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Dirac exchange energy

The exchange part is given by the Dirac exchange-energy functional... [Pg.225]

One can improve upon the TF model by incorporating two-electron effects into P nlpl as the approximate, local Dirac exchange energy functional (cx is the Dirac exchange constant)... [Pg.47]

The Thomas-Fermi kinetic energy density Ckp(r)5/3 derives directly from the first term on the RHS of Eq. (17), the Dirac exchange energy density —cxp(r)4/3 coming from the second term. Many-body perturbation theory on this state, in which electrons are fully delocalized, yields a precise result [36,37] for the correlation energy Ec in the high-density limit as A In rs + B, where for present purposes the correlation energy is defined as the difference between the true... [Pg.207]

With a = 2/3 this is identical to the Dirac expression. The original method used a = 1, but a value of 3/4 has been shown to give better agreement for atomic and molecular systems. The name Slater is often used as a synonym for the L(S)DA exchange energy involving die electron density raised to the 4/3 power (1/3 power for the energy density). [Pg.183]

The electron-electron exchange term, Hex In equation (16) it is necessary to consider only He . As has been discussed, the energy difference between T and S states is equal to Je . With a minimal overlap integral due to a relatively large inter-radical separation. Hex can be given by the Dirac exchange operator [equation (18)],... [Pg.69]

The exchange part, ex, which represents the exchange energy of an electron in a uniform electron gas of a particular density is, apart from the pre-factor, equal to the form found by Slater in his approximation of the Hartree-Fock exchange (Section 3.3) and was originally derived by Bloch and Dirac in the late 1920 s ... [Pg.88]

Coulomb exchange effects are commonly introduced by means of the Dirac-Slater expression for the exchange energy of a electron gas ... [Pg.196]

The integral of the first term in square brackets gives the non-relativistic Dirac-Slater exchange energy, the second giving the relativistic correction ... [Pg.210]

The same investigations of the idealized uniform electron gas that identified the Dirac exchange functional, found that the correlation energy (per electron) could also be... [Pg.379]

This proposition has been tested in the exact-exchange limit of the implied linear-response theory [329], The TDFT exchange response kernel disagrees qualitatively with the corresponding expression in Dirac s TDHF theory [79,289]. This can be taken as evidence that an exact local exchange potential does not exist in the form of a Frechet derivative of the exchange energy functional in TDFT theory. [Pg.89]

The kinetic and exchange energy functionals given by Eqs. (8) and (12), respectively, contain universal terms that just depend upon the one-particle density. In the case of the former, such term is p6/3, the Thomas-Fermi term [22,23] and for the latter, the set p(ri)(4+fc 3, where the first term p4 3 (for k = 0) is the Dirac exchange expression [24]. But in addition, in Eq. (8) we observe the presence of a factor, which we call Fis([p]jr) defined as ... [Pg.53]

The explicit form for Ex[ri was originally given by Dirac [26] as an approximation to the Hartree-Fock exchange energy,... [Pg.460]


See other pages where Dirac exchange energy is mentioned: [Pg.60]    [Pg.237]    [Pg.175]    [Pg.272]    [Pg.680]    [Pg.60]    [Pg.60]    [Pg.237]    [Pg.175]    [Pg.272]    [Pg.680]    [Pg.60]    [Pg.2182]    [Pg.2183]    [Pg.502]    [Pg.183]    [Pg.88]    [Pg.49]    [Pg.60]    [Pg.257]    [Pg.347]    [Pg.218]    [Pg.338]    [Pg.378]    [Pg.403]    [Pg.36]    [Pg.71]    [Pg.84]    [Pg.73]    [Pg.102]    [Pg.104]    [Pg.142]    [Pg.5]    [Pg.99]    [Pg.99]    [Pg.104]   
See also in sourсe #XX -- [ Pg.237 ]




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