相关实验视频
Updated: Feb 24, 2026

10:42
Preparing an Isotopically Pure 229Th Ion Beam for Studies of 229mTh
Published on: May 3, 2019
7.4K
^{93m}Mo的同位素耗尽是由不弹性核散射引发的,而不是由电子捕获引发的核激发
B Ding1,2, C X Jia1,2, S Guo1,2
1Institute of Modern Physics, State Key Laboratory of Heavy Ion Science and Technology, Chinese Academy of Sciences, Lanzhou 730000, China.
Physical review letters
|February 22, 2026
概括
研究了-93m中的同位素耗尽. 该研究发现,无弹性核散射,而不是电子捕获的核激发,导致了这种耗尽,精确的概率是用和碳薄膜测量的.
科学领域:
- 核物理 核物理 核物理
- 原子物理 原子物理
- 材料科学 材料科学 材料科学
背景情况:
- 异构体耗尽对于各种应用至关重要.
- 之前的研究将-93m的耗尽归因于通过电子捕获 (NEEC) 的核激发,但结果是矛盾的.
研究的目的:
- 精确测量-93m的同位素耗尽概率.
- 确定负责-93m中异构体耗尽的潜在机制.
主要方法:
- 使用一种低背景,基于光束的实验方法.
- 使用了纯化的-93m同位素束.
- 在和碳薄膜的减速过程中进行了测量.
主要成果:
- 在中,耗尽概率被确定为2.0(2) ×10−5,在碳中为4.7(13) ×10−6.
- 实验结果与不弹性核散射计算非常一致.
- 排除了NEEC机制作为主要原因.
结论:
- 在-93m中观察到的同位素耗尽归因于不弹性核散射.
- 这一发现解决了以前关于枯竭机制的矛盾.
相关概念视频
Atomic Nuclei: Nuclear Relaxation Processes
1.3K
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.
1.3K
Nuclear Overhauser Enhancement (NOE)
1.5K
Irradiation of a spin-active nucleus causes an increase or decrease in the signal intensity of neighboring nuclei that are not necessarily chemically bonded or involved in J-coupling. This phenomenon, called the nuclear Overhauser enhancement (NOE), results from through-space interactions between the nuclear spins. The NOE effect decreases with increasing internuclear distance and is generally not observed beyond 4 angstroms. In NOE, dipole-dipole interactions between neighboring spin-active...
1.5K
¹³C NMR: ¹H–¹³C Decoupling
1.9K
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...
1.9K
Atomic Nuclei: Magnetic Resonance
1.3K
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...
1.3K
Types of Radioactivity
20.0K
The most common types of radioactivity are α decay, β decay, γ decay, neutron emission, and electron capture.
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
Alpha (α) decay is the emission of an α particle from the nucleus. For example, polonium-210 undergoes α decay:
20.0K
Atomic Nuclei: Nuclear Spin State Overview
2.1K
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...
2.1K

