从单层到散装:分子半导体的薄膜特定多态转换
Nobutaka Shioya1, Fabian Gasser2, Nina Strasser2
1Institute for Chemical Research, Kyoto University, Gokasho, Uji, Kyoto 611-0011, Japan.
概括
这项研究揭示了dinaphtho-[2,3-b:2:2中的三个不同的晶体结构.
科学领域:
- 材料科学 材料科学 材料科学
- 有机电子 有机电子
- 晶体学 晶体学是指结晶学.
背景情况:
- 有机化合物形成薄膜和单层相,其特性对设备性能至关重要.
- 许多薄膜相仍然未被识别,阻碍了结构-属性关系分析.
- 迪纳弗托-[2,3-b:2',3'-f]-thieno-[3,2-b]-thiophene (DNTT) 是一个基准的有机半导体,但它的多态性是研究不足的.
研究的目的:
- 为了全面了解有机半导体中的多态转换.
- 为了研究DNTT蒸气沉积薄膜的厚度依赖结构变化.
- 识别和描述有机材料未知的薄膜相.
主要方法:
- 高分辨率红外布鲁斯特角度传输光谱学.
- 牧场发生率X射线衍射.
- 密度函数理论计算.
主要成果:
- 在基于厚度的DNTT膜中识别了三种不同的晶体结构:单层,薄膜和散装相.
- 确定单层阶段的结构溶液.
- 获得了薄膜阶段的候选结构.
结论:
- 建立了有机半导体薄膜生长的整体模型.
- 展示了分析和建模技术的强大组合,用于识别新的有机薄膜相.
- 进一步了解DNTT多态化及其对有机电子学的影响.
更多相关视频
相关概念视频
Types of Semiconductors
1.5K
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...
1.5K
Fermi Level Dynamics
763
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
763
Fermi Level
1.9K
The Fermi-Dirac function is represented by an S-shaped curve indicating the probability of an energy state being occupied by an electron at a given temperature. The Fermi level is the energy level at which there is a fifty percent chance of finding an electron, and it is positioned between the lower-energy valence band and the higher-energy conduction band.
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
At absolute zero temperature, electrons fill all energy states up to the Fermi level, leaving upper states empty. As the temperature rises,...
1.9K
Metal-Semiconductor Junctions
1.1K
The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
1.1K


