Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS5826623B2 - photocell - Google Patents
[go: Go Back, main page]

JPS5826623B2 - photocell - Google Patents

photocell

Info

Publication number
JPS5826623B2
JPS5826623B2 JP51154010A JP15401076A JPS5826623B2 JP S5826623 B2 JPS5826623 B2 JP S5826623B2 JP 51154010 A JP51154010 A JP 51154010A JP 15401076 A JP15401076 A JP 15401076A JP S5826623 B2 JPS5826623 B2 JP S5826623B2
Authority
JP
Japan
Prior art keywords
electrode
titanium
light
photovoltaic cell
photoelectrode
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP51154010A
Other languages
Japanese (ja)
Other versions
JPS5377188A (en
Inventor
勉 岩城
勝弘 高橋
信晴 小柴
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP51154010A priority Critical patent/JPS5826623B2/en
Publication of JPS5377188A publication Critical patent/JPS5377188A/en
Publication of JPS5826623B2 publication Critical patent/JPS5826623B2/en
Expired 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
    • Y02E10/542Dye sensitized solar cells

Landscapes

  • Hybrid Cells (AREA)
  • Photovoltaic Devices (AREA)

Description

【発明の詳細な説明】 本発明は、光エネルギーを電気エネルギーに変換するエ
ネルギー変換装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an energy conversion device that converts light energy into electrical energy.

電極に光を照射することによシ、電気化学的な挙動を示
す光電極は古くからよく知られておシ、多数の半導体が
光電極として用いられている。
Photoelectrodes that exhibit electrochemical behavior when the electrode is irradiated with light have been well known for a long time, and many semiconductors have been used as photoelectrodes.

一般的にn型半導体はアノード反応に光応答性があり、
p型半導体はカソード反応に光応答性がある。
In general, n-type semiconductors have photoresponsiveness in anode reactions,
P-type semiconductors have photoresponsiveness in cathode reactions.

各種多数の半導体の中において、n型半導体である酸化
チタン(ルチル型構造)をアノードとして用いた場合、
電極電位は他の半導体電極にくらべて卑であり、しかも
、比較的広範囲の電解液に不溶性でかつ安定であって、
電極自体はなんら変化しないで、溶液中の物質のみが、
電気化学反応にあづかるという非常にすぐれた特質をも
っているということが今日にいたって判明されている。
Among various semiconductors, when titanium oxide (rutile structure), which is an n-type semiconductor, is used as an anode,
The electrode potential is lower than that of other semiconductor electrodes, and it is insoluble and stable in a relatively wide range of electrolytes.
The electrode itself does not change in any way; only the substance in the solution changes.
It has been discovered to this day that it has a very unique property of being able to participate in electrochemical reactions.

とのルチル型酸化チタンをアノードとして、適当なカソ
ードと組み合わせることによって、種々の光電池を構成
することができる。
By using rutile titanium oxide as an anode and combining it with a suitable cathode, various photovoltaic cells can be constructed.

その中の1つとして、燃料電池で用いられる空気(酸素
)拡散型電極との組み合わせなども、試みられている。
One example of this is the combination with air (oxygen) diffusion type electrodes used in fuel cells.

この場合、電解液としてか性アルカリ液を用いるが、そ
の電池特性は起電力として約1.IVが得られ、アノー
ドへの十分な光照射により、ある程度の電力がとりだす
ことができ、新型光電池としてその実現可能性が期待さ
れている。
In this case, a caustic alkaline solution is used as the electrolyte, and its battery characteristics are approximately 1. By obtaining IV and irradiating the anode with sufficient light, a certain amount of electricity can be extracted, and there are high expectations for its feasibility as a new type of photovoltaic cell.

この光電池の反応は、アノードでは hν(光)→ e + p (h ニブラン
ク定数)4 p + 40H−→2H20+ 02↑(
シ:光の振動数) カソードでは (e:電子)02+2H2
0+4e→40H(p:電子ホール)の反応が進行する
と考えられている。
The reaction of this photocell is as follows at the anode: hν (light) → e + p (h Nyblank constant) 4 p + 40H− → 2H20+ 02↑(
C: Frequency of light) At the cathode (e: Electron) 02+2H2
It is thought that a reaction of 0+4e→40H (p: electron hole) proceeds.

したがって、アノードでは光照射によって水を分解して
酸素を生成し、カソードでは酸素が消費されている。
Therefore, at the anode, water is decomposed by light irradiation to generate oxygen, and at the cathode, oxygen is consumed.

