概括
我们理论上证明了在合成光子系统中以偏振控制的布洛赫振荡. 灯光 灯光 灯光 灯光
科学领域:
- 光子学是指光子学的使用方法.
- 量子光学是一种量子光学.
- 凝聚物质理论 凝聚物质理论
背景情况:
- 布洛赫振荡是基本的量子现象.
- 光子系统为模拟量子动力学提供了平台.
- 极化控制是操纵光属性的关键.
研究的目的:
- 理论上研究合成光子系统中受偏振控制的布洛赫振荡.
- 探索光极化在指导布洛赫振荡中的作用.
- 在这个框架内演示光学Zener道.
主要方法:
- 合成双层光子系统的理论建模.
- 使用水平和垂直光极化模拟伪脊柱状态.
- 在光晶相互作用过程中合成磁格子.
主要成果:
- 证明了极化光的方向布洛赫振荡.
- 观察到伴随布洛赫振荡的光学泽纳道.
- 通过事件光极化 (自转向上,自转向下和混合) 展示了布洛赫振荡的控制.
- 扩展了形式主义以实现拓旋转纹理的布洛赫振荡.
结论:
- 合成光子系统中的布洛克振荡可以通过事件光极化来有效控制.
- 提出的框架为光学信息处理设备提供了潜在的应用.
- 偏振控制的布洛赫振荡为光子系统中操纵光开辟了新的途径.
相关概念视频
Atomic Nuclei: Nuclear Relaxation Processes
1.2K
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
1.2K
Spin–Spin Coupling Constant: Overview
1.4K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.4K
Valence Bond Theory
11.1K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
11.1K
Atomic Nuclei: Nuclear Spin State Overview
1.9K
NMR-active nuclei have energy levels called 'spin states' that are associated with the orientations of their nuclear magnetic moments. In the absence of a magnetic field, the nuclear magnetic moments are randomly oriented, and the spin states are degenerate. When an external magnetic field is applied, the spin states have only 2 + 1 orientations available to them. A proton with = ½ has two available orientations. Similarly, for a quadrupolar nucleus with a nuclear spin value of one, the...
1.9K
Atomic Nuclei: Magnetic Resonance
1.1K
The number of nuclear spins aligned in the lower energy state is slightly greater than those in the higher energy state. In the presence of an external magnetic field, as the spins precess at the Larmor frequency, the excess population results in a net magnetization oriented along the z axis. When a pulse or a short burst of radio waves at the Larmor frequency is applied along the x axis, the coupling of frequencies causes resonance and flips the nuclear spins of the excess population from the...
1.1K
Spin–Spin Coupling: One-Bond Coupling
1.4K
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,...
1.4K


