通过双极相互作用在弱驱动的多层原子阵列中产生纠
Sanaa Agarwal1,2, A Piñeiro Orioli3,4, J K Thompson1
1<a href="https://ror.org/008hybe55">JILA</a>, NIST, Department of Physics, <a href="https://ror.org/02ttsq026">University of Colorado</a>, Boulder, Colorado 80309, USA.
Physical review letters
|December 23, 2024
概括
阵列中的多层原子可以变得强烈纠,形成自旋波,在激发后持续存在. 这项研究提出了-88作为探索光物质相互作用和多体物理学的平台.
科学领域:
- 原子物理 原子物理
- 量子光学就是一个量子光学.
- 凝聚物质理论 凝聚物质理论
背景情况:
- 驱动散流系统中的双层原子已经得到了很好的研究.
- 多层原子提供更丰富的量子现象,由于更复杂的能量层结构.
- 原子数组中的双极相互作用可以导致集体量子效应.
研究的目的:
- 在多层原子阵列中研究驱动散流动力学.
- 探索强纠及其在这些系统中的表现.
- 提出一个特定的实验平台来观察这些现象.
主要方法:
- 驱动散流动力学的理论研究.
- 在亚波长间隔的多层原子阵列中的相互作用分析.
- 纠增长和旋波动态的建模.
主要成果:
- 多层原子表现出强烈的纠,与两层系统不同.
- 纠表现为旋转波在基本状态多元体中的增长.
- 观察到的旋转波在外部驱动器关闭后仍然存在.
结论:
- 多层原子阵列为强纠和持续的旋转波提供了通路.
- 拟议的-88系统为实验验证提供了一个可行的平台.
- 这项工作为探索光物相互作用的多体物理学开辟了道路.
相关概念视频
Atomic Nuclei: Nuclear Relaxation Processes
622
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.
622
Van der Waals Interactions
63.5K
Atoms and molecules interact with each other through intermolecular forces. These electrostatic forces arise from attractive or repulsive interactions between particles with permanent, partial, or temporary charges. The intermolecular forces between neutral atoms and molecules are ion–dipole, dipole–dipole, and dispersion forces, collectively known as van der Waals forces.
63.5K
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
959
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
959
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
Intermolecular Forces
57.6K
Atoms and molecules interact through bonds (or forces): intramolecular and intermolecular. The forces are electrostatic as they arise from interactions (attractive or repulsive) between charged species (permanent, partial, or temporary charges) and exist with varying strengths between ions, polar, nonpolar, and neutral molecules. The different types of intermolecular forces are ion–dipole, dipole–dipole, hydrogen bonds, and dispersion; among these, dipole–dipole, hydrogen...
57.6K
Atomic Nuclei: Nuclear Spin State Overview
866
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...
866


