由正交叠的范德瓦尔斯NbOCl2晶体实现的极化纠
Qiangbing Guo1,2, Yun-Kun Wu3,4,5, Di Zhang6,7
1Department of Electrical and Computer Engineering, National University of Singapore, Singapore, Singapore. qbguo90@hotmail.com.
Nature communications
|December 2, 2024
概括
研究人员使用扭曲堆叠的范德瓦尔斯NbOCl2晶体实现了极化纠和量子贝尔状态. 这克服了先前用于先进光子量子技术的材料的局限性.
科学领域:
- 量子光学就是一个量子光学.
- 材料科学 是一种材料科学.
- 凝聚物质物理学 凝聚物质物理学
背景情况:
- 极化纠对于光子量子技术至关重要.
- 像GaP和LiNbO3薄膜这样的低波长非线性量子光源提供了优势.
- 范德瓦尔斯 (vdW) NbOCl2晶体具有强烈的光学非线性,但由于其非线性易感度张量,缺乏极化纠能力.
研究的目的:
- 为了克服NbOCl2晶体中极化纠的难以接近.
- 探索VDW系统在产生极化纠方面的潜力.
- 为了证明使用工程VDW材料准备量子贝尔状态.
主要方法:
- 在VDW系统中利用旋转堆叠的自由度.
- 制造工程NbOCl2晶体结构.
- 描述生成的量子状态.
主要成果:
- 在vdW NbOCl2晶体中成功制备了极化纠.
- 证明了量子贝尔状态的产生.
- 利用材料堆叠来设计非线性光学特性.
结论:
- 扭曲堆叠VDW材料提供了一种新的途径来实现极化纠.
- 这种方法可以开发具有增强功能的超薄量子光源.
- 这些发现为先进的光子量子技术开辟了新的途径.
相关概念视频
Potential Due to a Polarized Object
365
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
365
Dielectric Polarization in a Capacitor
4.6K
The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
4.6K
Hybridization of Atomic Orbitals I
46.5K
The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
46.5K
Ionic Crystal Structures
14.1K
Ionic crystals consist of two or more different kinds of ions that usually have different sizes. The packing of these ions into a crystal structure is more complex than the packing of metal atoms that are the same size.
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
Most monatomic ions behave as charged spheres, and their attraction for ions of opposite charge is the same in every direction. Consequently, stable structures for ionic compounds result (1) when ions of one charge are surrounded by as many ions as possible of the opposite...
14.1K
Crystal Field Theory - Tetrahedral and Square Planar Complexes
41.5K
Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
41.5K
Metallic Solids
18.2K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
18.2K


