JP3222945B2 - Method for manufacturing photovoltaic device - Google Patents
Method for manufacturing photovoltaic deviceInfo
- Publication number
- JP3222945B2 JP3222945B2 JP24327192A JP24327192A JP3222945B2 JP 3222945 B2 JP3222945 B2 JP 3222945B2 JP 24327192 A JP24327192 A JP 24327192A JP 24327192 A JP24327192 A JP 24327192A JP 3222945 B2 JP3222945 B2 JP 3222945B2
- Authority
- JP
- Japan
- Prior art keywords
- photovoltaic device
- film
- amorphous silicon
- light
- 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.)
- Expired - Lifetime
Links
- 238000000034 method Methods 0.000 title claims description 9
- 238000004519 manufacturing process Methods 0.000 title claims description 7
- 229910021417 amorphous silicon Inorganic materials 0.000 claims description 25
- 238000006243 chemical reaction Methods 0.000 claims description 20
- 239000001257 hydrogen Substances 0.000 claims description 20
- 229910052739 hydrogen Inorganic materials 0.000 claims description 20
- UFHFLCQGNIYNRP-UHFFFAOYSA-N Hydrogen Chemical compound [H][H] UFHFLCQGNIYNRP-UHFFFAOYSA-N 0.000 claims description 18
- 239000000758 substrate Substances 0.000 claims description 14
- 239000004065 semiconductor Substances 0.000 claims description 6
- 230000001678 irradiating effect Effects 0.000 claims description 4
- 239000010408 film Substances 0.000 description 51
- 239000000919 ceramic Substances 0.000 description 11
- 239000002245 particle Substances 0.000 description 9
- 230000015572 biosynthetic process Effects 0.000 description 7
- 239000000463 material Substances 0.000 description 7
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 5
- 238000010586 diagram Methods 0.000 description 5
- 238000007750 plasma spraying Methods 0.000 description 4
- 206010034960 Photophobia Diseases 0.000 description 2
- PNEYBMLMFCGWSK-UHFFFAOYSA-N aluminium oxide Inorganic materials [O-2].[O-2].[O-2].[Al+3].[Al+3] PNEYBMLMFCGWSK-UHFFFAOYSA-N 0.000 description 2
- 150000002431 hydrogen Chemical class 0.000 description 2
- 230000031700 light absorption Effects 0.000 description 2
- 208000013469 light sensitivity Diseases 0.000 description 2
- 239000012528 membrane Substances 0.000 description 2
- 239000000377 silicon dioxide Substances 0.000 description 2
- 229910018072 Al 2 O 3 Inorganic materials 0.000 description 1
- 206010034972 Photosensitivity reaction Diseases 0.000 description 1
- ATJFFYVFTNAWJD-UHFFFAOYSA-N Tin Chemical compound [Sn] ATJFFYVFTNAWJD-UHFFFAOYSA-N 0.000 description 1
- 238000010521 absorption reaction Methods 0.000 description 1
- 238000003486 chemical etching Methods 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 239000013078 crystal Substances 0.000 description 1
- 229910021419 crystalline silicon Inorganic materials 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000002474 experimental method Methods 0.000 description 1
- 239000004744 fabric Substances 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 239000011521 glass Substances 0.000 description 1
- AMGQUBHHOARCQH-UHFFFAOYSA-N indium;oxotin Chemical compound [In].[Sn]=O AMGQUBHHOARCQH-UHFFFAOYSA-N 0.000 description 1
- 239000011810 insulating material Substances 0.000 description 1
- 229910052751 metal Inorganic materials 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 230000036211 photosensitivity Effects 0.000 description 1
- 238000005268 plasma chemical vapour deposition Methods 0.000 description 1
- 239000002994 raw material Substances 0.000 description 1
- 239000002210 silicon-based material Substances 0.000 description 1
- 229910052709 silver Inorganic materials 0.000 description 1
- 239000004332 silver Substances 0.000 description 1
- 239000007790 solid phase Substances 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 239000010409 thin film Substances 0.000 description 1
- XOLBLPGZBRYERU-UHFFFAOYSA-N tin dioxide Chemical compound O=[Sn]=O XOLBLPGZBRYERU-UHFFFAOYSA-N 0.000 description 1
- 229910001887 tin oxide 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
- Y02E10/546—Polycrystalline 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
- 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
- Y02E10/548—Amorphous silicon PV cells
Landscapes
- Photovoltaic Devices (AREA)
Description
【0001】[0001]
【産業上の利用分野】本発明は、入射した光によるエネ
ルギーを電気エネルギーに変換する光起電力装置の製造
方法に関する。The present invention relates to a process for producing a photovoltaic equipment for converting energy according to the incident light into electrical energy.
