相关实验视频
Updated: Jun 2, 2025

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
12.8K
在里德伯格原子阵列中探测量子浮动相
Jin Zhang1,2,3, Sergio H Cantú4, Fangli Liu5
1Department of Physics and Astronomy, University of Iowa, Iowa City, IA, USA. jzhang91@cqu.edu.cn.
Nature communications
|January 17, 2025
概括
研究人员通过实验观察了中性原子量子比特中的量子浮动相. 这种不相称的阶段是从有序阶段的域壁增殖中产生的,呈现出准远程秩序.
科学领域:
- 量子物理学的量子物理学
- 凝聚物质物理学 凝聚物质物理学
- 原子物理 原子物理
背景情况:
- 浮动阶段是一个理论上预测的不相称的阶段.
- 假设它存在于晶体有序和无序相之间.
- 了解这些阶段是量子多体系统的关键.
研究的目的:
- 为了实验性地研究中性原子梯子阵列中的量子相.
- 为了观察量子浮动相的出现.
- 分析这个不相称的阶段的特征.
主要方法:
- 在梯子数组中使用中性原子量子比特 (最多92个量子比特).
- 进行了Rydberg状态密度的现场解析测量.
- 分析了密度密度相关的里埃光谱.
主要成果:
- 通过实验观察了量子浮动相.
- 识别了导致浮动阶段的域壁扩散.
- 通过富里埃分析检测到不相称的波序的签名.
- 观察到波向量靠近连续性随着系统大小的增加.
结论:
- 这项研究提供了量子浮动相的实验证据.
- 证明了从相称的顺序过渡到不相称的近距离远程顺序.
- 激励对相称-不相称过渡和非平衡物理学的进一步研究.
更多相关视频
相关概念视频
The Quantum-Mechanical Model of an Atom
41.9K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
41.9K
The Bohr Model
50.8K
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
50.8K
The de Broglie Wavelength
25.3K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.3K
¹H NMR: Complex Splitting
1.2K
A proton M that is coupled to a proton X results in doublet signals for M. However, NMR-active nuclei can be simultaneously coupled to more than one nonequivalent nucleus. When M is coupled to a second proton A, such as in styrene oxide, each peak in the doublet is split into another doublet.
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied...
Splitting diagrams or splitting tree diagrams are routinely used to depict such complex couplings. While drawing splitting diagrams, the splitting with the larger coupling constant is usually applied...
1.2K
Double Resonance Techniques: Overview
185
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
185
Emission Spectra
50.4K
When solids, liquids, or condensed gases are heated sufficiently, they radiate some of the excess energy as light. Photons produced in this manner have a range of energies, and thereby produce a continuous spectrum in which an unbroken series of wavelengths is present.
50.4K