この電池は、光と空気中の酸素を活物質として用いるの
で、充電することなく半永久的に作動が可能であるので
、シリコン太陽電池などと同様、繁雑な手入れはまった
く不必要である。
Since this battery uses light and oxygen in the air as active materials, it can operate semi-permanently without being recharged, so like silicon solar cells, it does not require any complicated maintenance.

ただ、このような光電池において、ルチル型二酸化チタ
ンのような半導体電極を用いた場合、電流がち1シ多く
とシだせない。
However, in such a photovoltaic cell, when a semiconductor electrode such as rutile-type titanium dioxide is used, the current cannot be increased by one current.

その原因として、(1)半導体表面での光の電子への変
換効率が低いとと(数多以下)。
The reasons for this are: (1) the conversion efficiency of light into electrons on the semiconductor surface is low (less than a few);

(j2)、1半導体電極の反応面は光照射面になるが、
対極は光照射の都合上、光照射面の反対側に配置せねば
ならず、そのために反応イオンは光電極を周回しなけれ
ばならないので、電解液抵抗が非常に大きくなる。
(j2), 1 The reaction surface of the semiconductor electrode becomes the light irradiation surface,
For convenience of light irradiation, the counter electrode must be placed on the opposite side of the light irradiation surface, and therefore the reactive ions must go around the photoelectrode, resulting in a very large electrolyte resistance.

(3)半導体電極の反応面は表面層であり、一面だけの
反応面に限られる。
(3) The reaction surface of a semiconductor electrode is a surface layer, and is limited to only one reaction surface.

(4)ルチル型二酸化チタン半導体の電気抵抗は大きく
、したがって電極中でのIR(電流×抵抗:降下が犬で
、電池内部抵抗は非常に大きい。
(4) The electrical resistance of the rutile type titanium dioxide semiconductor is large, so the IR (current x resistance: drop) in the electrode is very large, and the internal resistance of the battery is very large.

(5)光電極と導通する金属が、電解液に接すると局部
電池を形成し、内部損失を生ずるので、二酸化チタン粉
末と導電剤とを混合して、光電極を形成することはでき
ない。
(5) When the metal conductive to the photoelectrode comes into contact with the electrolyte, it forms a local battery and causes internal loss, so the photoelectrode cannot be formed by mixing titanium dioxide powder and a conductive agent.

などがあげられる。etc.

これらのことより、実用化が極めて困難とされているの
であるが、逆に上記のような問題点を改善すれば、それ
だけ実用化の可能性がます1す期待できるわけである。
These factors make it extremely difficult to put it into practical use, but on the other hand, if the above-mentioned problems can be improved, the possibility of practical application can be expected to increase.

本発明では、これらの問題に着目し、とくに上記(2)
と(3)の点について、改善を行いさらに放電特性のす
ぐれた光電池を実現することを目的とする。
In the present invention, we focus on these problems, and in particular, the above (2)
The purpose of the present invention is to improve the points (3) and to realize a photovoltaic cell with even better discharge characteristics.

すなわち、従来においては、ルチル型二酸化チタンの単
結晶体、あるいはその粉末体を焼結したものを用いるの
であるが、本発明ではこれにかえて、酸化によって表面
に二酸化チタン層を形成した、スポンジチタンあるいは
チタン粉末焼結体などの多孔体電極を採用するものであ
る。
That is, conventionally, a single crystal of rutile titanium dioxide or a sintered powder thereof is used, but in the present invention, instead of this, a sponge with a titanium dioxide layer formed on the surface by oxidation is used. A porous electrode made of titanium or titanium powder sintered body is used.

この場合には、多孔質なので、光照射面と対極に向かう
面とが裏表であっても、極板中を電解液が自由に通過す
ることができるので、イオン拡散が容易となり、反応部
分と対極との間の溶液抵抗はかなシ小さくなシ、また極
板の反応面積も三次元構造をなしているので、大巾に増
加する。
In this case, since it is porous, the electrolyte can freely pass through the electrode plate even if the light irradiation surface and the surface facing the counter electrode are front and back, facilitating ion diffusion and connecting the reaction part. The solution resistance between the electrode and the counter electrode is very small, and the reaction area of the electrode plate has a three-dimensional structure, so it increases significantly.