【0002】[0002]
【従来の技術】光起電力装置では、如何にして入射した
光の殆どを吸収するかが問題となる。図5は、従来の光
起電力装置の素子構造図である。図中の(61)は、光起電
力装置の支持体となるガラスやセラミックス等からなる
基板、(62)は基板(61)上に形成された金属膜から成る背
面電極、(63)は背面電極(62)上に形成された非晶質シリ
コン膜を母材とする光電変換層、この光電変換層には膜
面に平行なpin接合が形成されている。(64)は光電変
換層(63)上に形成された光入射用の電極として機能する
透光性電極である。この光起電力装置では膜形成面側か
ら入射した光(65)を光電変換し電子と正孔とからなる光
キャリアとして取り出すこととなる。2. Description of the Related Art In a photovoltaic device, there is a problem how to absorb most of incident light. FIG. 5 is an element structure diagram of a conventional photovoltaic device. In the figure, (61) is a substrate made of glass or ceramic or the like serving as a support of the photovoltaic device, (62) is a back electrode made of a metal film formed on the substrate (61), and (63) is a back surface. A photoelectric conversion layer having an amorphous silicon film formed on the electrode (62) as a base material, and a pin junction parallel to the film surface is formed on the photoelectric conversion layer. (64) is a translucent electrode formed on the photoelectric conversion layer (63) and functioning as a light incident electrode. In this photovoltaic device, light (65) incident from the film forming surface side is photoelectrically converted and extracted as a photocarrier composed of electrons and holes.
【0003】この従来例光起電力装置にあっては、図示
の如き凹凸形状を基板(61)の表面に施すことで、入射し
た光の有効利用が図られている。即ち、透光性電極(64)
を経て入射した光(65)は、光電変換層(63)内を進行中、
順次吸収されていくものの、通常この光(65)は一度だけ
の進行ではこの光電変換層(63)に十分吸収されず、その
一部は光電変換層(64)を通過し背面電極(62)にまで至っ
てしまう。[0003] In this conventional photovoltaic device, the incident light is effectively used by forming a concavo-convex shape as shown on the surface of the substrate (61). That is, the translucent electrode (64)
The light (65) incident through is traveling in the photoelectric conversion layer (63),
Although this light is sequentially absorbed, usually this light (65) is not sufficiently absorbed by this photoelectric conversion layer (63) only once, and a part of the light (65) passes through the photoelectric conversion layer (64) and the back electrode (62). To reach.
【0004】斯る場合に、基板(61)の表面に上記凹凸形
状を施しておくと、この凹凸形状はその基板表面に被着
された背面電極(62)の表面にまでその凹凸状態を反映さ
せる結果、その背面電極(62)の表面に生じた凹凸形状が
効果的に光(65)を散乱反射させることとなり、再度この
光を光電変換層(63)内に走行させることとなる。特に、
この散乱反射された光の多くは、この光電変換層(63)の
膜内を斜めに走行することから、この光電変換層(63)内
を走行する距離がその光電変換層(63)の膜厚よりも実質
的に長くなり、より多くの光吸収が可能となる。In such a case, if the above-mentioned uneven shape is formed on the surface of the substrate (61), the uneven shape reflects the uneven state to the surface of the back electrode (62) attached to the surface of the substrate. As a result, the irregularities formed on the surface of the back electrode (62) effectively scatter and reflect the light (65), and the light travels again into the photoelectric conversion layer (63). In particular,
Most of the light scattered and reflected travels obliquely in the film of the photoelectric conversion layer (63), so that the distance traveled in the film of the photoelectric conversion layer (63) is longer than that of the film of the photoelectric conversion layer (63). It is substantially longer than the thickness, allowing more light absorption.
【0005】従って、斯様な凹凸形状を利用することに
よって光起電力装置としての光電変換効率の向上、とり
わけ長波長光の吸収量が増加することによる、短絡電流
の増加が成し得る。斯る光起電力装置に関しては、例え
ば特開昭62−76569号等に詳細に記載されてい
る。[0005] Therefore, by utilizing such a concavo-convex shape, the photoelectric conversion efficiency of the photovoltaic device can be improved, and in particular, the short-circuit current can be increased due to an increase in the absorption of long-wavelength light. Such a photovoltaic device is described in detail in, for example, JP-A-62-76569.
