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Geometrical Derivatives and EPR G-tensor Based on Equation of Motion Coupled- Cluster Theory with Spin-Orbit Coupling

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报告题目   Geometrical Derivatives and EPR G-tensor Based on Equation of Motion Coupled- Cluster Theory with Spin-Orbit Coupling
报告人   王繁 教授
报告人单位   四川大学、原子与分子物理研究所
报告时间   2014-05-27
报告地点   理化大楼附属小楼(原计算中心楼)三楼会议室(301室)
主办单位   合肥微尺度物质科学国家实验室
报告介绍

报告摘要:
  Recently we developed a coupled-cluster approach (CC) for closed-shell systems with SOC included in post-Hartee-Fock treatment. Total energy, analytical first and second order derivates of this SOC-CC approach at the CCSD and CCSD(T) levels have been developed. Both time-reversal symmetry and spatial symmetry for D2h and its subgroups are exploited[1] in the implementation. In addition, the equation of motion method based on this SOC-CC approach for excitation energies, ionized states[2] as well as electron attachment[3] is also developed.
  Analytical energy gradient of this EOM-CCSD approach for excited, ionized or electron attached states with SOC has been implemented, which facilitates geometry optimization, harmonic frequencies calculations. In the implementation, a Lagrangian is introduced to avoid calculating first order derivatives of the eigenvectors and cluster operator. In addition, EPR g-tensor for open-shell molecules with one unpaired electron has also been calculated as a first order derivative of total energy based on EOMIP-CCSD and EOMEA-CCSD with SOC with respect to external magnetic field. To achieve high efficiency, a proper combination of different spin cases is introduced in the Lagrangian to restore time-reversal symmetry. We present equilibrium structures and harmonic frequencies of CH2ClI+, AuH2 based on EOMIP-CCSD as well as those of UO2+ with EOMEA-CCSD. Furthermore, EPR g-tensors of some diatomic molecules are also presented.

[1] Z. Tu, D. Yang, F. Wang and J. Guo, J. Chem. Phys.135, 034115, 2011.
[2] Z. Tu, F. Wang and X. Li, J. Chem. Phys. 136, 174102, 2012.
[3] D. Yang, F. Wang and J. Guo, Chem. Phys. Lett., 531, 236, 2012.

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