绿色发光半导体的材料设计:矿型硫化物 SrHfS3
Kota Hanzawa1, Soshi Iimura1, Hidenori Hiramatsu1,2
1Laboratory for Materials and Structures, Institute of Innovative Research , Tokyo Institute of Technology , Mailbox R3-3, 4259 Nagatsuta-cho, Midori-ku , Yokohama 226-8503 , Japan.
Journal of the American Chemical Society
|March 7, 2019
概括
研究人员发现了一种有前途的半导体材料,即石三硫化物 (SrHfS3),用于设备中有效发射绿色光. 这种材料提供可调节的导电性和载体极性,解决了光电子领域的一个关键挑战.
科学领域:
- 材料科学
- 固态物理
- 光电子产品
背景情况:
- 开发高效的绿色发光材料对于先进的发光设备至关重要.
- 现有的材料往往缺乏稳定和高效的绿光发射所需的特性.
研究的目的:
- 探索以早期过渡金属 (eTM) 为基础的矿的绿光发射.
- 为光电子应用确定具有特定电子带结构和可控制性质的半导体.
主要方法:
- 对深导带最小值 (CBM) 和浅价值带最大值 (VBM) 进行了研究.
- 采用带折叠技术来实现绿色排放的直接带隙.
- 用 (La) 和 (P) 合成和合Orthorhombic SrHfS3以调整导电性和载体极性.
主要成果:
- 在SrHfS3中实现可调节的电导率从6 × 10−7到7 × 10−1 S·cm−1 (La注) 和2 × 10−4 S·cm−1 (P注).
- 成功控制载体极性到n型通过La注和p型通过P注.
- 在未使用和使用的SrHfS3中观察到强烈的绿色光发光 (PL),这归因于波段到波段的转换或激子.
结论:
- hafnium trisulfide (SrHfS3) 显示出作为绿色发光应用的高效半导体的潜力.
- 该材料可调节的电子特性和强烈的绿色发射使其成为克服光电子现有局限性的可行候选者.
相关概念视频
Types of Semiconductors
1.4K
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...
1.4K
Semiconductors
1.5K
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...
1.5K
Preparation and Reactions of Sulfides
5.8K
Sulfides are the sulfur analog of ethers, just as thiols are the sulfur analog of alcohol. Like ethers, sulfides also consist of two hydrocarbon groups bonded to the central sulfur atom. Depending upon the type of groups present, sulfides can be symmetrical or asymmetrical. Symmetrical sulfides can be prepared via an SN2 reaction between 2 equivalents of an alkyl halide and one equivalent of sodium sulfide.
5.8K
Structure and Nomenclature of Thiols and Sulfides
5.7K
Thiols and sulfides are sulfur analogs of alcohols and ethers, respectively, where the sulfur atom takes the place of the oxygen atom. Thus, thiols are generally represented as RSH, where R is an alkyl substituent and —SH is the functional group. On the other hand, in sulfides, the central sulfur atom is bonded to two hydrocarbon groups on either side. Depending upon the type of group, sulfides can be either symmetrical or asymmetrical. Both thiols and sulfides display a bent geometry,...
5.7K
Metal-Semiconductor Junctions
953
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...
953
Types of Radioactivity
19.6K
The most common types of radioactivity are α decay, β decay, γ decay, neutron emission, and electron capture.
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
19.6K