【0006】[0006]
【発明が解決しようとする課題】然し乍ら、斯様な凹凸
形状を備えた基板(61)を製造することは一般に幾つかの
困難を伴う。However, manufacturing a substrate (61) having such a concavo-convex shape generally involves some difficulties.
【0007】つまり、この凹凸形状で有効に光反射させ
るには、その凹凸形状の程度を微細なものとする必要が
ある一方、形成されたその凹凸形状の凸部はあまり鋭利
なものであってはならない。即ち、その凸部があまりに
も鋭利なものとなると、その後に形成される背面電極(6
2)や光電変換層(63)が極めて薄い膜であることからそれ
ら膜を均一な膜厚を保った状態で形成することが困難と
なり、更には、形成された膜の膜内応力が大きく残留し
てしまい、そもそも光起電力装置としての特性が十分に
得られないものとなってしまうからである。In other words, in order to effectively reflect light in this uneven shape, it is necessary to make the degree of the uneven shape minute, while the formed convex portion of the uneven shape is too sharp. Not be. That is, if the projection becomes too sharp, the back electrode (6
2) and the photoelectric conversion layer (63) are extremely thin films, which makes it difficult to form them with a uniform thickness, and furthermore, the formed film has large residual stress in the film. This is because the characteristics as a photovoltaic device cannot be sufficiently obtained in the first place.
【0008】従来、斯る凹凸形状の製造方法としては、
基板表面への機械加工や、薬剤等による化学エッチング
によってなされることが多いが未だ幾つかの問題を有し
ていた。[0008] Conventionally, as a method of manufacturing such a concavo-convex shape,
It is often performed by mechanical processing on the substrate surface or chemical etching with a chemical or the like, but still has some problems.
【0009】とりわけ、光起電力装置は、より多くの光
を吸収するため、即ちより大きな出力を得るためにそも
そも大面積の装置として作製する必要があることから、
従来の上記方法によってしては、大面積に亘った均一で
且つ微細な凹凸形状を施すことはできなかった。In particular, a photovoltaic device must be manufactured as a device having a large area in order to absorb more light, that is, to obtain a larger output.
According to the above-mentioned conventional method, it was not possible to form a uniform and fine uneven shape over a large area.
【0010】[0010]
【課題を解決するための手段】本発明光起電力装置の製
造方法の特徴とするところは、基板上に水素を含有した
非晶質シリコン膜を形成し、これにエネルギービームを
照射するとともに、該非晶質シリコン膜の表面に、順次
背面電極、光電変換層そして透光性電極を形成すること
にある。A feature of the method of manufacturing a photovoltaic device according to the present invention is that an amorphous silicon film containing hydrogen is formed on a substrate, and the amorphous silicon film is irradiated with an energy beam. An object is to sequentially form a back electrode, a photoelectric conversion layer, and a translucent electrode on the surface of the amorphous silicon film.
【0011】[0011]
【0012】[0012]
【0013】[0013]
【0014】[0014]
【作用】 本 発明光起電力装置の製造方法によれば、水素
を含有する非晶質シリコン膜にエネルギービームを照射
することにより、この非晶質シリコン膜中に含まれる水
素が膜から噴出し、斯る噴出の際の圧力に因ってこの非
晶質シリコン膜の厚みに局所的な大小ができることとな
る。これにより、この非晶質シリコン膜が形成された基
板の表面には、光反射に適した微細な凹凸形状を施すこ
とができる。According to the production process of the working of the present invention a photovoltaic device, by irradiating an energy beam to the amorphous silicon film containing hydrogen, hydrogen is ejected from the membrane contained in the amorphous silicon film The thickness of the amorphous silicon film is locally increased or decreased due to the pressure at the time of the ejection. Thus, the surface of the substrate on which the amorphous silicon film is formed can be provided with a fine uneven shape suitable for light reflection.
