Javascript must be enabled to continue!
Indirect nuclear spin–spin couplings with third-order contributions added to the SOPPA method
View through CrossRef
In this article, a modification of the second-order polarization propagator approximation (SOPPA) method is introduced and illustrated for the calculation of the indirect nuclear spin–spin couplings. The standard SOPPA method, although cheaper in terms of computational cost, offers less accurate results than the ones obtained with coupled cluster methods. A new method, named SOPPA+A3-3, was therefore developed by adding the terms of the third-order A matrix that rely on the second-order double amplitudes. The performance of this third-order contribution was studied using the coupled cluster singles and doubles method as a reference, calculating the spin–spin couplings of molecules of diverse sizes and compositions, and comparing them to the SOPPA method. The results show that inclusion of this third-order contribution gives more accurate results than the standard SOPPA method with a level of accuracy close to that of the coupled cluster method with only a small increase in the computational cost of the response calculation that dominates the computational cost for small- to medium-sized molecules. The implementation of the first contributions to the third-order polarization propagator approximation in the Dalton program, thus, already shows a significant change in these molecular properties over those obtained with the standard SOPPA method.
Title: Indirect nuclear spin–spin couplings with third-order contributions added to the SOPPA method
Description:
In this article, a modification of the second-order polarization propagator approximation (SOPPA) method is introduced and illustrated for the calculation of the indirect nuclear spin–spin couplings.
The standard SOPPA method, although cheaper in terms of computational cost, offers less accurate results than the ones obtained with coupled cluster methods.
A new method, named SOPPA+A3-3, was therefore developed by adding the terms of the third-order A matrix that rely on the second-order double amplitudes.
The performance of this third-order contribution was studied using the coupled cluster singles and doubles method as a reference, calculating the spin–spin couplings of molecules of diverse sizes and compositions, and comparing them to the SOPPA method.
The results show that inclusion of this third-order contribution gives more accurate results than the standard SOPPA method with a level of accuracy close to that of the coupled cluster method with only a small increase in the computational cost of the response calculation that dominates the computational cost for small- to medium-sized molecules.
The implementation of the first contributions to the third-order polarization propagator approximation in the Dalton program, thus, already shows a significant change in these molecular properties over those obtained with the standard SOPPA method.
Related Results
Benchmarking NMR indirect nuclear spin-spin coupling constants: SOPPA, SOPPA(CC2), and SOPPA(CCSD) versus CCSD
Benchmarking NMR indirect nuclear spin-spin coupling constants: SOPPA, SOPPA(CC2), and SOPPA(CCSD) versus CCSD
Accurate calculations of NMR indirect nuclear spin-spin coupling constants require especially optimized basis sets and correlated wave function methods such as CCSD or SOPPA(CCSD)....
Benchmarking anisotropic polarizabilities for 14 (hetero)-aromatic molecules at RPA, RPA(D), HRPA, HRPA(D), SOPPA, SOPPA(CC2), SOPPA(CCSD), CC2, CCSD and CC3 levels
Benchmarking anisotropic polarizabilities for 14 (hetero)-aromatic molecules at RPA, RPA(D), HRPA, HRPA(D), SOPPA, SOPPA(CC2), SOPPA(CCSD), CC2, CCSD and CC3 levels
A benchmark of anisotropic polarizabilities has been carried out for
14 (hetero)-aromatic molecules using the methods: RPA, RPA(D), HRPA,
HRPA(D), SOPPA, SOPPA(CC2), SOPPA(CCSD), C...
Benchmarking anisotropic polarizabilities for 14 (hetero)‐aromatic molecules at RPA, RPA(D), HRPA, HRPA(D), SOPPA, SOPPA(CC2), SOPPA(CCSD), CC2, CCSD and CC3 levels
Benchmarking anisotropic polarizabilities for 14 (hetero)‐aromatic molecules at RPA, RPA(D), HRPA, HRPA(D), SOPPA, SOPPA(CC2), SOPPA(CCSD), CC2, CCSD and CC3 levels
AbstractA benchmark of anisotropic polarizabilities has been carried out for 14 (hetero)‐aromatic molecules using the methods: RPA, RPA(D), HRPA, HRPA(D), SOPPA, SOPPA(CC2), SOPPA(...
Tailoring spin dynamics in asymmetric FM1/Pt/FM2 trilayers via Pt spacer thickness
Tailoring spin dynamics in asymmetric FM1/Pt/FM2 trilayers via Pt spacer thickness
The study of trilayers with a non-magnetic (NM) spacer layer separating two ferromagnetic layers (FM/NM/FM) has been an active area of spintronics research due to their real-world ...
Dynamics of spinor fermions
Dynamics of spinor fermions
Ultracold atomic gases have established themselves as quantum systems, which are clean and offer a high degree of control over crucial parameters. They are well isolated from their...
Spin to charge current interconversion in Rasha interfaces and topological insulators
Spin to charge current interconversion in Rasha interfaces and topological insulators
Conversion entre courant de spin et courant de charge dans des interfaces Rashba et des isolants topologiques
L'interconversion entre courants de spin et de charge ...
Nuclear Weapons, Cyber Warfare, and Cyber Security: Ethical and Anticipated Ethical Issues
Nuclear Weapons, Cyber Warfare, and Cyber Security: Ethical and Anticipated Ethical Issues
In this paper, we discuss the interrelationship of nuclear weapons, cyber warfare, and cyber security. Some of the most significant cyber threats to nuclear stability are now ...
Exploring the effects of Zeeman field on spin-triplet superconductivity
Exploring the effects of Zeeman field on spin-triplet superconductivity
Exploration des effets d'un champ Zeeman sur les supraconducteurs spin-triplet
Les supraconducteurs non conventionnels sont classés en fonction des propriétés de sy...

