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57Fe Mössbauer parameters from domain based local pair-natural orbital coupled-cluster theory

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Datta,  Dipayan
Department of Chemistry and Ames Laboratory, Iowa State University;
Research Department Neese, Max-Planck-Institut für Kohlenforschung, Max Planck Society;

Saitow,  Masaaki
Research Department Neese, Max-Planck-Institut für Kohlenforschung, Max Planck Society;
Department of Chemistry, Graduate School of Science, Nagoya University;

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Neese,  Frank
Research Department Neese, Max-Planck-Institut für Kohlenforschung, Max Planck Society;
FACCTs GmbH;

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Citation

Datta, D., Saitow, M., Sandhöfer, B., & Neese, F. (2020). 57Fe Mössbauer parameters from domain based local pair-natural orbital coupled-cluster theory. The Journal of Chemical Physics, 153(20): 204101. doi:10.1063/5.0022215.


Cite as: http://hdl.handle.net/21.11116/0000-0007-AB0A-E
Abstract
We report on applications of the domain based local pair-natural orbital (PNO) coupled-cluster method within the singles and doubles approximation (DLPNO-CCSD) to the calculation of 57Fe isomer shifts and quadrupole splittings in a small training set of iron complexes consisting of large molecular ligands and iron atoms in varying charge, spin, and oxidation states. The electron densities and electric field gradients needed for these calculations were obtained within the recently implemented analytic derivative scheme. A method for the direct treatment of scalar relativistic effects in the calculation of effective electron densities is described by using the first-order Douglas–Kroll–Hess Hamiltonian and a Gaussian charge distribution model for the nucleus. The performance of DLPNO-CCSD is compared with four modern-day density functionals, namely, RPBE, TPSS, B3LYP, and B2PLYP, as well as with the second-order Møller–Plesset perturbation theory. An excellent correlation between the calculated electron densities and the experimental isomer shifts is attained with the DLPNO-CCSD method. The correlation constant a obtained from the slope of the linear correlation plot is found to be ≈−0.31 a.u.3 mm s−1, which agrees very well with the experimental calibration constant α = −0.31 ± 0.04 a.u.3 mm s−1. This value of a is obtained consistently using both nonrelativistic and scalar relativistic DLPNO-CCSD electron densities. While the B3LYP and B2PLYP functionals achieve equally good correlation between theory and experiment, the correlation constant a is found to deviate from the experimental value. Similar trends are observed also for quadrupole splittings. The value of the nuclear quadrupole moment for 57Fe is estimated to be 0.15 b at the DLPNO-CCSD level. This is consistent with previous results and is here supported by a higher level of theory. The DLPNO-CCSD results are found to be insensitive to the intrinsic approximations in the method, in particular the PNO occupation number truncation error, while the results obtained with density functional theory (DFT) are found to depend on the choice of the functional. In a statistical sense, i.e., on the basis of the linear regression analysis, however, the accuracies of the DFT and DLPNO-CCSD results can be considered comparable.