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相关概念视频

Atomic Nuclei: Nuclear Spin State Population Distribution01:14

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.
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Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

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Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
2.8K
Nuclear Stability03:18

Nuclear Stability

22.8K
Protons and neutrons, collectively called nucleons, are packed together tightly in a nucleus. With a radius of about 10−15 meters, a nucleus is quite small compared to the radius of the entire atom, which is about 10−10 meters. Nuclei are extremely dense compared to bulk matter, averaging 1.8 × 1014 grams per cubic centimeter. If the earth’s density were equal to the average nuclear density, the earth’s radius would be only about 200 meters.
To hold positively charged protons together...
22.8K
Atomic Nuclei: Nuclear Spin State Overview01:03

Atomic Nuclei: Nuclear Spin State Overview

1.9K
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...
1.9K
Atomic Nuclei: Nuclear Relaxation Processes01:23

Atomic Nuclei: Nuclear Relaxation Processes

1.2K
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.
1.2K
Nuclear Binding Energy02:13

Nuclear Binding Energy

14.6K
The difference between the calculated and experimentally measured masses is known as the mass defect of the atom. In the case of helium-4, the mass defect indicates a “loss” in mass of 4.0331 amu – 4.0026 amu = 0.0305 amu. The loss in mass accompanying the formation of an atom from protons, neutrons, and electrons is due to the conversion of that mass into energy that is evolved as the atom forms. The nuclear binding energy is the energy produced when the atoms’ nucleons are bound...
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Updated: Jan 8, 2026

Isotopic Effect in Double Proton Transfer Process of Porphycene Investigated by Enhanced QM/MM Method
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无信号无问题的核量子蒙特卡洛模拟

Zhong-Wang Niu1, Bing-Nan Lu1

  • 1Graduate School of China Academy of Engineering Physics, Beijing 100193, China.

Physical review letters
|December 12, 2025
PubMed
概括
此摘要是机器生成的。

研究人员为原子核开发了一种新的,无符号问题的量子蒙特卡洛 (QMC) 方法. 这一突破使得核结合能量的准确预测成为可能,进步了核结构计算.

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科学领域:

  • 核物理 核物理 核物理
  • 计算物理 计算物理
  • 量子多体系统是一个量子多体系统.

背景情况:

  • 量子蒙特卡洛 (QMC) 方法为量子系统提供了精确的解决方案.
  • 费米子符号问题严重限制了QMC在像原子核这样的系统中的应用.
  • 现有的无符号问题QMC算法仅限于具有有限预测能力的简单模型.

研究的目的:

  • 克服 QMC 在费米离子系统中的局限性.
  • 为原子核开发一个严格的无符号问题的QMC方法.
  • 为核结构计算建立一个可扩展和预测的工具.

主要方法:

  • 开发了一种新的格子核力,它对于偶数核是无符号问题的.
  • 在没有信号问题的QMC框架内实现了旋转轨道合.
  • 使用一个高效的QMC优化框架进行全局参数拟合.

主要成果:

  • 对于76个偶数核 (N,Z≤28) 来说,从实验性结合能量中获得了 σ=2.932 MeV 的标准偏差.
  • 计算了从4He到132Sn的结合能量,并且具有很高的数值精度.
  • 重现了对称的核物质和,并揭示了轻核中的自旋轨道驱动的聚类.

结论:

  • 将无信号无问题的QMC模拟转化为可扩展和预测的核结构工具.
  • 为重核的初始计算建立了一个高准确度,非扰动的基础.
  • 展示了新型相互作用的潜力,以匹配最先进的现象学模型.