uniformity is obtained in the plane direction of the layer is shown, even if the internal electric field in the photoelectric conversion layer 3 becomes non-uniform in the plane direction of the layer surface due to other causes, As described above, the ferroelectric material 5 is contained in the photovoltaic layer 3b of the photoelectric conversion layer 3 having a weak internal electric field, thereby making the internal electric field in the photoelectric conversion layer 3 uniform to some extent, and The fill factor in the device can be improved.
【0039】[0039]
【発明の効果】以上詳述したように、この発明において
は、内部に光発電層が設けられた光電変換層と透光性導
電膜とが接触する光起電力装置において、光電変換層に
おける内部電界がその層面の面方向に不均一である場合
に、内部電界が弱くなった光電変換層の部分における光
発電層に強誘電体を含有させたため、内部電界が弱い部
分における電界強度が上昇して他の部分と均一化し、従
来のように内部電界が弱くなった部分でキャリアが再結
合するということが少なくなり、光起電力装置における
曲線因子の低下が抑制され、変換効率のよい光起電力装
置が得られた。As described in detail above, according to the present invention, in a photovoltaic device in which a photoelectric conversion layer having a photovoltaic layer provided therein and a light-transmitting conductive film are in contact with each other, When the electric field is non-uniform in the plane direction of the layer surface, the photovoltaic layer in the portion of the photoelectric conversion layer where the internal electric field has weakened contains a ferroelectric substance, so that the electric field strength in the portion where the internal electric field is weak increases. In the photovoltaic device, the reduction of the fill factor is suppressed, and the photovoltaic device with high conversion efficiency is suppressed. A power device was obtained.
【0040】また、この発明においては、内部に光発電
層が設けられた光電変換層と透光性導電膜とが接触する
界面が凹凸形状に形成された光起電力装置において、透
光性導電膜の凹部と接する光電変換層の部分における光
発電層の透光性導電膜側の部分に強誘電体を含有させた
ため、この強誘電体により、透光性導電膜の凹部と接す
る内部電界が弱い光電変換層の透光性導電膜側の部分に
おいて、その電界強度が上昇し、他の部分との内部電界
の差が少なくなって内部電界が均一化し、従来のように
この部分でキャリアが再結合するということが少なくな
った。Further, according to the present invention, there is provided a photovoltaic device in which an interface at which a photoelectric conversion layer having a photovoltaic layer provided therein and a light-transmitting conductive film come into contact with each other is formed in an uneven shape. Since the ferroelectric material is contained in the portion of the photoelectric conversion layer on the light-transmitting conductive film side in the portion of the photoelectric conversion layer in contact with the concave portion of the film, the internal electric field in contact with the concave portion of the light-transmitting conductive film is reduced by this ferroelectric material. In the portion of the weak photoelectric conversion layer on the side of the light-transmitting conductive film, the electric field strength increases, the difference in the internal electric field from the other portions is reduced, and the internal electric field is made uniform. Recombination is less likely.
【0041】この結果、透光性導電膜と光電変換層とが
接する界面を凹凸形状にし、光が透光性導電膜を通して
光電変換層に導かれる際に、透光性導電膜と光電変換層
との界面で光が反射するのを抑制して光電変換層に導か
れる光の量を増加させたり、光電変換層に導かれた光を
散乱させて光電変換層内を通過する光の光路長を長くし
て短絡電流を増加させるようにした光起電力装置におい
て、その曲線因子の低下を抑制して、さらに変換効率を
向上させることができるようになった。As a result, the interface where the light-transmitting conductive film and the photoelectric conversion layer are in contact with each other is made uneven, and when light is guided to the photoelectric conversion layer through the light-transmitting conductive film, the light-transmitting conductive film and the photoelectric conversion layer Suppresses the reflection of light at the interface with and increases the amount of light guided to the photoelectric conversion layer, or scatters the light guided to the photoelectric conversion layer and scatters the light to pass through the photoelectric conversion layer. In the photovoltaic device in which the short-circuit current is increased by increasing the length, the reduction of the fill factor can be suppressed, and the conversion efficiency can be further improved.
【図1】透光性導電膜と光電変換層との接触する界面が
平坦になった従来の光起電力装置の概略断面図である。FIG. 1 is a schematic cross-sectional view of a conventional photovoltaic device in which a contact interface between a light-transmitting conductive film and a photoelectric conversion layer is flattened.
【図2】透光性導電膜と光電変換層との接触する界面が
凹凸形状になった従来の光起電力装置の概略断面図であ
る。FIG. 2 is a schematic cross-sectional view of a conventional photovoltaic device in which an interface between a light-transmitting conductive film and a photoelectric conversion layer has an uneven shape.
【図3】図2に示した光起電力装置において、その光電
変換層内における電気力線及び等電位線の状態を示した
概略説明図である。FIG. 3 is a schematic explanatory view showing states of electric lines of force and equipotential lines in a photoelectric conversion layer of the photovoltaic device shown in FIG.
【図4】この発明の一実施例に係る光起電力装置の構造
を示した概略断面図である。FIG. 4 is a schematic sectional view showing a structure of a photovoltaic device according to one embodiment of the present invention.
【図5】同実施例の光起電力装置を製造する工程を示し
た概略説明図である。FIG. 5 is a schematic explanatory view showing a step of manufacturing the photovoltaic device of the embodiment.
