相关实验视频
Updated: Jun 29, 2025

10:37
Spatial Separation of Molecular Conformers and Clusters
Published on: January 9, 2014
9.0K
核量子效应在水性星团中的多体视角
Eleftherios Lambros1, Jonathan H Fetherolf2, Sharon Hammes-Schiffer2
1Department of Chemistry, University of Washington, Seattle, Washington 98195, United States.
The journal of physical chemistry letters
|April 8, 2024
概括
核量子效应显著影响水群相互作用. 质子定量化稳定了高阶分子相互作用,揭示了它在水系热力学中的关键作用.
科学领域:
- 物理化学 物理化学
- 计算化学的计算化学
- 量子力学就是量子力学.
背景情况:
- 核量子效应对于理解水系统至关重要.
- 精确的水集群建模需要考虑这些量子效应.
- 传统的方法往往很难有效地结合这些效应.
研究的目的:
- 调查水中质子量子化的能量贡献.
- 用核电子轨道 (NEO) 理论分析多体相互作用.
- 为了证明核量子效应在水热力学中的重要性.
主要方法:
- 进行多体膨胀分析.
- 使用核电子轨道 (NEO) 理论进行计算.
- 在水集群上进行单点能量计算.
主要成果:
- 质子量子化产生了对多体相互作用的显著能量贡献.
- 零点运动在单体水平上增加能量.
- 核量子效应稳定了水中的更高阶分子相互作用.
结论:
- 核量子效应在水系统的多体相互作用中起着非常重要的作用.
- NEO方法有效地将核量子效应纳入能源计算中.
- 这项研究提供了一种将核量子效应整合到水潜在能量表面的方法.
相关概念视频
The Quantum-Mechanical Model of an Atom
42.3K
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.
42.3K
Atomic Nuclei: Nuclear Spin State Population Distribution
974
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.
974
Atomic Nuclei: Nuclear Spin State Overview
938
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...
938
Atomic Nuclei: Nuclear Relaxation Processes
649
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.
649
Nuclear Binding Energy
12.4K
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...
12.4K
Atomic Radii and Effective Nuclear Charge
51.6K
The elements in groups of the periodic table exhibit similar chemical behavior. This similarity occurs because the members of a group have the same number and distribution of electrons in their valence shells.
51.6K

