Time-dependent vibrational coupled cluster theory: Theory and implementation at the two-mode coupling level.
Mads Bøttger Hansen1, Niels Kristian Madsen1, Alberto Zoccante1
1Department of Chemistry, Aarhus University, Langelandsgade 140, DK-8000 Aarhus C, Denmark.
The Journal of Chemical Physics
|October 24, 2019
Summary
Time-dependent vibrational coupled cluster (TDVCC) theory accurately describes molecular vibrations. Numerical experiments confirm TDVCC
Area of Science:
- Quantum chemistry
- Computational chemistry
- Molecular dynamics
Background:
- Accurate simulation of molecular vibrations is crucial for understanding chemical reactions and material properties.
- Time-dependent methods are essential for describing dynamic processes in molecules.
Purpose of the Study:
- To derive and implement equations for time-dependent vibrational coupled cluster (TDVCC) wave functions, including both ket and bra states.
- To analyze the behavior of TDVCC under time-dependent Hamiltonians and assess its accuracy and efficiency.
Main Methods:
- Derivation of time evolution equations for TDVCC ket and Λ bra states.
- Implementation for Hamiltonians and cluster operators with at most two-mode coupling.
- Theoretical and numerical analysis of norm, energy, and expectation value evolution.
- Study of state separability for noninteracting systems.
- Numerical experiments on polycyclic aromatic hydrocarbons.
Main Results:
- The TDVCC theory and its implementation capture the complex dynamics of molecular vibrations.
- Analysis revealed non-trivial behavior in norm, energy, and expectation values due to nonunitary time evolution.
- The coupled cluster state exhibits correct separability, while the Λ state shows more intricate behavior.
- TDVCC in incomplete expansions outperforms standard linear variational methods in accuracy.
- Equivalent results are achieved with complete expansions.
Conclusions:
- TDVCC provides a robust framework for studying time-dependent vibrational dynamics.
- The method demonstrates superior accuracy compared to variational approaches for a given number of parameters.
- TDVCC is efficient for large molecular systems, as shown by applications to polycyclic aromatic hydrocarbons.
Related Concept Videos
Spin–Spin Coupling: Two-Bond Coupling (Geminal Coupling)
1.5K
Two NMR-active nuclei bonded to a central atom can be involved in geminal or two-bond coupling. Geminal coupling is commonly seen between diastereotopic protons in chiral molecules and unsymmetrical alkenes, among others.
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
The central atom need not be NMR-active because its electrons are affected by the electron polarization of the spin-active atoms. However, spin information is transmitted less effectively than in one-bond coupling, and 2J values are usually weaker than 1J values. The energy of...
1.5K
Hybridization of Atomic Orbitals II
47.4K
sp3d and sp3d 2 Hybridization
47.4K
Spin–Spin Coupling: Three-Bond Coupling (Vicinal Coupling)
1.4K
Vicinal or three-bond coupling is commonly observed between protons attached to adjacent carbons. Here, nuclear spin information is primarily transferred via electron spin interactions between adjacent C‑H bond orbitals. This generally favors the antiparallel arrangement of spins, so 3J values are usually positive.
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...
The extent of coupling depends on the C‑C bond length, the two H‑C‑C angles, any electron-withdrawing substituents, and the dihedral angle between the involved orbitals. The...
1.4K
Hybridization of Atomic Orbitals I
65.0K
The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
65.0K
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
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


