TY - JOUR
T1 - The Importance of Tight f Basis Functions for Heavy p-Block Oxides and Halides: A Parallel With Tight d functions in the Second Row
AU - Mehta, Nisha
AU - Martin, Jan M L
N1 - Publisher Copyright: © 2023 The Authors. Published by American Chemical Society.
PY - 2023/3/9
Y1 - 2023/3/9
N2 - It is well-known that both wave function ab initio and DFT calculations on second-row compounds exhibit anomalously slow basis set convergence unless the basis sets are augmented with additional "tight" (high-exponent) d functions, as in the cc-pV(n+d)Z and aug-cc-pV(n+d)Z basis sets. This has been rationalized as being necessary for a better description of the low-lying 3d orbital, which as the oxidation state increases sinks low enough to act as a back-donation acceptor from chalcogen and halogen lone pairs. This prompts the question whether a similar phenomenon exists for the isovalent compounds of the heavy p-block. We show that for the fourth and fifth row, this is the case, but this time for tight f functions enhancing the description of the low-lying 4f and 5f Rydberg orbitals, respectively. In the third-row heavy p block, the 4f orbitals are too far up, while the 4d orbitals are adequately covered by the basis functions already present to describe the 3d subvalence orbitals.
AB - It is well-known that both wave function ab initio and DFT calculations on second-row compounds exhibit anomalously slow basis set convergence unless the basis sets are augmented with additional "tight" (high-exponent) d functions, as in the cc-pV(n+d)Z and aug-cc-pV(n+d)Z basis sets. This has been rationalized as being necessary for a better description of the low-lying 3d orbital, which as the oxidation state increases sinks low enough to act as a back-donation acceptor from chalcogen and halogen lone pairs. This prompts the question whether a similar phenomenon exists for the isovalent compounds of the heavy p-block. We show that for the fourth and fifth row, this is the case, but this time for tight f functions enhancing the description of the low-lying 4f and 5f Rydberg orbitals, respectively. In the third-row heavy p block, the 4f orbitals are too far up, while the 4d orbitals are adequately covered by the basis functions already present to describe the 3d subvalence orbitals.
UR - http://www.scopus.com/inward/record.url?scp=85149143016&partnerID=8YFLogxK
U2 - https://doi.org/10.1021/acs.jpca.3c00544
DO - https://doi.org/10.1021/acs.jpca.3c00544
M3 - مقالة
C2 - 36854651
SN - 1089-5639
VL - 127
SP - 2104
EP - 2112
JO - The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory
JF - The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory
IS - 9
ER -