在 ^{9}Be^{+} 中使用单个被困离子测量D线的绝对频率
D M Fairbank1, A L Banducci1, R W Gunkelman1
1Department of Physics, Colorado State University, Fort Collins, Colorado 80523, USA.
Physical review letters
|September 18, 2023
概括
研究人员精确测量了^{9}Be^{+} D线过渡的光学频率,在被困离子中实现了电偶极允许过渡的记录精度. 这一进步改善了原子光谱学和基本物理学的理解.
科学领域:
- 原子物理 原子物理
- 量子光学是一种量子光学.
- 频谱学是一种光谱学.
背景情况:
- 被困离子实验对于高精度测量至关重要.
- 电二极允许 (E1) 过渡提供了有价值的原子结构信息.
- 之前对^{9}Be^{+}D线的测量在精度上有局限性.
研究的目的:
- 用前所未有的精度测量D线过渡的光学频率在^{9}Be^{+}中.
- 为了提高原子光谱学对被困离子的精度.
- 为了提取基本的原子参数,如细结构分裂和超细常数.
主要方法:
- 使用一个单个激光冷却的离子储存在无线电频率保罗陷中.
- 采用了一种光谱激光器,该激光器被稳定到光学频率.
- 通过NIST,将测量值转换为协调普世时间 (UTC).
- 仔细考虑了光子反弹和量子干扰效应.
主要成果:
- 获得了D直线过渡的Δν/ν=5×10^{-11}的相对不确定性.
- 与之前的工作相比,不确定性减少了10 (D1) 和30 (D2) 的因素.
- 提取了 ^{2}P 细结构分割 (Δνfs) 的 197,064.54(7) MHz.
- 确定 ^{2}P_{1/2} 超精度常数 (A P1/2) 是 -117.92(4) MHz.
结论:
- 这项研究证明了迄今为止被困离子实验中E1过渡的最高精度.
- 提高精度为测试基本物理和改进原子钟开辟了新的途径.
- 提取的原子参数为原子结构理论提供了关键数据.
相关概念视频
Mass Analyzers: Common Types
642
The quadrupole mass analyzer consists of four cylindrical metal rods arranged in a diamond carrying a DC voltage and a radio-frequency AC voltage. The motion of ions through the quadrupole depends on the field strength, causing only ions of a certain m/z to resonate successfully and strike the detector at a given field strength. Though the transmission rate for these analyzers is high, the exact elemental composition of the sample is not determined because of low resolution; however, they are...
642
Atomic Nuclei: Larmor Precession Frequency
1.5K
The earth's gravitational field produces a 'twisting force' perpendicular to the angular momentum of a spinning mass (such as a spinning top) that causes the mass to 'wobble' around the gravitational field axis in a phenomenon called precession. Similarly, the magnetic moment (μ) of a spinning nucleus precesses due to an external magnetic field directed along the z-axis. The precession of the magnetic moment vector about the magnetic field is called Larmor precession,...
1.5K
¹H NMR: Interpreting Distorted and Overlapping Signals
1.1K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.1K
Atomic Nuclei: Nuclear Relaxation Processes
676
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.
676
¹³C NMR: ¹H–¹³C Decoupling
1.1K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.1K
Atomic Nuclei: Nuclear Spin State Population Distribution
1.0K
Near absolute zero temperatures, in the presence of a magnetic field, the majority of nuclei prefer the lower energy spin-up state to the higher energy spin-down state. As temperatures increase, the energy from thermal collisions distributes the spins more equally between the two states. The Boltzmann distribution equation gives the ratio of the number of spins predicted in the spin −½ (N−) and spin +½ (N+) states.
1.0K