【0015】[0015]
【0016】[0016]
【0017】[0017]
【実施例】図1は、本発明の参考となる光起電力装置の
参考例の素子構造図である。図中の(1)はセラミックス
等からなる基板、(2)は絶縁材(2a)中に絶縁性セラミッ
クス粒(2b)を含む絶縁膜、(3)は絶縁膜(2)上に形成され
た銀等からなる背面電極、(4)は当該光起電力装置の光
電変換層で、本例では非晶質シリコン膜を使用し、その
構成としてはn型非晶質シリコン(4n)、真性非晶質シリ
コン(4i)そしてp型非晶質シリコン(4p)の三層構造から
成る。(5)は光入射側の酸化インジュウム錫や酸化錫等
からなる透光性電極である。DETAILED DESCRIPTION FIG. 1, the important reference photovoltaic device of the present invention
It is a device structure figure of a reference example . In the figure, (1) is a substrate made of ceramics or the like, (2) is an insulating film containing insulating ceramic particles (2b) in an insulating material (2a), and (3) is formed on the insulating film (2). A back electrode made of silver or the like, (4) is a photoelectric conversion layer of the photovoltaic device. In this example, an amorphous silicon film is used. The structure thereof is n-type amorphous silicon (4n), It has a three-layer structure of crystalline silicon (4i) and p-type amorphous silicon (4p). (5) is a light-transmitting electrode made of indium tin oxide, tin oxide, or the like on the light incident side.
【0018】セラミックス粒(2b)を含んだ絶縁膜(2)以
外は従来周知の材料であり、表1に上記光電変換層(4)
の代表的な形成条件を示す。Materials other than the insulating film (2) containing the ceramic particles (2b) are conventionally known materials, and Table 1 shows the photoelectric conversion layer (4).
The typical formation conditions of are shown.
【0019】[0019]
【表1】 [Table 1]
【0020】本参考例の特徴である絶縁膜(2)は以下の
ように形成される。セラミックス粒(2b)として粒径約5
μmのアルミナ粒を含むシリカ(SiO2)溶液を基板(1)の
表面に塗布した後、約500℃の温度で硬化させる。硬
化後の絶縁膜(2)の膜厚としては、0.5μm〜500
μmが実用的な範囲である。また、セラミックス粒(2b)
の粒径としては、0.1μm〜10μmが代表的な範囲
である。The insulating film (2) which is a feature of this embodiment is formed as follows. Particle size of about 5 as ceramic particles (2b)
After a silica (SiO 2 ) solution containing alumina particles of μm is applied to the surface of the substrate (1), it is cured at a temperature of about 500 ° C. The thickness of the cured insulating film (2) is 0.5 μm to 500 μm.
μm is a practical range. Also, ceramic grains (2b)
The typical range of the particle size is 0.1 μm to 10 μm.
【0021】これにより、シリカはそのセラミックス粒
(2b)を包み込むようにその粒間を埋めると共に、上記硬
化後の絶縁膜(2)表面をセラミックス粒(2b)によって凹
凸化することができることとなる。As a result, the silica becomes
In addition to filling the interstices so as to enclose (2b), the surface of the cured insulating film (2) can be made uneven by the ceramic grains (2b).
【0022】尚、本参考例では絶縁膜の膜厚は、硬化後
約20μmとなるように設計したが、本発明者等の実験
によればこの膜厚は0.5μm〜500μmの範囲にお
いて使用可能であることを確認している。又、本参考例
の場合にあってはこの絶縁膜の表面に生じる凹凸の程度
は約2μmとなった。[0022] The thickness of the insulating film in the present embodiment has been designed to be approximately 20μm after cure, the film thickness according to the experiments of the present inventors used in the range of 0.5μm~500μm Make sure it is possible. Further, in the case of the present reference example, the degree of irregularities generated on the surface of the insulating film was about 2 μm.
【0023】表2は、上記参考例光起電力装置の特性値
を示した表であり、同表には従来例光起電力装置のそれ
についても比較のために示してある。この従来例光起電
力装置としては、本参考例の特徴であるセラミックス粒
を含む絶縁膜に替え、シリカ単体からなる絶縁膜を使用
したこと以外は、全く同様の構造としている。Table 2 is a table showing the characteristic values of the photovoltaic device of the reference example, and the table also shows the values of the conventional photovoltaic device for comparison. This conventional photovoltaic device has a completely similar structure except that an insulating film made of silica alone is used instead of the insulating film containing ceramic particles, which is a feature of this reference example .
