基于密度矩阵嵌入的多参考扰动理论方法对单离子磁铁
1Beijing National Laboratory for Molecular Sciences, College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China.
The Journal of chemical physics
|June 11, 2025
概括
密度矩阵嵌入理论 (DMET) 与NEVPT2 (DMET + NEVPT2) 结合,准确计算了单离子磁铁中的磁性异性质. 这种方法显著降低了计算成本,使磁性质的先进研究成为可能.
科学领域:
- 计算化学计算化学
- 量子力学就是量子力学.
- 材料科学 材料科学 材料科学
背景情况:
- 多配置波函数理论 (MC-WFT),特别是CASSCF-SO,对于理解单离子磁铁 (SIM) 是至关重要的.
- 高的计算成本限制了CASSCF-SO对复杂SIM结构的应用.
- 密度矩阵嵌入理论 (DMET) 提供了一个严格的框架来结合低级和高级量子化学方法.
研究的目的:
- 通过使用二阶n电子价值扰动理论 (NEVPT2) 结合动态相关性来扩展DMET框架,创建DMET + NEVPT2.
- 为了对DMET + NEVPT2的准确性进行基准测试,用于计算过渡金属复合体中的分子磁性异性质.
- 评估新的DMET + NEVPT2方法的计算效率和可扩展性.
主要方法:
- 密度矩阵嵌入理论 (DMET) 框架的开发和应用.
- 在CASSCF之上,通过二阶n电子价值扰动理论 (NEVPT2) 包含动态相关性.
- 在过渡金属复合体中对分子磁性异性质的全电子计算进行基准测试.
主要成果:
- DMET + NEVPT2的效果与计算上昂贵的全电子处理非常相似.
- 通过增加中央集群的大小,可以系统地提高DMET + NEVPT2的准确性.
- 由于DMET的轨道缩小,因此实现了计算成本的显著降低.
结论:
- DMET + NEVPT2有效地捕捉了SIM中磁性异构性所必需的动态相关性.
- 这种方法为高精度的ab initio自旋声波放松研究提供了计算效率高的途径.
- 开发的方法促进了SIM的高通量计算.
更多相关视频
07:42Optimizing Magnetic Force Microscopy Resolution and Sensitivity to Visualize Nanoscale Magnetic Domains
Published on: July 20, 2022
2.7K
06:53Author Spotlight: Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
Published on: June 9, 2023
1.9K
相关概念视频
Diamagnetism
2.4K
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....
2.4K
Paramagnetism
2.5K
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...
2.5K
Potential Due to a Magnetized Object
263
Magnetic dipoles in magnetic materials are aligned when placed under an external magnetic field. For paramagnets and ferromagnets, dipole alignment occurs in the direction of the magnetic field. However, the dipoles align opposite to the field in the case of diamagnets. This state of magnetic polarization due to the external field is called magnetization. Magnetization is defined as the dipole moment per unit volume. It plays a similar role to polarization in electrostatics.
The vector...
The vector...
263
Magnetic Susceptibility and Permeability
996
In linear magnetic materials, like paramagnets and diamagnets, magnetization is proportional to the magnetic field intensity. The constant of proportionality, a dimensionless number, is called magnetic susceptibility. The value of the susceptibility depends on the type of material.
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
When diamagnetic materials are placed under an external magnetic field, the moments opposite to the field are induced. Hence, the susceptibility for diamagnets has a minimal negative value of 10-5–10-6. Since...
996
Ferromagnetism
2.4K
Materials like iron, nickel, and cobalt consist of magnetic domains, within which the magnetic dipoles are arranged parallel to each other. The magnetic dipoles are rigidly aligned in the same direction within a domain by quantum mechanical coupling among the atoms. This coupling is so strong that even thermal agitation at room temperature cannot break it. The result is that each domain has a net dipole moment. However, some materials have weaker coupling, and are ferromagnetic at lower...
2.4K
Magnetic Vector Potential
562
In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
562
