Orbital-optimized third-order Møller-Plesset perturbation theory and its spin-component and spin-opposite scaled variants: application to symmetry breaking problems.
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[1] Matthew L. Leininger,et al. PSI3: An open‐source Ab Initio electronic structure package , 2007, J. Comput. Chem..
[2] M. Jacox,et al. Evidence for the stabilization of rectangular O+4 in solid neon , 1994 .
[3] H. Monkhorst,et al. Calculation of properties with the coupled-cluster method , 2009 .
[4] Henry F. Schaefer,et al. Large multiconfiguration self-consistent-field wave functions for the ozone molecule , 1981 .
[5] Rodney J. Bartlett,et al. Similarity transformed equation-of-motion coupled-cluster theory: Details, examples, and comparisons , 1997 .
[6] Poul Jo,et al. Transition moments and dynamic polarizabilities in a second order polarization propagator approach , 1980 .
[7] K. Andersson,et al. Vibrational frequencies of ozone : a multiconfigurational approach , 1992 .
[8] J. Olsen,et al. Orbital-optimized coupled-cluster theory does not reproduce the full configuration-interaction limit. , 2005, The Journal of chemical physics.
[9] M. Jacox,et al. The vibrational spectra of molecular ions isolated in solid neon. II. O+4 and O−4 , 1989 .
[10] R. Lindh,et al. Symmetry breaking in O+4: an application of the Brueckner coupled-cluster method , 1994 .
[11] S. Grimme,et al. Is spin-component scaled second-order Møller-Plesset perturbation theory an appropriate method for the study of noncovalent interactions in molecules? , 2007, The journal of physical chemistry. A.
[12] Thomas Bondo Pedersen,et al. Gauge invariant coupled cluster response theory using optimized nonorthogonal orbitals , 2001 .
[13] Trygve Helgaker,et al. Molecular Electronic-Structure Theory: Helgaker/Molecular Electronic-Structure Theory , 2000 .
[14] A. Barbe,et al. Infrared spectra of 16O3 and 18O3: Darling and Dennison resonance and anharmonic potential function of ozone , 1974 .
[15] M. Head‐Gordon,et al. Approaching closed-shell accuracy for radicals using coupled cluster theory with perturbative triple substitutions , 2003 .
[16] Frank Neese,et al. Assessment of Orbital-Optimized, Spin-Component Scaled Second-Order Many-Body Perturbation Theory for Thermochemistry and Kinetics. , 2009, Journal of chemical theory and computation.
[17] R. Bartlett,et al. A full coupled‐cluster singles and doubles model: The inclusion of disconnected triples , 1982 .
[18] G. Scuseria,et al. The optimization of molecular orbitals for coupled cluster wavefunctions , 1987 .
[19] Trygve Helgaker,et al. Mo/ller–Plesset energy derivatives , 1988 .
[20] T. H. Dunning. Gaussian basis sets for use in correlated molecular calculations. I. The atoms boron through neon and hydrogen , 1989 .
[21] Anna I. Krylov,et al. Second order perturbation corrections to singles and doubles coupled-cluster methods: General theory and application to the valence optimized doubles model , 2000 .
[22] Krishnan Raghavachari,et al. Highly correlated systems: Structure, binding energy and harmonic vibrational frequencies of ozone , 1989 .
[23] Poul Jo,et al. Optimization of orbitals for multiconfigurational reference states , 1978 .
[24] E. Davidson,et al. Symmetry breaking in polyatomic molecules: real and artifactual , 1983 .
[25] H. Schaefer,et al. C3+ is bent , 1990 .
[26] Takehiko Tanaka,et al. Coriolis interaction and anharmonic potential function of ozone from the microwave spectra in the excited vibrational states , 1970 .
[27] William A. Goddard,et al. Configuration interaction studies of O3 and O+3. Ground and excited states , 1975 .
[28] S. Grimme. Improved second-order Møller–Plesset perturbation theory by separate scaling of parallel- and antiparallel-spin pair correlation energies , 2003 .
[29] Poul Jørgensen,et al. The second-order approximate coupled cluster singles and doubles model CC2 , 1995 .
[30] Ivan Hubač,et al. Size-extensivity correction for the state-specific multireference Brillouin–Wigner coupled-cluster theory , 2000 .
[31] P. Pulay. Convergence acceleration of iterative sequences. the case of scf iteration , 1980 .
[32] Josef Paldus,et al. Simultaneous handling of dynamical and nondynamical correlation via reduced multireference coupled cluster method: Geometry and harmonic force field of ozone , 1999 .
[33] Henry F. Schaefer,et al. On the evaluation of analytic energy derivatives for correlated wave functions , 1984 .
