scholarly journals Erratum: “A class IV charge model for molecular excited states” [J. Chem. Phys. 110, 724 (1999)]

1999 ◽  
Vol 111 (12) ◽  
pp. 5624-5624
Author(s):  
Jiabo Li ◽  
Brian Williams ◽  
Christopher J. Cramer ◽  
Donald G. Truhlar
1999 ◽  
Vol 110 (2) ◽  
pp. 724-733 ◽  
Author(s):  
Jiabo Li ◽  
Brian Williams ◽  
Christopher J. Cramer ◽  
Donald G. Truhlar

2020 ◽  
Vol 102 (6) ◽  
Author(s):  
Jules Tilly ◽  
Glenn Jones ◽  
Hongxiang Chen ◽  
Leonard Wossnig ◽  
Edward Grant

2019 ◽  
Author(s):  
Jacob Nite ◽  
Carlos A. Jimenez-Hoyos

Quantum chemistry methods that describe excited states on the same footing as the ground state are generally scarce. In previous work, Gill et al. (J. Phys. Chem. A 112, 13164 (2008)) and later Sundstrom and Head-Gordon (J. Chem. Phys. 140, 114103 (2014)) considered excited states resulting from a non-orthogonal configuration interaction (NOCI) on stationary solutions of the Hartree–Fock equations. We build upon those contributions and present the state-averaged resonating Hartree–Fock (sa-ResHF) method, which differs from NOCI in that spin-projection and orbital relaxation effects are incorporated from the onset. Our results in a set of small molecules (alanine, formaldehyde, acetaldehyde, acetone, formamide, and ethylene) suggest that sa-ResHF excitation energies are a notable improvement over configuration interaction singles (CIS), at a mean-field computational cost. The orbital relaxation in sa-ResHF, in the presence of a spin-projection operator, generally results in excitation energies that are closer to the experimental values than the corresponding NOCI ones.


2019 ◽  
Author(s):  
Jacob Nite ◽  
Carlos A. Jimenez-Hoyos

Quantum chemistry methods that describe excited states on the same footing as the ground state are generally scarce. In previous work, Gill et al. (J. Phys. Chem. A 112, 13164 (2008)) and later Sundstrom and Head-Gordon (J. Chem. Phys. 140, 114103 (2014)) considered excited states resulting from a non-orthogonal configuration interaction (NOCI) on stationary solutions of the Hartree–Fock equations. We build upon those contributions and present the state-averaged resonating Hartree–Fock (sa-ResHF) method, which differs from NOCI in that spin-projection and orbital relaxation effects are incorporated from the onset. Our results in a set of small molecules (alanine, formaldehyde, acetaldehyde, acetone, formamide, and ethylene) suggest that sa-ResHF excitation energies are a notable improvement over configuration interaction singles (CIS), at a mean-field computational cost. The orbital relaxation in sa-ResHF, in the presence of a spin-projection operator, generally results in excitation energies that are closer to the experimental values than the corresponding NOCI ones.


2016 ◽  
Vol 16 (4) ◽  
pp. 467-473 ◽  
Author(s):  
K. Wang ◽  
P. Murahari ◽  
K. Yokoyama ◽  
J. S. Lord ◽  
F. L. Pratt ◽  
...  

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