【0024】[0024]
【表2】 [Table 2]
【0025】同表で明らかなように、本参考例光起電力
装置は従来例光起電力装置と比較して短絡電流が20%
以上増加している。これは、本参考例光起電力装置にあ
ってはセラミックス粒による光反射が効果的に生じてい
る結果、光吸収が有効に行われ短絡電流の増加が成し得
たと考えられる。As is clear from the table, the photovoltaic device of this reference example has a short-circuit current of 20% as compared with the conventional photovoltaic device.
It is increasing. This is presumably because in the photovoltaic device of the present reference example , as a result of the effective reflection of light by the ceramic grains, light absorption was effectively performed and the short-circuit current could be increased.
【0026】本参考例における絶縁膜は、前述した塗布
法による形成のみならず、所謂プラズマ溶射法によって
形成された絶縁膜であってもよい。このプラズマ溶射法
とは、空中に噴出されたパウダ状原料をプラズマによる
エネルギーによって分解し、これを膜形成のための材料
とするものである。このプラズマ溶射法については例え
ば特開平4−45521号に詳細に記載されている。The insulating film in the present embodiment is not only formed by a coating fabric method described above, it may be an insulating film formed by a so-called plasma spraying. In the plasma spraying method, a powdery material spouted into the air is decomposed by the energy of plasma, and this is used as a material for forming a film. This plasma spraying method is described in detail in, for example, JP-A-4-45521.
【0027】このプラズマ溶射法による形成方法にあっ
ては、表3に示すような原材料及びガスを利用すること
によって前記参考例と同様に絶縁膜を形成することがで
きる。In this plasma spraying method, an insulating film can be formed in the same manner as in the reference example by using raw materials and gases as shown in Table 3.
【0028】[0028]
【表3】 [Table 3]
【0029】また、このセラミックス粒としては、上記
アルミナ(Al2O3)の他にTiN,TiC等を使用す
ることができる。As the ceramic particles, TiN, TiC or the like can be used in addition to the above-mentioned alumina (Al 2 O 3 ).
【0030】次に、本願発明の実施例について説明す
る。この実施例に於ける基板表面に凹凸形状を施す方法
は、水素を含有した非晶質シリコン膜にレーザビーム等
のエネルギービームを照射することに因り、斯る水素の
膜中からの爆発的な噴出現象を生じさせ、これにより、
その非晶質シリコン膜の表面に凹凸形状を施すものであ
る。Next, a description will be given of actual施例of the present invention. In this embodiment, the method of forming the unevenness on the substrate surface is performed by irradiating the hydrogen-containing amorphous silicon film with an energy beam such as a laser beam. Cause the eruption phenomenon,
The surface of the amorphous silicon film is made uneven.
【0031】この噴出現象が生ずる基となる水素、の膜
中含有量と、その膜にエネルギービームを照射したこと
によるその凹凸の程度との関係を示したのが図2であ
る。横軸はエネルギービームとして利用したArFエキ
シマレーザのエネルギー密度であり、縦軸はその凹凸の
程度を示したもので、同図には膜中の水素含有量とし
て、(a)18%、(b)13%、(c)8%の3種類について
示している。尚、これら水素含有量の制御は、後述する
膜の形成温度を調整することによって行った。FIG. 2 shows the relationship between the content of hydrogen, which is the base of the ejection phenomenon, in the film and the degree of unevenness due to the irradiation of the film with the energy beam. The horizontal axis shows the energy density of the ArF excimer laser used as the energy beam, and the vertical axis shows the degree of the unevenness. In the figure, the hydrogen content in the film is (a) 18%, (b) 13) and (c) 8%. The control of the hydrogen content was performed by adjusting the film formation temperature described later.
【0032】同図から明らかなように、膜中の水素含有
量とエネルギー密度とが共に増加するにつれて、その凹
凸の程度は急速に大きくなる。特に18%の水素含有量
の場合にあってはエネルギー密度が200mJ/cm2
以上で急激に増加している。As can be seen from the figure, as the hydrogen content and the energy density in the film both increase, the degree of the irregularities rapidly increases. In particular, when the hydrogen content is 18%, the energy density is 200 mJ / cm 2.
Above, it has increased sharply.
【0033】図3は、その形成温度と膜中の水素含有量
との関係を示す特性図である。同図によれば、形成温度
200℃から500℃へと高温化するにつれて漸次減少
することが分かる。従って、この形成温度による膜中の
水素含有量の制御は極めて容易であり且つ再現性のよい
ものであることが分かる。FIG. 3 is a characteristic diagram showing the relationship between the formation temperature and the hydrogen content in the film. The figure shows that the temperature gradually decreases as the formation temperature increases from 200 ° C. to 500 ° C. Therefore, it is understood that the control of the hydrogen content in the film by the formation temperature is extremely easy and has good reproducibility.