【図6】同実施例の光起電力装置において、BaTiO
3 粒子を含有させた光電変換層内における電気力線及び
等電位線の状態を示した概略説明図である。FIG. 6 shows a photovoltaic device according to the embodiment, in which BaTiO 3 is used.
FIG. 3 is a schematic explanatory view showing states of electric lines of force and equipotential lines in a photoelectric conversion layer containing three particles.
【図7】上記実施例及び比較例1,2の各光起電力装置
において、各光発電層の内部における電界強度の状態を
示した図である。FIG. 7 is a diagram showing a state of an electric field strength inside each photovoltaic layer in each of the photovoltaic devices of the example and comparative examples 1 and 2.
【図8】光電変換層の内部に含有させるBaTiO3 粒
子の平均粒径と光起電力装置における開放電圧,短絡電
流,曲線因子,変換効率との関係を示した図である。FIG. 8 is a diagram showing the relationship between the average particle size of BaTiO 3 particles contained in the photoelectric conversion layer and the open voltage, short circuit current, fill factor, and conversion efficiency in the photovoltaic device.
【図9】光電変換層内においてBaTiO3 粒子を含有
させる位置と光起電力装置の変換効率との関係を示した
図である。FIG. 9 is a diagram showing the relationship between the position where BaTiO 3 particles are contained in the photoelectric conversion layer and the conversion efficiency of the photovoltaic device.
【符号の説明】 1 透光性基板 2 透光性導電膜 2a 透光性導電膜の凹部 3 光電変換層 3a p型半導体層 3b 光発電層 3c n型半導体層 5 強誘電体(BaTiO3 粒子)[Description of Signs] 1 translucent substrate 2 translucent conductive film 2a concave portion of translucent conductive film 3 photoelectric conversion layer 3a p-type semiconductor layer 3b photovoltaic layer 3c n-type semiconductor layer 5 ferroelectric (BaTiO 3 particles) )
───────────────────────────────────────────────────── フロントページの続き (58)調査した分野(Int.Cl.7,DB名) H01L 31/04 - 31/078 ──────────────────────────────────────────────────続 き Continued on the front page (58) Field surveyed (Int.Cl. 7 , DB name) H01L 31/04-31/078
Claims (3)
と透光性導電膜とが接触する光起電力装置において、光
電変換層における内部電界がその層面の面方向に不均一
である場合に、内部電界が弱くなった光電変換層の部分
における光発電層に強誘電体を含有させたことを特徴と
する光起電力装置。In a photovoltaic device in which a photoelectric conversion layer having a photovoltaic layer provided therein and a light-transmitting conductive film are in contact with each other, an internal electric field in the photoelectric conversion layer is non-uniform in a plane direction of the layer surface. A photovoltaic device, wherein the photovoltaic layer at the portion of the photoelectric conversion layer where the internal electric field has weakened contains a ferroelectric substance.
と透光性導電膜とが接触する界面が凹凸形状になった光
起電力装置において、透光性導電膜の凹部と接する光電
変換層の部分における光発電層の透光性導電膜側の部分
に強誘電体を含有させたことを特徴とする光起電力装
置。2. A photovoltaic device in which an interface between a photoelectric conversion layer having a photovoltaic layer provided therein and a light-transmitting conductive film has an uneven shape, wherein the photoelectric contacting a concave portion of the light-transmitting conductive film. A photovoltaic device, wherein a ferroelectric substance is contained in a portion of the photovoltaic layer on the light-transmitting conductive film side in the portion of the conversion layer.
おいて、上記の強誘電体として、BaTiO3 ,PbT
iO3 ,LiNbO3 ,LiTaO3 ,SbSIの何れ
かの物質を用いたことを特徴とする光起電力装置。3. The photovoltaic device according to claim 1, wherein said ferroelectric material is BaTiO 3 , PbT.
A photovoltaic device using any one of iO 3 , LiNbO 3 , LiTaO 3 , and SbSI.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17017594A JP3172368B2 (en) | 1994-06-28 | 1994-06-28 | Photovoltaic device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP17017594A JP3172368B2 (en) | 1994-06-28 | 1994-06-28 | Photovoltaic device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0818083A JPH0818083A (en) | 1996-01-19 |
| JP3172368B2 true JP3172368B2 (en) | 2001-06-04 |
Family
ID=15900091
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP17017594A Expired - Fee Related JP3172368B2 (en) | 1994-06-28 | 1994-06-28 | Photovoltaic device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3172368B2 (en) |
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6365699B1 (en) | 1995-05-01 | 2002-04-02 | Ppg Industries Ohio, Inc. | Curable compositions composite coatings and process for having improved mar and abrasion resistance |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| KR100786855B1 (en) * | 2001-08-24 | 2007-12-20 | 삼성에스디아이 주식회사 | Solar cell using ferroelectric |
-
1994
- 1994-06-28 JP JP17017594A patent/JP3172368B2/en not_active Expired - Fee Related
Cited By (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6365699B1 (en) | 1995-05-01 | 2002-04-02 | Ppg Industries Ohio, Inc. | Curable compositions composite coatings and process for having improved mar and abrasion resistance |
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0818083A (en) | 1996-01-19 |
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