测量正子子异常磁矩到127ppb的测量
D P Aguillard1, T Albahri2, D Allspach3
1University of Michigan, Ann Arbor, Michigan, USA.
Physical review letters
|September 22, 2025
概括
在FNAL的Muon g-2实验提出了一个新的测量子.
科学领域:
- 粒子物理学 粒子物理学
- 量子场理论 量子场理论
- 电磁主义 电磁主义
背景情况:
- 子 (a_μ) 的磁异常是粒子物理学中的一个基本参数.
- 理论预测和a_μ的实验测量之间的差异可能表明标准模型之外的新物理学.
研究的目的:
- 为了呈现一个新的,更精确的测量子的磁异常 (a_μ).
- 为了提高 a_μ.μ. 的实验世界平均值的精度.
主要方法:
- 由费米国家加速器实验室 (FNAL) Muon g-2实验收集的2020-2023年的数据.
- 基于存储环磁场中子和质子的前行频率比的测量.
- 利用了基本常数的精确已知的比率.
主要成果:
- 数据集的新测量结果是: a_μ = 1.165920710(162) × 10−12 (139 ppb).
- 与以前的结果相结合的测量: a_μ = 1.165920705(148) × 10−12 (127 ppb).
- 全球新实验平均值:a_μ(exp) = 1.165920715(145) × 10−12 (124 ppb) 的值.
结论:
- FNAL Muon g-2实验显著提高了a_μ的世界平均值的精度,超过4.
- 增加的统计数据和精度为进一步探索潜在的新物理学铺平了道路.
更多相关视频
10:42Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
7.3K
08:42High-Sensitivity Nuclear Magnetic Resonance at Giga-Pascal Pressures: A New Tool for Probing Electronic and Chemical Properties of Condensed Matter under Extreme Conditions
Published on: October 10, 2014
11.9K
相关概念视频
Atomic Nuclei: Nuclear Magnetic Moment
3.1K
All atomic nuclei are positively charged. When they have a nonzero spin, they behave like rotating charges. As a consequence of their charge and spin, these nuclei generate a magnetic field (B). This, in turn, gives rise to a magnetic moment (μ), which is randomly oriented in the absence of an external magnetic field. When an external magnetic field (B0) is applied, the magnetic moment vectors can align with the field or against it in 2 + 1 orientations. A hydrogen nucleus, which is just a...
3.1K
Magnetic Moment of an Electron
2.8K
Electrons revolving around a nucleus are analogous to a circular current carrying loop. This current produces a magnetic dipole moment proportional to the electron's orbital angular momentum. Since the orbital angular momentum is quantized in terms of the reduced Planck's constant, the dipole moment is quantized in the Bohr Magneton. The value of the Bohr magneton is 9.27 x 10-24 Am2. Electrons also have an intrinsic spin angular momentum, and the associated spin magnetic moment is...
2.8K
Diamagnetism
2.9K
Materials consisting of paired electrons have zero net magnetic moments. However, when these materials are placed under an external magnetic field, the moments opposite to the field are induced. Such materials are called diamagnets. Diamagnetism is the response of the diamagnets when placed in an external magnetic field.
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
Diamagnetism was discovered by Anton Brugmans in 1778 when he observed that bismuth gets repelled by magnetic fields, thus theorizing that diamagnets get repelled by magnets....
2.9K
Paramagnetism
3.0K
Paramagnets are materials with unpaired electrons that possess a finite magnetic moment. In the absence of a magnetic field, these moments are randomly oriented, and thus the net moment is zero. Under an external field, a torque acting on the moments tends to align them along the field's direction. However, the random thermal motion of electrons produces a torque opposite to the external field and tries to disorient the moments. These two competing effects align only a few moments along the...
3.0K
Subatomic Particles
112.2K
Dalton was only partially correct about the particles that make up matter. All matter is composed of atoms, and atoms are composed of three smaller subatomic particles: protons, neutrons, and electrons. These three particles account for the mass and the charge of an atom.
112.2K
Atomic Nuclei: Nuclear Spin State Population Distribution
2.3K
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.
2.3K
