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The Adiabatic Connection Formula

Similarly, taking as an approximate wave function for H yields [Pg.409]

Addition of these two inequalities gives Eq + Eo Eq + Eo, showing that the assumption was wrong. In other words, for the ground state there is a one-to-one correspondence between the electron density and the nuclear potential, and thereby also with the Hamilton operator and tlie energy. In the language of Density Functional Theory, the energy is a unique functional of the electron density, [p]. [Pg.409]

Litegrating over A between tlie limits 0 and 1 corresponds to smoothly transforming the non-interacting reference to the real system. This integration is done under the assumption that the density remains constant. [Pg.409]

Note that it is the same density that appears in the two integrals over Vext(O) and Vext(l), [Pg.409]

Using that Vext(l) = Vne, separating out the Coulomb part of Vge and using the definition of Ei (eq. (6.7)), gives the adiabatic connection formula (eq. (6.32)). [Pg.410]

Theory, the energy is a unique functional of the electron density, E[p]. [Pg.409]


Although the adiabatic connection formula of Eq. (8) justifies a certain amount of Hartree-Fock mixing, there are situations in which a should vanish. In a spin-restricted description of the molecule Hj at infinite bond length (Sect. 4) the Hartree-Fock or A = 0 hole is equally distributed over both atoms, and is independent of the electron s position. But the hole for any finite A, however small, is entirely localized on the electron s atom, so no amount of Hartree-Fock mixing is acceptable in this case. [Pg.23]

The starting point for the proposed new approach is an exact formula [238], [239], based on the adiabatic connection formula and the zero-temperature fluctuation-dissipation theorem, relating the groundstate xc energy to the inter-... [Pg.159]

Substitution of these expressions into the adiabatic connection formula of Eq. (29)... [Pg.700]

The idea of mixing density functional approximations with exact (Hartree-Fock-Uke) exchange rests on theoretical considerations involving the adiabatic connection formula... [Pg.708]

The adiabatic connection formula is at the root of the ACMs. This formula is usually expressed in the form ... [Pg.57]

Several gradient corrected exchange [28-30] and correlation [31-34] functionals have been proposed. In our study we use different combinations of those of Becke [28] and Perdew and Wang [30] for the exchange and the functionals proposed by Perdew [31] and Proynov [34] for the correlation. Recently, Becke [29] has introduced the so-called hybrid functional that is based on the "adiabatic connection" formula [35], Because of its reliability, largely validated in the literature [36-38], we employ in our work also the B3LYP functional which uses the Becke gradient... [Pg.95]

The Variational Principle The Hohenberg-Kohn Theorems The Adiabatic Connection Formula Reference... [Pg.227]

The philosophy behind the hybrid functionals is simple and rooted in the adiabatic connection formula, which is a rigorous ab initio formula for the exchange-... [Pg.23]


See other pages where The Adiabatic Connection Formula is mentioned: [Pg.187]    [Pg.409]    [Pg.410]    [Pg.96]    [Pg.121]    [Pg.239]    [Pg.239]    [Pg.164]    [Pg.165]    [Pg.477]    [Pg.187]    [Pg.409]    [Pg.410]    [Pg.675]    [Pg.174]    [Pg.252]    [Pg.572]    [Pg.573]    [Pg.204]    [Pg.239]    [Pg.136]    [Pg.213]    [Pg.323]    [Pg.434]   


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Adiabatic connection formula

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