異なるステキオメトリーで電荷キャリアの生成と輸送 APFO3:PC61BM 太陽電池
Vytenis Pranculis1, Yingyot Infahsaeng, Zheng Tang
1Center for Physical Sciences and Technology , Savanoriu 231, LT-02300 Vilnius, Lithuania.
Journal of the American Chemical Society
|July 16, 2014
まとめ
APFO3:PC61BMの太陽電池を調査すると,キャリア漂流と抽出ダイナミクスはステキオメトリーに大きく依存していることが明らかになる. より速い電子運動は,効率的な電荷分離と高い太陽電池効率に不可欠です.
科学分野:
- 有機太陽光発電は,有機太陽光発電です.
- 半導体デバイス物理学の物理
- マテリアルサイエンス 材料科学
背景:
- チャージキャリアダイナミクスを理解することは,有機太陽電池の性能を最適化するために重要です.
- ドナーと受容体の混合物のステキオメトリーは,デバイスの効率に大きく影響します.
研究 の 目的:
- 異なるステキオメトリーを持つ太陽電池でキャリアの漂流と抽出のダイナミクスを調査する.
- キャリアダイナミクスを太陽電池の変換効率と相関させるため.
主な方法:
- 超高速光学電場探査と一時的な統合光電流技術を使用しました.
- 研究したAPFO3:PC61BM太陽電池は,ステキオメトリーが 2:1, 1:1, 1:4.
- 分析されたキャリアダイナミクスは,サブピコ秒からマイクロ秒までの時間帯に及ぶ.
主要な成果:
- キャリアの漂流と抽出は,ステキオメトリーに強く依存しています.
- 電子のドリフトと抽出速度は,PC61BM濃度が高くなるにつれて増加します.
- 穴の抽出は,電子抽出と比較してステキオメトリーにあまり依存していません.
結論:
- 素早い電子運動は,高効率な電荷载体分離とゲミナート再結合の防止に不可欠である.
- ステキオメトリーの最適化は,電子抽出と太陽電池全体の効率を高めるための鍵です.
さらに関連する動画
06:49In situ Grazing Incidence Small Angle X-ray Scattering on Roll-To-Roll Coating of Organic Solar Cells with Laboratory X-ray Instrumentation
Published on: March 2, 2021
6.8K
11:38Influence of Hybrid Perovskite Fabrication Methods on Film Formation, Electronic Structure, and Solar Cell Performance
Published on: February 27, 2017
20.0K
関連する概念動画
P-N junction
1.6K
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
1.6K
Carrier Generation and Recombination
1.5K
Carrier generation is the process by which electron-hole pairs (EHPs) are created within the semiconductor. In direct-bandgap semiconductors, such as gallium arsenide (GaAs), this occurs efficiently when energy absorption prompts valence electrons to leap into the conduction band, leaving behind holes.
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
This process is given by the generation rate G and is efficient due to the conservation of momentum between the valence band maximum and conduction band minimum.
Indirect generation involves an...
1.5K
The Z-Scheme of Electron Transport in Photosynthesis
12.6K
The light reactions of photosynthesis assume a linear flow of electrons from water to NADP+. During this process, light energy drives the splitting of water molecules to produce oxygen. However, oxidation of water molecules is a thermodynamically unfavorable reaction and requires a strong oxidizing agent. This is accomplished by the first product of light reactions: oxidized P680 (or P680+), the most powerful oxidizing agent known in biology. The oxidized P680 that acquires an electron from the...
12.6K
Carrier Transport
1.2K
The generation of electrical current in semiconductors is fundamentally driven by two mechanisms: drift and diffusion. These processes are essential for the functionality and performance of semiconductor-based devices.
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
Drift Current:
The drift of charge carriers is started by an external electric field (E). Charged particles, such as electrons and holes, experience an acceleration between collisions with lattice atoms. For electrons, this results in a drift velocity (vd) given by:
1.2K
Photosystem I
52.7K
Although structurally similar to photosystem II (PSII), photosystem I (PSI) is has a different electron supplier and electron acceptor.
Both these photosystems work in concert. An excited electron from PSII is relayed to PSI via an electron transport chain in the thylakoid membrane of the chloroplast, which is comprised of the carrier molecule plastoquinone, the dual-protein cytochrome complex, and plastocyanin. As electrons move between PSII and PSI, they lose energy and must be re-energized...
Both these photosystems work in concert. An excited electron from PSII is relayed to PSI via an electron transport chain in the thylakoid membrane of the chloroplast, which is comprised of the carrier molecule plastoquinone, the dual-protein cytochrome complex, and plastocyanin. As electrons move between PSII and PSI, they lose energy and must be re-energized...
52.7K
