具有远程合的拓度链的波函数断层扫描.
F Pellerin1, R Houvenaghel2, W A Coish3
1Département de Physique, Université de Montréal, C.P. 6128, Succursale Centre-Ville, Montréal, Québec H3C 3J7, Canada.
Physical review letters
|May 17, 2024
概括
研究人员设计了具有可调节的远程跳跃的光子二元链,将Su-Schrieffer-Heeger模型通用化. 这使得能够精确地控制物质的拓相,使用合成尺寸场.
科学领域:
- 凝聚物质物理学 凝聚物质物理学
- 量子光学是一种量子光学.
- 光子学 是一个光子学.
背景情况:
- 在格子中定制网站间连接是新型拓阶段的关键.
- 像Su-Schrieffer-Heeger这样的传统模型仅限于最近邻合器.
研究的目的:
- 实验实现可调节的远程跳转的光子二元链.
- 将苏-施里弗-希格尔模型用任意的跳跃强度和相位进行概括.
- 探索由合成尺寸场所驱动的拓相位过渡.
主要方法:
- 在光纤循环中使用合成维度方案与频率模式.
- 直接访问带分散和布洛赫波函数几何.
- 提取各种配置的绕线号码.
主要成果:
- 成功创建了可控远程跳跃的光子二元链.
- 一个通用的Su-Schrieffer-Heeger模型的演示.
- 观察由合成尺寸场诱导的拓相位过渡.
结论:
- 这项工作为在光子网格中工程拓带提供了一个多功能平台.
- 这些发现提供了一条通往物质新型拓相的途径.
- 该系统属于AIII对称类,使其具有特定的拓性质.
相关概念视频
¹H NMR: Long-Range Coupling
1.7K
The coupling interactions of nuclei across four or more bonds are usually weak, with J values less than 1 Hz. While these are usually not observed in spectra, the presence of multiple bonds along the coupling pathway can result in observable long-range coupling.
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
In alkenes, spin information is communicated via σ–π overlap, as seen in allylic (four-bond) and homoallylic (five-bond) couplings. These coupling interactions are stronger when the σ bond is parallel to the alkene...
1.7K
¹H NMR of Conformationally Flexible Molecules: Temporal Resolution
831
At room temperature, the chair conformer of cyclohexane undergoes rapid ring flipping between two equivalent chair conformers at a rate of approximately 105 times per second. These two chair conformers are in equilibrium. The rapid ring flipping results in the interconversion of the axial proton to an equatorial proton and an equatorial to the axial proton. Such interconversions are too rapid and cannot be detected on the NMR timescale. Hence, the NMR spectrometer cannot distinguish between the...
831
NMR Spectroscopy: Spin–Spin Coupling
1.3K
The spin state of an NMR-active nucleus can have a slight effect on its immediate electronic environment. This effect propagates through the intervening bonds and affects the electronic environments of NMR-active nuclei up to three bonds away; occasionally, even farther. This phenomenon is called spin–spin coupling or J-coupling. Coupling interactions are mutual and result in small changes in the absorption frequencies of both nuclei involved. While nuclei of the same element are involved...
1.3K
Spin–Spin Coupling: One-Bond Coupling
957
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
957
Network Covalent Solids
13.4K
Network covalent solids contain a three-dimensional network of covalently bonded atoms as found in the crystal structures of nonmetals like diamond, graphite, silicon, and some covalent compounds, such as silicon dioxide (sand) and silicon carbide (carborundum, the abrasive on sandpaper). Many minerals have networks of covalent bonds.
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
To break or to melt a covalent network solid, covalent bonds must be broken. Because covalent bonds are relatively strong, covalent network solids are typically...
13.4K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)
1.1K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the...
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the...
1.1K


