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Multireference states

With suitable methods, such interactions can be treated properly, and reasonable potential energy surfaces obtained, but this requires the ability to describe inherently multireference states. Most such methods are not many-body in nature, and of course we prefer a size-extensive approach if possible. [Pg.286]

CASPT2 Second order perturbation theory on top of a CASSCF wave function yp n5 Cheapest for multireference states... [Pg.238]

Multireference State-Specific Coupled Cluster Theory with a Complete Active Space Reference... [Pg.69]

Multireference State-Specific Coupled Cluster Theory... [Pg.71]

Multireference State-Specific Generalization of CCSD Theory... [Pg.71]

The current volume presents the compilation of splendid contributions distributed over 21 chapters. The very first chapter contributed by Istvan Hargittai presents the historical account of development of structural chemistry. It also depicts some historical memories of scientists presented in the form of their pictures. This historical description covers a vast period of time. Intruder states pose serious problem in the multireference formulation based on Rayleigh-Schrodinger expansion. Ivan Hubac and Stephen Wilson discuss the ciurent development and future prospects of Many-Body Brillouin-Wigner theories to avoid the problem of intruder states in the next chapter. The third chapter written by Vladimir Ivanov and collaborators reveals the development of multireference state-specific coupled cluster theory. The next chapter from Maria Barysz discusses the development and application of relativistic effects in chemical problems while the fifth chapter contributed by Manthos Papadopoulos and coworkers describes electronic, vibrational and relativistic contributions to the linear and nonlinear optical properties of molecules. [Pg.686]

BWPT = Brillouin-Wigner perturbation theory EN = Epstein-Nesbet FCI = full Cl MBPT = many-body perturbation theory MRS PT = multireference state perturbation theory PT = perturbation theory RSPT = Rayleigh-SchrSdinger perturbation theory SRS PT = single-reference state perturbation theory. [Pg.1706]

MP methods have been developed for both spin-restricted HF (RHF), spin-unrestricted HF (UHF), and restricted open-shell HF (ROHF) wavefunctions to investigate both closed- and open-shell systems (see Table 2). For the calculation of electron systems with multireference character such as biradicals various multireference state (MRS) MP methods have been developed (Table 2). All these methods describe atoms, molecules, and reaction systems in the gas phase. However, many chemical reactions take place in solution phases. For this purpose, MP methods are available that start from a solvent corrected wavefunction where mostly polarizable continuum models are used (see Self-consistent Reaction Field Methods). [Pg.1723]


See other pages where Multireference states is mentioned: [Pg.329]    [Pg.69]    [Pg.1717]    [Pg.2651]   
See also in sourсe #XX -- [ Pg.161 ]




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