【0034】次に、この水素の噴出現象により凹凸形状
を施した光起電力装置の特性について説明する。図4
は、上記第2の実施例光起電力装置の特性を従来の光起
電力装置の特性と比較したもので、同図には夫々の光感
度特性を示している。本実施例光起電力装置(a)の具
体的な素子構造は、前述した参考例光起電力装置の絶縁
膜(2)に替えて、エネルギービームの照射に因る水素噴
出で凹凸形状を施した非晶質シリコン膜を使用したこと
以外、全く同様である。Next, the characteristics of the photovoltaic device provided with the uneven shape due to the hydrogen ejection phenomenon will be described. FIG.
Is a comparison of the characteristics of the photovoltaic device of the second embodiment with the characteristics of a conventional photovoltaic device. FIG. 4 shows the respective photosensitivity characteristics. The specific element structure of the photovoltaic device (a) of the present embodiment is different from the insulating film (2) of the photovoltaic device of the reference example described above in that the unevenness is formed by the ejection of hydrogen due to the irradiation of the energy beam. This is exactly the same except that an amorphous silicon film is used.
【0035】実施例で使用した非晶質シリコン膜として
は、その形成温度が約250℃とし、膜厚が約3000
Åの膜である。又、従来例光起電力装置(b)としては
表2における従来例光起電力装置と同様のもので評価し
た。The amorphous silicon film used in the embodiment has a formation temperature of about 250 ° C. and a thickness of about 3000
膜 film. Further, as the conventional photovoltaic device (b), the same device as the conventional photovoltaic device in Table 2 was evaluated.
【0036】同図によれば、本発明光起電力装置(a)
では、600nm〜800nmの長波長領域での光感度
が大きく向上しており、入射した光、とりわけ長波長光
を十分利用できていることから、水素噴出による凹凸形
状が良好に形成できていることが分かる。According to the figure, the photovoltaic device of the present invention (a)
In the above, the light sensitivity in the long wavelength region of 600 nm to 800 nm is greatly improved, and the incident light, especially the long wavelength light, can be sufficiently utilized, so that the uneven shape by the hydrogen ejection can be formed well. I understand.
【0037】[0037]
【0038】[0038]
【0039】[0039]
【0040】[0040]
【0041】[0041]
【0042】[0042]
【0043】[0043]
【0044】[0044]
【0045】前述した実施例の半導体材料として主に非
晶質半導体を使用したが、本発明の効果は斯る半導体材
料に限られるものではなく、例えば多結晶半導体や単結
晶半導体の組合わせによって成る光電変換層であって
も、水素を含有した非晶質シリコン材料を使用する限り
全く同様に形成できる。更にはこの光電変換層として
は、実施例で利用したプラズマCVD法等によって形成
されたものだけに限られるものではなく、例えば固相成
長法等で形成されたものであってもよい。Although an amorphous semiconductor is mainly used as the semiconductor material in the above-described embodiment, the effect of the present invention is not limited to such a semiconductor material. For example, a combination of a polycrystalline semiconductor and a single-crystal semiconductor may be used. Such a photoelectric conversion layer can be formed in exactly the same manner as long as an amorphous silicon material containing hydrogen is used. Further, the photoelectric conversion layer is not limited to one formed by the plasma CVD method or the like used in the embodiment, and may be one formed by, for example, a solid phase growth method.
【0046】[0046]
【発明の効果】本発明光起電力装置の製造方法によれ
ば、水素を含有する非晶質シリコン膜にエネルギービー
ムを照射することにより、この非晶質シリコン膜中に含
まれる水素が膜から噴出し、斯る噴出の際の圧力に因っ
てこの非晶質シリコン膜の厚みに局所的な大小ができる
こととなる。これにより、この非晶質シリコン膜が形成
された基板の表面には、光反射に適した微細な凹凸形状
を施すことができる。 According to the photovoltaic device manufacturing method of the present invention ,
Energy beam on amorphous silicon film containing hydrogen.
Irradiation of the amorphous silicon film
Hydrogen is ejected from the membrane, and due to the pressure at the time of the ejection,
Leverage amorphous silicon film thickness can be locally large or small
It will be. Thereby, this amorphous silicon film is formed.