さらに、多孔体電極であることから、光の極板内部への
透過も可能であり、多孔体極板の内部への乱反射も、反
応に寄与し、充分光エネルギーの利用を行なうことがで
きる。
Furthermore, since it is a porous electrode, it is possible for light to pass into the inside of the electrode plate, and diffuse reflection into the inside of the porous electrode plate also contributes to the reaction, making it possible to fully utilize light energy.

一方、導電性の点からみても、連続するチタン金属導電
網の上に、ルチル型二酸化チタン層が直接形成されてい
るので、反応点から集電金属W4での近接距離は、従来
の酸化物を焼結した電極に比べて小さくなり、電極抵抗
は著しく小さくなる。
On the other hand, from the viewpoint of conductivity, since the rutile-type titanium dioxide layer is directly formed on the continuous titanium metal conductive network, the proximity distance from the reaction point to the current collecting metal W4 is smaller than that of the conventional oxide. The electrode resistance is significantly smaller than that of a sintered electrode.

さて、表面に酢化層を有する電極としては、スクリーン
状のもの、エキスパンデッド状のもの、あるいはパンチ
ング板状のものなどが考えられるが、この場合には、イ
オンの透過性はよくなるが、極板の反応面積は小さくな
るし、上記極板は平面的なので、極板の孔を通過した光
量は損失することになる。
Now, as an electrode having an acetylated layer on the surface, it is possible to use a screen-shaped electrode, an expanded electrode, or a punched plate-shaped electrode.In this case, the ion permeability is improved, but The reaction area of the electrode plate becomes small, and since the electrode plate is flat, the amount of light passing through the holes in the electrode plate is lost.

したがって、必ずしも有効とは限らない。Therefore, it is not necessarily effective.

これらのことから、本発明の表面を酸化して、二酸化チ
タン層を形成したチタン金属多孔体電極の方が、従来の
ものより大巾に上回る電流をとりだすことができる。
For these reasons, the titanium metal porous electrode of the present invention, whose surface is oxidized to form a titanium dioxide layer, can extract a much higher current than the conventional electrode.

以下実施例によって、本発明の特徴と効果を説明する。The features and effects of the present invention will be explained below with reference to Examples.

1ず、本発明の光電極を第1図に示す。First, the photoelectrode of the present invention is shown in FIG.

図中、1は金属チタン層、2は二酸化チタン層、3は空
孔、4はリードである。
In the figure, 1 is a metal titanium layer, 2 is a titanium dioxide layer, 3 is a hole, and 4 is a lead.

なお、この第1図の光電極5は数μから数nの孔を有す
るスポンジチタンを1200℃の温度で、酸素雰囲気中
において熱処理したものである。
The photoelectrode 5 shown in FIG. 1 is made of titanium sponge having pores ranging from several microns to several nanometers and heat-treated at a temperature of 1200° C. in an oxygen atmosphere.

ここで熱処理温度を1200℃としたが、1040℃以
上であれば何度でもよい。
Here, the heat treatment temperature was set at 1200°C, but any temperature may be used as long as it is 1040°C or higher.

その理由は、光電極の二酸化チタンはルチル型が好まし
く、ルチル型が得られる温度は1040℃以上だからで
ある。
The reason is that the titanium dioxide of the photoelectrode is preferably a rutile type, and the temperature at which the rutile type is obtained is 1040° C. or higher.

こうして得られた光電極と、酸素(空気)極とを組み合
わせた光電池をAとする。
A photovoltaic cell combining the thus obtained photoelectrode and an oxygen (air) electrode is designated as A.

この光電池の概略を第2図に示す。A schematic diagram of this photovoltaic cell is shown in FIG.

5は前記の光電極で、大きさは縦10s+sX横10u
×厚さ2uである。
5 is the photoelectrode mentioned above, and its size is 10s long x 10u wide
x Thickness: 2u.

6は空気極で縦10n×横10mである。6 is an air electrode, which is 10n long by 10m wide.

7は1ノルマルのKOH水溶液、8はエポキシ樹脂の電
槽、9は光を透過するための石英ガラス、10は電槽の
蓋、11は電極5のリードでエポキシ樹脂で被ふくして
いる。
7 is a 1N KOH aqueous solution, 8 is an epoxy resin container, 9 is quartz glass for transmitting light, 10 is the lid of the container, and 11 is the lead of the electrode 5, which is covered with epoxy resin.

