密度函数方法的系统比较,用于确定旋转状态能量差距和旋转交叉复合体的旋转过渡温度
1Department of Chemical Sciences, Indian Institute of Science Education Research (IISER) Mohali Sector-81, Knowledge City, S.A.S. Nagar Mohali 140306 Punjab India vigneshkuduvar@iisermohali.ac.in.
RSC advances
|January 12, 2026
概括
密度函数理论 (DFT) 的计算评估了九个函数用于旋转交叉 (SCO) 复杂行为. 功能性TPSSh和B3LYP*准确地预测了SCO综合体的地面状态和能量差距.
科学领域:
- 计算化学的计算化学
- 材料科学 材料科学 材料科学
- 量子化学 是一个量子化学.
背景情况:
- 旋转交叉 (SCO) 复合体表现出明显的高旋转和低旋转状态,对于分子开关和传感器至关重要.
- 准确的理论预测SCO行为需要仔细选择计算方法,考虑到分散和等因素.
研究的目的:
- 综合分析九个密度函数理论 (DFT) 函数在26个SCO复合体的旋转状态能量差距和过渡温度预测中的性能.
- 确定最可靠的DFT函数,用于精确的旋转交叉现象理论建模.
主要方法:
- 通过密度函数理论 (DFT) 研究了26种过渡金属SCO复合体.
- 使用了九种不同的密度函数:TPSS,BLYP,TPSSh,B3LYP,B3LYP*,OPBE,O3LYP,B3P86和X3LYP.
- 计算了自旋状态能量差距,并考虑了分散和振动等物理性质.
主要成果:
- 混合元GGA TPSSh和B3LYP*功能器准确预测了所有SCO复合体的基本状态和合理的高旋转/低旋转 (HS-LS) 能量差距.
- 纯元-GGA TPSS和GGA BLYP函数正确预测了基本状态,但高估了HS-LS差距.
- 对于大多数SCO复合体,包括具有不寻常几何形状的复合体,TPSSh与实验旋转过渡温度 (T1/2) 有很好的一致性.
结论:
- 强烈建议使用TPSSh功能来准确计算自旋交叉行为的DFT,提供可靠的能量差距和过渡温度预测.
- B3LYP*还显示出作为SCO复杂研究的可靠函数的前景.
- 仔细选择DFT函数对于理解和预测SCO属性至关重要.
更多相关视频
相关概念视频
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.
2.3K
Valence Bond Theory
11.2K
Coordination compounds and complexes exhibit different colors, geometries, and magnetic behavior, depending on the metal atom/ion and ligands from which they are composed. In an attempt to explain the bonding and structure of coordination complexes, Linus Pauling proposed the valence bond theory, or VBT, using the concepts of hybridization and the overlapping of the atomic orbitals. According to VBT, the central metal atom or ion (Lewis acid) hybridizes to provide empty orbitals of suitable...
11.2K
Spin–Spin Coupling Constant: Overview
1.4K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.4K
¹H NMR: Interpreting Distorted and Overlapping Signals
1.5K
Spin systems where the difference in chemical shifts of the coupled nuclei is greater than ten times J are called first-order spin systems. These nuclei are weakly coupled, and their chemical shifts and coupling constant can generally be estimated from the well-separated signals in the spectrum.
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
As Δν decreases and the signals move closer, the doublets appear increasingly distorted. The intensities of the inner lines increase at the cost of those of the outer lines as the signals are...
1.5K
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
Spin–Spin Coupling: One-Bond Coupling
1.4K
Coupling interactions are strongest between NMR-active nuclei bonded to each other, where spin information can be transmitted directly through the pair of bonding electrons. While nuclei polarize their electrons to the opposite spins, the bonding electron pair has opposite spins. Configurations with antiparallel nuclear spins are expected to be lower in energy. When coupling makes antiparallel states more favorable, J is considered to have a positive value. The one-bond coupling constant, 1J,...
1.4K


