从使用真实空间网格的量子蒙特卡洛计算中获得准确的电子密度
Alexander Kaiser1, Stephan Kümmel1
1Theoretical Physics IV, University of Bayreuth, 95447 Bayreuth, Germany.
The Journal of chemical physics
|April 7, 2025
概括
扩散蒙特卡洛 (DMC) 计算为Li2,C和N2提供了准确的基态能量和电子密度. 这种全电子,真实空间网格方法为量子化学计算提供了强大的方法.
科学领域:
- 量子化学 是一个量子化学.
- 计算物理 计算物理
背景情况:
- 精确计算电子能量和密度对于理解分子和原子性质至关重要.
- 量子蒙特卡洛 (QMC) 方法为高精度的电子结构计算提供了强大的框架.
研究的目的:
- 在固定节点近似中使用扩散蒙特卡洛 (DMC) 计算Li2,C和N2的精确基态能量和电子密度.
- 为了证明在DMC中使用的全电子,实空间网格方法计算轨道的优点.
- 调查不同密度函数对计算电子密度的影响.
主要方法:
- 固定节点近似中的扩散蒙特卡罗 (DMC).
- 实时空间网格方法用于计算轨道和电子密度.
- 捆绑技术用于密度计算和规范化用于人工物校正.
- 地方密度近似和精确交换函数的比较.
主要成果:
- DMC地面状态能量可与精心设计的单一参考QMC方法相比较.
- 精确的电子密度是使用实空间网格方法获得的.
- 在QMC密度中证明剩余的统计文物,并通过规范化对其进行校正.
- 在碳原子的电子密度中观察取决于方向的非对称衰变.
结论:
- 全电子,实空间网格DMC方法提供精确的能量和密度.
- 正规化有效地纠正了QMC密度中的统计文物.
- 精确的密度揭示了碳原子衰变的方向差异,与精确的Kohn-Sham潜力联系在一起.
相关概念视频
The Quantum-Mechanical Model of an Atom
41.6K
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...
41.6K
Atomic Radii and Effective Nuclear Charge
50.7K
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.
50.7K
Electron Orbital Model
67.2K
Orbitals are the areas outside of the atomic nucleus where electrons are most likely to reside. They are characterized by different energy levels, shapes, and three-dimensional orientations. The location of electrons is described most generally by a shell or principal energy level, then by a subshell within each shell, and finally, by individual orbitals found within the subshells.
The first shell is closest to the nucleus, and it has only one subshell with a single spherical orbital called the...
The first shell is closest to the nucleus, and it has only one subshell with a single spherical orbital called the...
67.2K
Maxwell-Boltzmann Distribution: Problem Solving
1.3K
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
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
1.3K
Trends in Lattice Energy: Ion Size and Charge
23.5K
An ionic compound is stable because of the electrostatic attraction between its positive and negative ions. The lattice energy of a compound is a measure of the strength of this attraction. The lattice energy (ΔHlattice) of an ionic compound is defined as the energy required to separate one mole of the solid into its component gaseous ions. For the ionic solid sodium chloride, the lattice energy is the enthalpy change of the process:
23.5K
Energy Associated With a Charge Distribution
1.5K
The work done to bring a charge through a distance r is given by the potential difference between the initial and the final position. To assemble a collection of point charges, the total work done can be expressed in terms of the product of each pair of charges divided by their separation distance, defined with respect to a suitable origin. Solving this expression gives the energy stored in a point charge distribution.
1.5K