12は空気極6のリード、13は光源で、500Wの高
圧水銀ランプ、14はガス抜き孔である。
12 is a lead of the air electrode 6, 13 is a light source, which is a 500W high-pressure mercury lamp, and 14 is a gas vent hole.

比較のため、従来光電気化学的に活性であると言われて
いるルチル型二酸化チタンの単結晶を粉砕し、これを焼
結して大きさ縦10imX横10簡×厚さ2fiの多孔
体とし、これに光を受ける面と反対の面よシ集電体のチ
タンネットを銀ペーストを介して密着させ、Aと同様の
構成で光電池を組みたてた。
For comparison, a single crystal of rutile titanium dioxide, which is conventionally said to be photoelectrochemically active, was crushed and sintered to form a porous body with dimensions of 10 mm long x 10 mm wide x 2 fi thick. A photovoltaic cell was assembled in the same manner as in A by adhering a titanium net as a current collector to this via silver paste on the opposite side of the light-receiving surface.

これをBとする。さらに同様に金属チタン面を酸化し金
属上にチタンの光電気化学的に活性な酸化物を形成する
にしても、もともとの基体の金属が多孔体であることが
どのように効果的であるかを比較する意味で、厚さ2n
のチタンの金属板を酸化雰囲気中で1200’Cで表面
酸化し、これを電極として用いた。
Let this be B. Furthermore, even if we similarly oxidize the metal titanium surface to form a photoelectrochemically active oxide of titanium on the metal, how effective is it that the original base metal is porous? For comparison, the thickness is 2n
The surface of a titanium metal plate was oxidized at 1200'C in an oxidizing atmosphere, and this was used as an electrode.

この電極を用いて同様に構成した光電池をCとする。A photovoltaic cell constructed in the same manner using this electrode is designated as C.

1ず、これらの電池を0.1mAの電流で放電して安定
させた後、分極特性を測定した。
First, these batteries were stabilized by discharging them at a current of 0.1 mA, and then their polarization characteristics were measured.

この結果を第3図に示す。The results are shown in FIG.

第3図から明らかなように、分極特性は人の方がB、C
ようはるかに良好である。
As is clear from Figure 3, the polarization characteristics of humans are higher than B and C.
Like it's much better.

A、Bの比較においては、同じく多孔体であっても、導
体が多孔体全体の骨格をなし、その骨格そのものの表面
に直結して光電気化学的に活性なルチル型二酸化チタン
が形成されることが、分極を少なくし電池特性として良
い結果を導くことを示している。
In comparing A and B, even though they are porous, the conductor forms the skeleton of the entire porous body, and is directly connected to the surface of the skeleton itself to form photoelectrochemically active rutile titanium dioxide. This has been shown to reduce polarization and lead to better battery characteristics.

人、Cの比較においては、同じく導体のチタン骨格の表
置がルチル型に酸化されたとしても、基体が板状である
場合は実施例のように他の電極と対で用いる上での特別
の配慮を電池構成上必要とすることになることを示す。
In the comparison of C and C, even if the surface of the titanium skeleton of the conductor is oxidized to the rutile type, if the substrate is plate-shaped, it is difficult to use it in pairs with other electrodes as in the example. This indicates that consideration must be given to the battery configuration.

つまシ、光電極である以上、照射面側に障害物を置くこ
とは不可能で、対極は照射と反対側に置かねばならず、
その時の照射面と対極の間には板状の導体が存在するこ
とになると、たとえ照射面での特性が優れていても、結
局、分極抵抗は犬となる。
Since it is a photoelectrode, it is impossible to place obstacles on the side of the irradiation surface, and the counter electrode must be placed on the side opposite to the irradiation side.
If a plate-shaped conductor is present between the irradiated surface and the counter electrode at that time, even if the characteristics on the irradiated surface are excellent, the polarization resistance will eventually be poor.

この点、本発明の場合は、基体を含めて全体が多孔体で
あるので、光照射側と裏面側の対極との間は金属のよう
なイオン伝導に対する障害はない。
In this regard, in the case of the present invention, since the entire body including the base is porous, there is no obstacle to ion conduction between the light irradiation side and the counter electrode on the back side, unlike metals.

このように電池設計上は、単に素子自体の活性を論する
以上に、他の電極や構成材料との関係で素子自体の構造
を論する必要がある。
In this manner, when designing a battery, it is necessary to discuss the structure of the element itself in relation to other electrodes and constituent materials, rather than simply discussing the activity of the element itself.