[34] John F. Stanton,et al. Many-body perturbation theory with a restricted open-shell Hartree—Fock reference , 1991 .
[35] Stefan Grimme,et al. Improved third‐order Møller–Plesset perturbation theory , 2003, J. Comput. Chem..
[36] Poul Jørgensen,et al. Response functions from Fourier component variational perturbation theory applied to a time-averaged quasienergy , 1998 .
[37] W. D. Allen,et al. Hartree-Fock orbital instability envelopes in highly correlated single-reference wave functions , 1997 .
[38] M. Head‐Gordon,et al. Violations of N-representability from spin-unrestricted orbitals in Møller–Plesset perturbation theory and related double-hybrid density functional theory , 2009 .
[39] W. D. Allen,et al. The analytic evaluation of energy first derivatives for two‐configuration self‐consistent‐field configuration interaction (TCSCF‐CI) wave functions. Application to ozone and ethylene , 1987 .
[40] A. Varandas. Spin-component-scaling second-order Møller-Plesset theory and its variants for economical correlation energies: unified theoretical interpretation and use for quartet N3. , 2010, The Journal of chemical physics.
[41] Henry F. Schaefer,et al. Ordering of the O-O stretching vibrational frequencies in ozone , 1989 .
[42] K. Kowalski. Implementation of the locally renormalized CCSD(T) approaches for arbitrary reference function. , 2005, The Journal of chemical physics.
[43] Trygve Helgaker,et al. Analytical Calculation of Geometrical Derivatives in Molecular Electronic Structure Theory , 1988 .
[44] Frank Neese,et al. Correlated ab initio spin densities for larger molecules: orbital-optimized spin-component-scaled MP2 method. , 2010, The journal of physical chemistry. A.
[45] Henrik Koch,et al. Coupled cluster response functions , 1990 .
[46] Ron Shepard,et al. The Analytic Gradient Method for Configuration Interaction Wave Functions , 1995 .
[47] W. D. Allen,et al. Is the oxywater radical cation more stable than neutral oxywater , 1996 .
[48] Anna I. Krylov,et al. Excited states theory for optimized orbitals and valence optimized orbitals coupled-cluster doubles models , 2000 .
[49] Ove Christiansen,et al. Response functions in the CC3 iterative triple excitation model , 1995 .
[50] Anna I. Krylov,et al. Size-consistent wave functions for nondynamical correlation energy: The valence active space optimized orbital coupled-cluster doubles model , 1998 .
[51] James A Platts,et al. Spin-Component Scaling Methods for Weak and Stacking Interactions. , 2007, Journal of chemical theory and computation.
[52] Martin Head-Gordon,et al. Optimization of wave function and geometry in the finite basis Hartree-Fock method , 1988 .
[53] R. Bartlett,et al. The equilibrium structure and harmonic vibrational frequencies of ozone: coupled cluster results including triple excitations , 1989 .
[54] Garnet Kin-Lic Chan,et al. Tailored coupled cluster singles and doubles method applied to calculations on molecular structure and harmonic vibrational frequencies of ozone. , 2006, The Journal of chemical physics.
[55] Jürgen Gauss,et al. Calculation of excited-state properties using general coupled-cluster and configuration-interaction models. , 2004, The Journal of chemical physics.
[56] Martin Head-Gordon,et al. The perfect quadruples model for electron correlation in a valence active space. , 2009, The Journal of chemical physics.
[57] Martin Head-Gordon,et al. Scaled opposite-spin second order Møller-Plesset correlation energy: an economical electronic structure method. , 2004, The Journal of chemical physics.
[58] David H. Magers,et al. Highly correlated single‐reference studies of the O3 potential surface. I. Effects of high order excitations on the equilibrium structure and harmonic force field of ozone , 1989 .
[59] Francesco A Evangelista,et al. Coupling term derivation and general implementation of state-specific multireference coupled cluster theories. , 2007, The Journal of chemical physics.
[60] Rudolph C. Mayrhofer,et al. Complete active space self‐consistent field potential energy surfaces, dipole moment functions, and spectroscopic properties of O3, CF2, NO−2, and NF+2 , 1991 .
[61] Björn O. Roos,et al. The Multiconfigurational (MC) SCF Method , 1983 .
[62] R. Bartlett,et al. Connected quadruples for the frequencies of O3 , 1999 .
[63] C. Sherrill. Computations of Noncovalent π Interactions , 2009 .
[64] Rodney J. Bartlett,et al. Analytic energy derivatives in many‐body methods. I. First derivatives , 1989 .
