オーガニック半導体のバンド構造工学
Martin Schwarze1, Wolfgang Tress2, Beatrice Beyer3
1Institut für Angewandte Photophysik, Technische Universität Dresden, 01069 Dresden, Germany.
まとめ
研究者達は 有機半導体を ハロゲン製の誘導体と混ぜて設計しました この方法は有機太陽電池の電離エネルギーや 光電性能などの 電子特性を調整します
科学分野:
- 材料科学
- オーガニック電子
- 固体物理学
背景:
- バンド構造の工学は現代の電子機器にとって不可欠であり,調節可能な電子特性を可能にします.
- 有機半導体は,強い電子状態の局所化により,帯域構造工学に課題を提示する.
研究 の 目的:
- 有機半導体における電子状態の局所化の限界を克服する.
- オーガニック半導体の電子特性を継続的に調整する方法を実証する.
主な方法:
- 有機半導体とそのハロゲン誘導体の混合を用いる.
- イオン化エネルギーを測定するために光電子スペクトロスコーピーを用いた.
- 有機太陽電池を製造し,特徴づけ,光伏の性能を評価する.
主要な成果:
- 広範囲にわたる結晶有機半導体における電離エネルギーの継続的な調整を証明した.
- 有機太陽電池の光伏ギャップとオープン回路の電圧の継続的な調節性を示しました.
- 遠距離クーロン相互作用が,このトナビリティを実現する役割を強調した.
結論:
- 有機半導体とハロゲン誘導体の混合は,バンド構造工学の実行可能な戦略を提供します.
- 長期カロン相互作用は有機システムにおける局所効果を克服する鍵となる.
- このアプローチは,高度な有機電子デバイスの光電子特性に対する正確な制御を可能にします.
さらに関連する動画
関連する概念動画
Band Theory
17.7K
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
17.7K
Energy Bands in Solids
2.3K
Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
2.3K
Semiconductors
1.8K
There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
1.8K
Structure of Benzene: Molecular Orbital Model
13.5K
According to the molecular orbital (MO) model, benzene has a planar structure with a regular hexagon of six sp2 hybridized carbons. As shown in Figure 1, each carbon is bonded to three other atoms with C–C–C and H–C–C bond angles of 120°. The C–H bond length is 109 pm, and the C–C bond length is 139 pm which is midway between the single bond length of sp3 hybridized carbons (154 pm) and sp2 hybridized carbons (133 pm).
13.5K
Resonance and Hybrid Structures
28.6K
According to the theory of resonance, if two or more Lewis structures with the same arrangement of atoms can be written for a molecule, ion, or radical, the actual distribution of electrons is an average of that shown by the various Lewis structures.
Resonance Structures and Resonance Hybrids
The Lewis structure of a nitrite anion (NO2−) may actually be drawn in two different ways, distinguished by the locations of the N–O and N=O bonds.
Resonance Structures and Resonance Hybrids
The Lewis structure of a nitrite anion (NO2−) may actually be drawn in two different ways, distinguished by the locations of the N–O and N=O bonds.
28.6K
Types of Semiconductors
1.7K
Intrinsic semiconductors are highly pure materials with no impurities. At absolute zero, these semiconductors behave as perfect insulators because all the valence electrons are bound, and the conduction band is empty, disallowing electrical conduction. The Fermi level is a concept used to describe the probability of occupancy of energy levels by electrons at thermal equilibrium. In intrinsic semiconductors, the Fermi level is positioned at the midpoint of the energy gap at absolute zero. When...
1.7K