さらに付加すれば、素子自体の活性の比較として照射光
の障害にならないように照射側に白金対極をリング状に
配して分極すると、Cの電池で用いた電極でもAに用い
た電極と同程度の分極に近づく、このことは、板状であ
ることによる難点を除けば電気化学的な活性そのものは
Cでも高いことを示している。
Additionally, in order to compare the activity of the element itself, if a platinum counter electrode is arranged in a ring shape on the irradiation side and polarized so as not to interfere with the irradiation light, the electrode used in battery C is the same as the electrode used in battery A. This shows that the electrochemical activity itself is high even with C, except for the drawbacks due to the plate shape.

しかし、同一分極値での電流値がAの電極の場合に比べ
て80〜90%と若干低下する傾向にあるのは、もとも
と多孔体の基体を酸化した粗な表面を有するAの電極は
平滑な板を酸化したCに比べて反射率が低く、それだけ
吸収効率としては高くなることに基づくものと推察され
る。
However, the current value at the same polarization value tends to be slightly lower by 80 to 90% compared to the case of electrode A. This is because electrode A, which originally had a rough surface made by oxidizing the porous substrate, has a smooth surface. It is presumed that this is because the reflectance is lower than that of C which is an oxidized plate, and the absorption efficiency is correspondingly higher.

また、この実施例では、スポンジチタンを用いたが、チ
タン粉末の焼結体を用いた場合も、スポンジチタンと同
様な処理、すなわち1040’C以上の温度により酸化
性雰囲気中で加熱処理を行なって、光電極として、Aと
ほぼ同様の結果を得ることができた。
In addition, although titanium sponge was used in this example, when a sintered body of titanium powder is used, it can be treated in the same way as titanium sponge, that is, heat treated in an oxidizing atmosphere at a temperature of 1040'C or higher. As a result, almost the same results as A were obtained as a photoelectrode.

この場合には、粒径5oμ〜500μのチタン粉末を縦
1抽冨×横10+mX深さ2泪の大きさのアルミナ製の
型に充填し、真空中にて、1200℃の温度で1時間焼
結し、しかるのちに、酸素をIt/minの速度で約2
0分間送り込み、電極実表面を良好な酸化状態とし、こ
れを光電極としたものである。
In this case, titanium powder with a particle size of 5oμ to 500μ is filled into an alumina mold with dimensions of 1 drawer (vertical) x 10+m (horizontal) x 2 (depth), and baked in a vacuum at a temperature of 1200°C for 1 hour. After that, oxygen is added at a rate of It/min to about 2
The electrode was fed for 0 minutes to bring the actual surface of the electrode into a good oxidation state, and this was used as a photoelectrode.

以上のことから、本発明の光電池は、従来に比べて、電
池特性が大巾に上昇し、光エネルギーの有効利用をはか
る上において、その工業的価値はきわめて大きいもので
ある。
From the above, the photovoltaic cell of the present invention has significantly improved cell characteristics compared to conventional cells, and has extremely great industrial value in terms of effective utilization of light energy.

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

第1図は本発明の実施例における光電極を示す図、第2
図は同光電極を用いた光電池の概略断面図、第3図は分
極特性を示す図である。 1・・・・・・金属チタン層、2・曲・二酸化チタン層
、3・・・・・・空孔、5・・開光電極。
FIG. 1 is a diagram showing a photoelectrode in an embodiment of the present invention, and FIG.
The figure is a schematic cross-sectional view of a photovoltaic cell using the same photoelectrode, and FIG. 3 is a diagram showing polarization characteristics. DESCRIPTION OF SYMBOLS 1...Metal titanium layer, 2...Curved titanium dioxide layer, 3...Vacancy, 5...Light opening electrode.