[65] R. Bartlett,et al. A direct product decomposition approach for symmetry exploitation in many-body methods. I. Energy calculations , 1991 .
[66] Alistair P. Rendell,et al. The analytic configuration interaction gradient method: The calculation of one electron properties , 1987 .
[67] Martin Head-Gordon,et al. The Theoretical Prediction of Molecular Radical Species: a Systematic Study of Equilibrium Geometries and Harmonic Vibrational Frequencies , 2001 .
[68] Trygve Helgaker,et al. The CC3 model: An iterative coupled cluster approach including connected triples , 1997 .
[69] Thom H. Dunning,et al. Gaussian basis sets for use in correlated molecular calculations. V. Core-valence basis sets for boron through neon , 1995 .
[70] R. Fink. Spin-component-scaled Møller-Plesset (SCS-MP) perturbation theory: a generalization of the MP approach with improved properties. , 2010, The Journal of chemical physics.
[71] H. Schaefer,et al. Molecular geometry and vibrational frequencies of ozone from compact variational wave functions explicitly including triple and quadruple substitutions , 1997 .
[72] J. Linderberg,et al. State vectors and propagators in many‐electron theory. A unified approach , 1977 .
[73] Anna I. Krylov,et al. Energies and analytic gradients for a coupled-cluster doubles model using variational Brueckner orbitals: Application to symmetry breaking in O4+ , 1998 .
[74] Gustavo E. Scuseria,et al. The vibrational frequencies of ozone , 1990 .
[75] Martin Head-Gordon,et al. A tractable and accurate electronic structure method for static correlations: the perfect hextuples model. , 2010, The Journal of chemical physics.
[76] Rohini C. Lochan,et al. Orbital-optimized opposite-spin scaled second-order correlation: an economical method to improve the description of open-shell molecules. , 2007, The Journal of chemical physics.
[77] Trygve Helgaker,et al. Excitation energies from the coupled cluster singles and doubles linear response function (CCSDLR). Applications to Be, CH+, CO, and H2O , 1990 .
[78] S. Grimme,et al. Spin-component scaled second-order Møller–Plesset perturbation theory for the calculation of molecular geometries and harmonic vibrational frequencies , 2004 .
[79] John F. Stanton,et al. A benchmark coupled-cluster single, double, and triple excitation (CCSDT) study of the structure and harmonic vibrational frequencies of the ozone molecule☆ , 1991 .
[80] John F. Stanton,et al. Restricted open-shell Hartree-Fock-based many-body perturbation theory: Theory and application of energy and gradient calculations , 1992 .
[81] D. A. Horner,et al. The lithium superoxide radical: Symmetry breaking phenomena and potential energy surfaces , 1989 .
[82] R. Lindh,et al. The fraternal twins of quartet O+4 , 1994 .
[83] N. Handy,et al. Large basis set calculations using Brueckner theory , 1994 .
[84] Michael T. Heath,et al. Scientific Computing: An Introductory Survey , 1996 .
[85] Hua Guo,et al. Accurate ab initio near-equilibrium potential energy and dipole moment functions of the ground electronic state of ozone , 2000 .
[86] P. Jeffrey Hay,et al. Geometries and energies of the excited states of O3 from ab initio potential energy surfaces , 1977 .
[87] Charles W. Bauschlicher,et al. Theoretical calculation of ozone vibrational infrared intensities , 1985 .
[88] H. Koch,et al. Gauge invariant coupled cluster response theory , 1999 .
[89] A. D. McLean,et al. Contracted Gaussian basis sets for molecular calculations. I. Second row atoms, Z=11–18 , 1980 .
[90] R. Bartlett,et al. On the choice of orbitals for symmetry breaking problems with application to NO3 , 1992 .
[91] Hans-Joachim Werner,et al. Calculation of intermolecular interactions in the benzene dimer using coupled-cluster and local electron correlation methods. , 2006, Physical chemistry chemical physics : PCCP.
[92] R. Bartlett,et al. COUPLED-CLUSTER CALCULATIONS OF STRUCTURE AND VIBRATIONAL FREQUENCIES OF OZONE : ARE TRIPLE EXCITATIONS ENOUGH? , 1998 .
[93] J. Pople,et al. Self‐consistent molecular orbital methods. XX. A basis set for correlated wave functions , 1980 .
[94] Uğur Bozkaya,et al. Quadratically convergent algorithm for orbital optimization in the orbital-optimized coupled-cluster doubles method and in orbital-optimized second-order Møller-Plesset perturbation theory. , 2011, The Journal of chemical physics.
[95] P. C. Hariharan,et al. The influence of polarization functions on molecular orbital hydrogenation energies , 1973 .