Fine uneven surface suitable for light reflection
Can be applied.
【0047】[0047]
【0048】[0048]
【図1】本発明の参考となる光起電力装置の参考例の素
子構造断面図である。1 is a device structure cross-sectional view of a reference example of important reference photovoltaic device of the present invention.
【図2】水素を含有する非晶質シリコンへのエネルギー
ビーム照射のエネルギー密度と、凹凸形状の程度を示す
特性図である。FIG. 2 is a characteristic diagram showing the energy density of energy beam irradiation on amorphous silicon containing hydrogen and the degree of unevenness.
【図3】非晶質シリコンの形成条件と膜中水素含有量と
の関係を示す特性図である。FIG. 3 is a characteristic diagram showing a relationship between amorphous silicon formation conditions and hydrogen content in a film.
【図4】本発明光起電力装置と従来例光起電力装置の光
感度特性図である。FIG. 4 is a light sensitivity characteristic diagram of the photovoltaic device of the present invention and a conventional photovoltaic device.
【図5】従来例光起電力装置の素子構造断面図である。FIG. 5 is a sectional view of an element structure of a conventional photovoltaic device.
(1)…基板 (2)…絶縁膜 (2b)…絶縁性セラミックス粒 (3)…背面電
極 (4)…光電変換層 (5)…透光性
電極(1) ... substrate (2) ... insulating film (2b) ... insulating ceramic particles (3) ... back electrode (4) ... photoelectric conversion layer (5) ... translucent electrode
───────────────────────────────────────────────────── フロントページの続き (56)参考文献 特開 平4−196364(JP,A) 特開 平2−180081(JP,A) 特開 平3−159179(JP,A) 特開 平4−299575(JP,A) 特開 平3−212977(JP,A) 特開 昭57−71188(JP,A) (58)調査した分野(Int.Cl.7,DB名) H01L 31/04 - 31/078 ──────────────────────────────────────────────────続 き Continuation of the front page (56) References JP-A-4-196364 (JP, A) JP-A-2-180081 (JP, A) JP-A-3-159179 (JP, A) JP-A-4-199 299575 (JP, A) JP-A-3-212977 (JP, A) JP-A-57-71188 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) H01L 31/04-31 / 078
Claims (1)
膜を形成する工程と、 上記非晶質シリコン膜に対して、エネルギービームを照
射する工程と、 上記非晶質シリコン膜上に背面電極を形成する工程と、 上記背面電極上に半導体から成る光電変換層を形成する
工程と、 上記光電変換層上に透光性電極を形成する工程と、 から成ることを特徴とする光起電力装置の製造方法。 Amorphous silicon containing hydrogen on a substrate
Forming a film, and irradiating the amorphous silicon film with an energy beam.
Irradiating , forming a back electrode on the amorphous silicon film, and forming a photoelectric conversion layer made of a semiconductor on the back electrode.
A method for manufacturing a photovoltaic device, comprising: a step of forming a translucent electrode on the photoelectric conversion layer .
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24327192A JP3222945B2 (en) | 1992-09-11 | 1992-09-11 | Method for manufacturing photovoltaic device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP24327192A JP3222945B2 (en) | 1992-09-11 | 1992-09-11 | Method for manufacturing photovoltaic device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH0697475A JPH0697475A (en) | 1994-04-08 |
| JP3222945B2 true JP3222945B2 (en) | 2001-10-29 |
Family
ID=17101390
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP24327192A Expired - Lifetime JP3222945B2 (en) | 1992-09-11 | 1992-09-11 | Method for manufacturing photovoltaic device |
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| Country | Link |
|---|---|
| JP (1) | JP3222945B2 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| AUPP699798A0 (en) * | 1998-11-06 | 1998-12-03 | Pacific Solar Pty Limited | Thin films with light trapping |
| AUPR719801A0 (en) * | 2001-08-23 | 2001-09-13 | Pacific Solar Pty Limited | Glass beads coating process |
| JP2005311292A (en) * | 2004-03-25 | 2005-11-04 | Kaneka Corp | Substrate for thin film solar cell, manufacturing method therefor, and thin film solar cell using the same |
| EP1732139B1 (en) | 2004-03-25 | 2018-12-12 | Kaneka Corporation | Method for producing a substrate for thin-film solar cell |
-
1992
- 1992-09-11 JP JP24327192A patent/JP3222945B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH0697475A (en) | 1994-04-08 |
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