Claims (1)

【特許請求の範囲】 1 立体的な三次元構造を有し、かつ表面に二酸化チタ
ン層を形成したチタン多孔体からなる光電極を用いたこ
とを特徴とする光電池。 2 チタン多孔体が、スポンジチタンを1040℃以上
の温度の酸化性雰囲気中で熱処理したものである特許請
求の範囲第1項記載の光電池。 3 チタン多孔体が、チタン粉末の焼結体を1040℃
以上の温度の酸化性雰囲気中で熱処理したものである特
許請求の範囲第1項記載の光電池。
[Scope of Claims] 1. A photovoltaic cell characterized by using a photoelectrode made of a porous titanium material having a three-dimensional three-dimensional structure and having a titanium dioxide layer formed on its surface. 2. The photovoltaic cell according to claim 1, wherein the titanium porous body is made by heat-treating titanium sponge in an oxidizing atmosphere at a temperature of 1040° C. or higher. 3 The titanium porous body heats the sintered body of titanium powder to 1040°C.
The photovoltaic cell according to claim 1, which has been heat-treated in an oxidizing atmosphere at a temperature above.
JP51154010A 1976-12-20 1976-12-20 photocell Expired JPS5826623B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP51154010A JPS5826623B2 (en) 1976-12-20 1976-12-20 photocell

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP51154010A JPS5826623B2 (en) 1976-12-20 1976-12-20 photocell

Publications (2)

Publication Number Publication Date
JPS5377188A JPS5377188A (en) 1978-07-08
JPS5826623B2 true JPS5826623B2 (en) 1983-06-03

Family

ID=15574926

Family Applications (1)

Application Number Title Priority Date Filing Date
JP51154010A Expired JPS5826623B2 (en) 1976-12-20 1976-12-20 photocell

Country Status (1)

Country Link
JP (1) JPS5826623B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4544470A (en) * 1984-05-31 1985-10-01 Ford Motor Company Electrochemical photocatalytic structure
CH674596A5 (en) * 1988-02-12 1990-06-15 Sulzer Ag
JP5438471B2 (en) * 2009-11-09 2014-03-12 株式会社クラレ Photovoltaic cell and photovoltaic battery

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5913831B2 (en) * 1975-03-17 1984-04-02 健一 本多 electrochemical photocell

Also Published As

Publication number Publication date
JPS5377188A (en) 1978-07-08

Similar Documents

Publication Publication Date Title
Zhang et al. Unconventional direct synthesis of Ni 3 N/Ni with N-vacancies for efficient and stable hydrogen evolution
Bu et al. Rechargeable sunlight-promoted Zn-air battery constructed by bifunctional oxygen photoelectrodes: Energy-band switching between ZnO/Cu2O and ZnO/CuO in charge-discharge cycles
Chen et al. An iron-based film for highly efficient electrocatalytic oxygen evolution from neutral aqueous solution
Singh et al. Electrochemical Studies on Protective Thin Co3 O 4 and NiCo2 O 4 Films Prepared on Titanium by Spray Pyrolysis for Oxygen Evolution
US6780347B2 (en) Manganese oxide based electrode for alkaline electrochemical system and method of its production
EP2527495B1 (en) Hydrogen generation device
Lee et al. Si-based water oxidation photoanodes conjugated with earth-abundant transition metal-based catalysts
Hanzu et al. Electrical and point defect properties of TiO2 nanotubes fabricated by electrochemical anodization
JPH05500432A (en) Proton-conducting solid electrolyte battery
Fekete et al. Photoelectrochemical water oxidation by screen printed ZnO nanoparticle films: effect of pH on catalytic activity and stability
KR100806168B1 (en) Photocatalytic Water Decomposition Hydrogen Energy Manufacturing Method Using Electromotive Force of Solar Cell
Khan et al. Stability and Photoresponse of Nanocrystalline n‐TiO2 and n‐TiO2/Mn2 O 3 Thin Film Electrodes during Water Splitting Reactions
WO2005008806A2 (en) Photoelectrolysis of water using proton exchange membranes
JP6355083B2 (en) Photocatalyst composition and method for producing the same
CN108541275A (en) Electrode of substrate(SE)Interface irradiation type optoelectronic pole and photoelectrochemical cell
Lan et al. Smart solar–metal–air batteries based on BiOCl photocorrosion for monolithic solar energy conversion and storage
EP0553023B1 (en) Photochargeable air battery
JP4568124B2 (en) Air electrode and air secondary battery using the air electrode
JPH01227361A (en) Manufacture of anode for fuel cell
Zhou et al. Enhanced photo-electrochemical water oxidation on MnO x in buffered organic/inorganic electrolytes
JPS5826623B2 (en) photocell
CN104549233A (en) Preparation method of fuel cell anode catalyst
JP2014216059A (en) Secondary battery having graphene oxide as solid electrolyte
JP5375545B2 (en) Solid electrolyte fuel cell and manufacturing method thereof
Hada et al. Energy conversion and storage in solid-state photogalvanic cells.